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diff --git a/.gitlab-ci.yml b/.gitlab-ci.yml
index 6c74e21..76773e9 100644
--- a/.gitlab-ci.yml
+++ b/.gitlab-ci.yml
@@ -1,86 +1,115 @@
.tags_template:
tags: &tags_def
- docker
stages:
- minimal_compile
- extended_tests
- different_compile
+ - publish
variables:
HEJ_Install_DIR: tmp_HEJ/HEJ_installed
HEJ_build_DIR: tmp_HEJ/build_HEJ
FOG_build_DIR: tmp_HEJ/build_FOG
after_script:
- date
.HEJ_compile:
tags: *tags_def
before_script:
- date
- source /cvmfs/pheno.egi.eu/HEJ/HEJ_env.sh || exit 1
- export t_HEJ_Install_DIR=${PWD}/$HEJ_Install_DIR
- export t_HEJ_build_DIR=${PWD}/$HEJ_build_DIR
- export t_HEJ_DIR=${PWD}
- mkdir -p ${t_HEJ_build_DIR}
- cd ${t_HEJ_build_DIR}
- cmake ${t_HEJ_DIR} -DCMAKE_BUILD_TYPE=DEBUG -DCMAKE_INSTALL_PREFIX=${t_HEJ_Install_DIR}
- make -j 8
Minimal_setup:
stage: minimal_compile
extends: .HEJ_compile
image: hejdock/hepenv
script:
- make test
FOG:
stage: extended_tests
extends: .HEJ_compile
image: hejdock/hepenv
script:
- date
# install HEJ
- make install
# setup env
- export LD_LIBRARY_PATH=${t_HEJ_Install_DIR}/lib:${LD_LIBRARY_PATH}
- export PATH=${t_HEJ_Install_DIR}/bin:${PATH}
- export t_FOG_build_DIR=${PWD}/$FOG_build_DIR
- export t_FOG_DIR=${t_HEJ_DIR}/FixedOrderGen
# compile
- mkdir -p ${t_FOG_build_DIR}
- cd ${t_FOG_build_DIR}
- cmake ${t_FOG_DIR} -DCMAKE_BUILD_TYPE=DEBUG
- make -j 8
- make test
rivet:
stage: different_compile
extends: .HEJ_compile
image: hejdock/rivetenv
variables:
HEJ_build_DIR: tmp_HEJ/build_HEJ_rivet
script:
- make test
- bash -c '[ -f tst.yoda ]' && echo "found rivet output"
- rivet-cmphistos tst.yoda
- bash -c '[ -f MC_XS_XS.dat ]' && echo "yoda not empty"
QCDloop:
stage: different_compile
extends: .HEJ_compile
image: hejdock/qcdloopenv
variables:
HEJ_build_DIR: tmp_HEJ/build_HEJ_qcd
script:
- make test
HepMC3:
stage: different_compile
extends: .HEJ_compile
image: hejdock/hepmc3env
variables:
HEJ_build_DIR: tmp_HEJ/build_HEJ_HepMC3
script:
- make test
+
+.Publish:
+ stage: publish
+ tags: *tags_def
+ image: hejdock/git
+ before_script:
+ - mkdir -p .ssh/ && echo "${SSH_KEY}" > .ssh/id_rsa && chmod 0600 .ssh/id_rsa
+ - rm -rf ~/.ssh/id_rsa; mkdir -p ~/.ssh/
+ - ln -s $PWD/.ssh/id_rsa ~/.ssh/id_rsa && chmod 0600 ~/.ssh/id_rsa
+ - ssh -T ${PUBLIC_GIT_PREFIX} -o "StrictHostKeyChecking no" || echo "added ssh"
+ script:
+ - git remote add public ${PUBLIC_GIT_PREFIX}${PUBLIC_GIT_POSTFIX}
+ - git checkout $CI_COMMIT_REF_NAME
+ - git branch
+ - git pull
+ - git push public
+ - git push public --tags
+ after_script:
+ - rm -f /root/.ssh/id_rsa && rm -fr .ssh
+ - git remote rm public
+
+Publish_version:
+ extends: .Publish
+ only:
+ - /^v\d+\.\d+$/
+ except:
+ - tags
+ when: on_success
diff --git a/CMakeLists.txt b/CMakeLists.txt
index 776d284..ca963fb 100644
--- a/CMakeLists.txt
+++ b/CMakeLists.txt
@@ -1,237 +1,255 @@
cmake_minimum_required(VERSION 3.1 FATAL_ERROR)
set(CMAKE_LEGACY_CYGWIN_WIN32 0)
set(CMAKE_EXPORT_COMPILE_COMMANDS ON)
-project("HEJ" VERSION 0.0.1 LANGUAGES C CXX)
+project("HEJ" VERSION 2.0.3 LANGUAGES C CXX)
+
+# Set a default build type if none was specified
+set(default_build_type "Release")
+
+if(NOT CMAKE_BUILD_TYPE AND NOT CMAKE_CONFIGURATION_TYPES)
+ message(STATUS "Setting build type to '${default_build_type}' as none was specified.")
+ set(CMAKE_BUILD_TYPE "${default_build_type}" CACHE
+ STRING "Choose the type of build." FORCE)
+ # Set the possible values of build type for cmake-gui
+ set_property(CACHE CMAKE_BUILD_TYPE PROPERTY STRINGS
+ "Debug" "Release" "MinSizeRel" "RelWithDebInfo")
+endif()
## Flags for the compiler. No warning allowed.
if (CMAKE_COMPILER_IS_GNUCC OR CMAKE_COMPILER_IS_GNUCXX)
set(CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -Wall -Wextra")
elseif (MSVC)
set(CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} /W4 /WX /EHsc")
endif()
set(CMAKE_CXX_STANDARD_REQUIRED ON)
set(CMAKE_CXX_STANDARD 14)
## Create Version
set(CMAKE_MODULE_PATH ${CMAKE_MODULE_PATH} "${CMAKE_SOURCE_DIR}/cmake/Modules/")
# Get the latest abbreviated commit hash of the working branch
execute_process(
COMMAND git rev-parse HEAD
WORKING_DIRECTORY ${CMAKE_CURRENT_SOURCE_DIR}
OUTPUT_VARIABLE PROJECT_GIT_REVISION
OUTPUT_STRIP_TRAILING_WHITESPACE
)
# Get the current working branch
execute_process(
COMMAND git rev-parse --abbrev-ref HEAD
WORKING_DIRECTORY ${CMAKE_CURRENT_SOURCE_DIR}
OUTPUT_VARIABLE PROJECT_GIT_BRANCH
OUTPUT_STRIP_TRAILING_WHITESPACE
)
## target directories for install
set(INSTALL_INCLUDE_DIR_BASE include)
set(INSTALL_INCLUDE_DIR ${INSTALL_INCLUDE_DIR_BASE}/HEJ)
set(INSTALL_BIN_DIR bin)
set(INSTALL_LIB_DIR lib)
set(INSTALL_CONFIG_DIR lib/cmake/HEJ)
## Template files
configure_file( ${CMAKE_CURRENT_SOURCE_DIR}/cmake/Templates/Version.hh.in
${PROJECT_BINARY_DIR}/include/HEJ/Version.hh @ONLY )
configure_file( ${CMAKE_CURRENT_SOURCE_DIR}/cmake/Templates/HEJ-config.cc.in
${PROJECT_BINARY_DIR}/src/bin/HEJ-config.cc @ONLY )
# Generate CMake config file
include(CMakePackageConfigHelpers)
configure_package_config_file(
cmake/Templates/hej-config.cmake.in
${CMAKE_CURRENT_BINARY_DIR}/${INSTALL_CONFIG_DIR}/hej-config.cmake
INSTALL_DESTINATION ${INSTALL_CONFIG_DIR}
PATH_VARS INSTALL_INCLUDE_DIR_BASE INSTALL_LIB_DIR
)
write_basic_package_version_file(
${CMAKE_CURRENT_BINARY_DIR}/${INSTALL_CONFIG_DIR}/hej-config-version.cmake
COMPATIBILITY SameMajorVersion
)
install(
FILES ${CMAKE_CURRENT_BINARY_DIR}/${INSTALL_CONFIG_DIR}/hej-config.cmake
${CMAKE_CURRENT_BINARY_DIR}/${INSTALL_CONFIG_DIR}/hej-config-version.cmake
DESTINATION ${INSTALL_CONFIG_DIR})
## Add directories and find dependences
include_directories(${CMAKE_CURRENT_SOURCE_DIR}/include ${PROJECT_BINARY_DIR}/include)
find_package(fastjet REQUIRED)
include_directories(${fastjet_INCLUDE_PATH})
find_package(clhep 2.3 REQUIRED)
-include_directories(${clhep_INCLUDE_PATH})
+include_directories(${CLHEP_INCLUDE_PATH})
find_package(lhapdf REQUIRED)
include_directories(${lhapdf_INCLUDE_PATH})
## Amend unintuitive behaviour of FindBoost.cmake
## Priority of BOOST_ROOT over BOOSTROOT matches FindBoost.cmake
## at least for cmake 3.12
if(DEFINED BOOST_ROOT)
message("BOOST_ROOT set - only looking for Boost in ${BOOST_ROOT}")
set(Boost_NO_BOOST_CMAKE ON)
elseif(DEFINED BOOSTROOT)
message("BOOSTROOT set - only looking for Boost in ${BOOSTROOT}")
set(Boost_NO_BOOST_CMAKE ON)
endif()
find_package(Boost REQUIRED COMPONENTS iostreams)
include_directories(${Boost_INCLUDE_DIRS})
find_package(yaml-cpp)
include_directories(${YAML_CPP_INCLUDE_DIR})
find_package(HepMC 2)
if(${HepMC_FOUND})
message (STATUS "HepMC installation found: ${HepMC_INCLUDE_DIRS}")
set(
CMAKE_CXX_FLAGS
"${CMAKE_CXX_FLAGS} -DHEJ_BUILD_WITH_HepMC_VERSION=${HepMC_VERSION_MAJOR}"
)
include_directories(${HepMC_INCLUDE_DIRS})
find_package(rivet)
if(${rivet_FOUND})
include_directories(${rivet_INCLUDE_PATH})
set(
CMAKE_CXX_FLAGS
"${CMAKE_CXX_FLAGS} -DHEJ_BUILD_WITH_RIVET"
)
endif()
endif()
find_package(QCDloop 2)
if(${QCDloop_FOUND})
set(CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -DHEJ_BUILD_WITH_QCDLOOP")
include_directories(SYSTEM ${QCDloop_INCLUDE_DIRS})
endif()
add_subdirectory(src)
## define executable
add_executable(HEJ src/bin/HEJ.cc)
## link libraries
target_link_libraries(HEJ hejlib)
add_executable(HEJ-config src/bin/HEJ-config.cc)
file(GLOB hej_headers ${CMAKE_CURRENT_SOURCE_DIR}/include/HEJ/*.hh ${PROJECT_BINARY_DIR}/include/HEJ/*.hh)
file(GLOB lhef_headers ${CMAKE_CURRENT_SOURCE_DIR}/include/LHEF/*.h)
install(FILES ${hej_headers} DESTINATION ${INSTALL_INCLUDE_DIR})
install(FILES ${lhef_headers} DESTINATION include/LHEF/)
install(TARGETS HEJ HEJ-config DESTINATION ${INSTALL_BIN_DIR})
## tests
enable_testing()
set(tst_dir "${CMAKE_CURRENT_SOURCE_DIR}/t")
add_executable(test_classify ${tst_dir}/test_classify.cc)
add_executable(test_psp ${tst_dir}/test_psp.cc)
add_executable(test_ME_generic ${tst_dir}/test_ME_generic.cc)
add_executable(check_res ${tst_dir}/check_res.cc)
add_executable(check_lhe ${tst_dir}/check_lhe.cc)
add_library(scales SHARED ${tst_dir}/scales.cc)
add_executable(test_scale_import ${tst_dir}/test_scale_import)
add_executable(test_descriptions ${tst_dir}/test_descriptions)
+add_executable(test_scale_arithmetics ${tst_dir}/test_scale_arithmetics)
target_link_libraries(test_classify hejlib)
target_link_libraries(test_psp hejlib)
target_link_libraries(test_ME_generic hejlib)
target_link_libraries(check_res hejlib)
target_link_libraries(check_lhe hejlib)
target_link_libraries(test_scale_import hejlib)
target_link_libraries(test_descriptions hejlib)
+target_link_libraries(test_scale_arithmetics hejlib)
## add tests
add_test(
NAME t_classify
COMMAND test_classify ${tst_dir}/classify.lhe.gz
)
add_test(
NAME t_psp
COMMAND test_psp ${tst_dir}/psp_gen.lhe.gz
)
set(tst_ME_data_dir "${tst_dir}/ME_data")
add_test(
NAME t_ME_j
COMMAND test_ME_generic ${tst_ME_data_dir}/config_mtinf.yml ${tst_ME_data_dir}/ME_jets.dat ${tst_ME_data_dir}/PSP_jets.lhe.gz
)
add_test(
NAME t_ME_h
COMMAND test_ME_generic ${tst_ME_data_dir}/config_mtinf.yml ${tst_ME_data_dir}/ME_h_mtinf.dat ${tst_ME_data_dir}/PSP_h.lhe.gz
)
if(${QCDloop_FOUND})
add_test(
NAME t_ME_h_mt
COMMAND test_ME_generic ${tst_ME_data_dir}/config_mt.yml ${tst_ME_data_dir}/ME_h_mt.dat ${tst_ME_data_dir}/PSP_h.lhe.gz
)
add_test(
NAME t_ME_h_mtmb
COMMAND test_ME_generic ${tst_ME_data_dir}/config_mtmb.yml ${tst_ME_data_dir}/ME_h_mtmb.dat ${tst_ME_data_dir}/PSP_h.lhe.gz
)
endif()
add_test(
NAME t_2j
COMMAND check_res ${tst_dir}/2j.lhe.gz 3.49391e+07 419684
)
add_test(
NAME t_3j
COMMAND check_res ${tst_dir}/3j.lhe.gz 2.37902e+06 25746.6
)
add_test(
NAME t_4j
COMMAND check_res ${tst_dir}/4j.lhe.gz 603713 72822.6
)
add_test(
NAME t_h_3j
COMMAND check_res ${tst_dir}/h_3j.lhe.gz 0.821622 0.0220334
)
add_test(
NAME t_h_3j_uno
COMMAND check_res ${tst_dir}/h_3j_uno.lhe.gz 0.0261968 0.000341549 uno
)
if(${HepMC_FOUND})
file(READ "${tst_dir}/jet_config.yml" config)
file(WRITE "${tst_dir}/jet_config_withHepMC.yml" "${config} - tst.hepmc")
if(${rivet_FOUND})
file(READ "${tst_dir}/jet_config_withHepMC.yml" config)
file(WRITE "${tst_dir}/jet_config_withRivet.yml" "${config}\n\nanalysis:\n rivet: MC_XS\n output: tst")
add_test(
NAME t_main
COMMAND HEJ ${tst_dir}/jet_config_withRivet.yml ${tst_dir}/2j.lhe.gz
)
else()
add_test(
NAME t_main
COMMAND HEJ ${tst_dir}/jet_config_withHepMC.yml ${tst_dir}/2j.lhe.gz
)
endif()
if(${HepMC_VERSION_MAJOR} GREATER 2)
add_executable(check_hepmc ${tst_dir}/check_hepmc.cc)
target_link_libraries(check_hepmc hejlib)
add_test(
NAME t_hepmc
COMMAND check_hepmc tst.hepmc
)
endif()
else()
add_test(
NAME t_main
COMMAND HEJ ${tst_dir}/jet_config.yml ${tst_dir}/2j.lhe.gz
)
endif()
add_test(
NAME t_lhe
COMMAND check_lhe tst.lhe
)
add_test(
NAME t_scale_import
COMMAND test_scale_import ${tst_dir}/jet_config_with_import.yml
)
add_test(
NAME t_descriptions
COMMAND test_descriptions
)
+add_test(
+ NAME t_scale_arithmetics
+ COMMAND test_scale_arithmetics ${tst_dir}/jet_config.yml ${tst_dir}/2j.lhe.gz
+ )
diff --git a/COPYING b/COPYING
new file mode 100644
index 0000000..d8cf7d4
--- /dev/null
+++ b/COPYING
@@ -0,0 +1,280 @@
+ GNU GENERAL PUBLIC LICENSE
+ Version 2, June 1991
+
+ Copyright (C) 1989, 1991 Free Software Foundation, Inc.,
+ 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA
+ Everyone is permitted to copy and distribute verbatim copies
+ of this license document, but changing it is not allowed.
+
+ Preamble
+
+ The licenses for most software are designed to take away your
+freedom to share and change it. By contrast, the GNU General Public
+License is intended to guarantee your freedom to share and change free
+software--to make sure the software is free for all its users. This
+General Public License applies to most of the Free Software
+Foundation's software and to any other program whose authors commit to
+using it. (Some other Free Software Foundation software is covered by
+the GNU Lesser General Public License instead.) You can apply it to
+your programs, too.
+
+ When we speak of free software, we are referring to freedom, not
+price. Our General Public Licenses are designed to make sure that you
+have the freedom to distribute copies of free software (and charge for
+this service if you wish), that you receive source code or can get it
+if you want it, that you can change the software or use pieces of it
+in new free programs; and that you know you can do these things.
+
+ To protect your rights, we need to make restrictions that forbid
+anyone to deny you these rights or to ask you to surrender the rights.
+These restrictions translate to certain responsibilities for you if you
+distribute copies of the software, or if you modify it.
+
+ For example, if you distribute copies of such a program, whether
+gratis or for a fee, you must give the recipients all the rights that
+you have. You must make sure that they, too, receive or can get the
+source code. And you must show them these terms so they know their
+rights.
+
+ We protect your rights with two steps: (1) copyright the software, and
+(2) offer you this license which gives you legal permission to copy,
+distribute and/or modify the software.
+
+ Also, for each author's protection and ours, we want to make certain
+that everyone understands that there is no warranty for this free
+software. If the software is modified by someone else and passed on, we
+want its recipients to know that what they have is not the original, so
+that any problems introduced by others will not reflect on the original
+authors' reputations.
+
+ Finally, any free program is threatened constantly by software
+patents. We wish to avoid the danger that redistributors of a free
+program will individually obtain patent licenses, in effect making the
+program proprietary. To prevent this, we have made it clear that any
+patent must be licensed for everyone's free use or not licensed at all.
+
+ The precise terms and conditions for copying, distribution and
+modification follow.
+
+ GNU GENERAL PUBLIC LICENSE
+ TERMS AND CONDITIONS FOR COPYING, DISTRIBUTION AND MODIFICATION
+
+ 0. This License applies to any program or other work which contains
+a notice placed by the copyright holder saying it may be distributed
+under the terms of this General Public License. The "Program", below,
+refers to any such program or work, and a "work based on the Program"
+means either the Program or any derivative work under copyright law:
+that is to say, a work containing the Program or a portion of it,
+either verbatim or with modifications and/or translated into another
+language. (Hereinafter, translation is included without limitation in
+the term "modification".) Each licensee is addressed as "you".
+
+Activities other than copying, distribution and modification are not
+covered by this License; they are outside its scope. The act of
+running the Program is not restricted, and the output from the Program
+is covered only if its contents constitute a work based on the
+Program (independent of having been made by running the Program).
+Whether that is true depends on what the Program does.
+
+ 1. You may copy and distribute verbatim copies of the Program's
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+along with the Program.
+
+You may charge a fee for the physical act of transferring a copy, and
+you may at your option offer warranty protection in exchange for a fee.
+
+ 2. You may modify your copy or copies of the Program or any portion
+of it, thus forming a work based on the Program, and copy and
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+above, provided that you also meet all of these conditions:
+
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+either of that version or of any later version published by the Free
+Software Foundation. If the Program does not specify a version number of
+this License, you may choose any version ever published by the Free Software
+Foundation.
+
+ 10. If you wish to incorporate parts of the Program into other free
+programs whose distribution conditions are different, write to the author
+to ask for permission. For software which is copyrighted by the Free
+Software Foundation, write to the Free Software Foundation; we sometimes
+make exceptions for this. Our decision will be guided by the two goals
+of preserving the free status of all derivatives of our free software and
+of promoting the sharing and reuse of software generally.
+
+ NO WARRANTY
+
+ 11. BECAUSE THE PROGRAM IS LICENSED FREE OF CHARGE, THERE IS NO WARRANTY
+FOR THE PROGRAM, TO THE EXTENT PERMITTED BY APPLICABLE LAW. EXCEPT WHEN
+OTHERWISE STATED IN WRITING THE COPYRIGHT HOLDERS AND/OR OTHER PARTIES
+PROVIDE THE PROGRAM "AS IS" WITHOUT WARRANTY OF ANY KIND, EITHER EXPRESSED
+OR IMPLIED, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF
+MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE. THE ENTIRE RISK AS
+TO THE QUALITY AND PERFORMANCE OF THE PROGRAM IS WITH YOU. SHOULD THE
+PROGRAM PROVE DEFECTIVE, YOU ASSUME THE COST OF ALL NECESSARY SERVICING,
+REPAIR OR CORRECTION.
+
+ 12. IN NO EVENT UNLESS REQUIRED BY APPLICABLE LAW OR AGREED TO IN WRITING
+WILL ANY COPYRIGHT HOLDER, OR ANY OTHER PARTY WHO MAY MODIFY AND/OR
+REDISTRIBUTE THE PROGRAM AS PERMITTED ABOVE, BE LIABLE TO YOU FOR DAMAGES,
+INCLUDING ANY GENERAL, SPECIAL, INCIDENTAL OR CONSEQUENTIAL DAMAGES ARISING
+OUT OF THE USE OR INABILITY TO USE THE PROGRAM (INCLUDING BUT NOT LIMITED
+TO LOSS OF DATA OR DATA BEING RENDERED INACCURATE OR LOSSES SUSTAINED BY
+YOU OR THIRD PARTIES OR A FAILURE OF THE PROGRAM TO OPERATE WITH ANY OTHER
+PROGRAMS), EVEN IF SUCH HOLDER OR OTHER PARTY HAS BEEN ADVISED OF THE
+POSSIBILITY OF SUCH DAMAGES.
+
+ END OF TERMS AND CONDITIONS
diff --git a/Changes.md b/Changes.md
new file mode 100644
index 0000000..ebdf244
--- /dev/null
+++ b/Changes.md
@@ -0,0 +1,20 @@
+# Version 2.0
+
+## 2.X.0
+
+* Made `MatrixElement::tree_kin` and `MatrixElement::tree_param` public
+* Allow multiplication and division of multiple scale functions e.g. `H_T/2*m_j1j2`
+
+## 2.0.3
+
+* Fixed parsing of (numerical factor) * (base scale) in configuration
+* Don't change scale names, but sanitise Rivet output file names instead
+
+## 2.0.2
+
+* Changed scale names to `"_over_"` and `"_times_"` for proper file names (was
+ `"/"` and `"*"` before)
+
+## 2.0.1
+
+* Fixed name of fixed-order generator in error message.
diff --git a/FixedOrderGen/CMakeLists.txt b/FixedOrderGen/CMakeLists.txt
index a305384..f720610 100644
--- a/FixedOrderGen/CMakeLists.txt
+++ b/FixedOrderGen/CMakeLists.txt
@@ -1,110 +1,122 @@
cmake_minimum_required(VERSION 3.1 FATAL_ERROR)
set(CMAKE_LEGACY_CYGWIN_WIN32 0)
set(CMAKE_EXPORT_COMPILE_COMMANDS ON)
-project("HEJ Fixed Order Generation" VERSION 0.0.1 LANGUAGES C CXX)
+project("HEJ Fixed Order Generation" VERSION 2.0.3 LANGUAGES C CXX)
+
+# Set a default build type if none was specified
+set(default_build_type "Release")
+
+if(NOT CMAKE_BUILD_TYPE AND NOT CMAKE_CONFIGURATION_TYPES)
+ message(STATUS "Setting build type to '${default_build_type}' as none was specified.")
+ set(CMAKE_BUILD_TYPE "${default_build_type}" CACHE
+ STRING "Choose the type of build." FORCE)
+ # Set the possible values of build type for cmake-gui
+ set_property(CACHE CMAKE_BUILD_TYPE PROPERTY STRINGS
+ "Debug" "Release" "MinSizeRel" "RelWithDebInfo")
+endif()
## Flags for the compiler. No warning allowed.
if (CMAKE_COMPILER_IS_GNUCC OR CMAKE_COMPILER_IS_GNUCXX)
set(CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -Wall -Wextra")
elseif (MSVC)
set(CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} /W4 /WX /EHsc")
endif()
set(CMAKE_CXX_STANDARD_REQUIRED ON)
set(CMAKE_CXX_STANDARD 14)
## Create Version
set(CMAKE_MODULE_PATH ${CMAKE_MODULE_PATH} "${CMAKE_SOURCE_DIR}/cmake/Modules/")
# Get the latest abbreviated commit hash of the working branch
execute_process(
COMMAND git rev-parse HEAD
WORKING_DIRECTORY ${CMAKE_CURRENT_SOURCE_DIR}
OUTPUT_VARIABLE PROJECT_GIT_REVISION
OUTPUT_STRIP_TRAILING_WHITESPACE
)
# Get the current working branch
execute_process(
COMMAND git rev-parse --abbrev-ref HEAD
WORKING_DIRECTORY ${CMAKE_CURRENT_SOURCE_DIR}
OUTPUT_VARIABLE PROJECT_GIT_BRANCH
OUTPUT_STRIP_TRAILING_WHITESPACE
)
CONFIGURE_FILE( ${CMAKE_CURRENT_SOURCE_DIR}/cmake/Templates/Version.hh.in
${PROJECT_BINARY_DIR}/include/Version.hh @ONLY )
## Add directories and find dependences
include_directories(${CMAKE_CURRENT_SOURCE_DIR}/include ${PROJECT_BINARY_DIR}/include
${CMAKE_CURRENT_SOURCE_DIR}/../include)
set(CMAKE_MODULE_PATH ${CMAKE_MODULE_PATH} "${CMAKE_SOURCE_DIR}/../cmake/Modules/")
find_package(HEJ REQUIRED)
include_directories(${HEJ_INCLUDE_PATH})
find_package(fastjet REQUIRED)
include_directories(${fastjet_INCLUDE_PATH})
find_package(clhep 2.3 REQUIRED)
-include_directories(${clhep_INCLUDE_PATH})
+include_directories(${CLHEP_INCLUDE_PATH})
find_package(lhapdf REQUIRED)
include_directories(${lhapdf_INCLUDE_PATH})
## Amend unintuitive behaviour of FindBoost.cmake
## Priority of BOOST_ROOT over BOOSTROOT matches FindBoost.cmake
## at least for cmake 3.12
if(DEFINED BOOST_ROOT)
message("BOOST_ROOT set - only looking for Boost in ${BOOST_ROOT}")
set(Boost_NO_BOOST_CMAKE ON)
elseif(DEFINED BOOSTROOT)
message("BOOSTROOT set - only looking for Boost in ${BOOSTROOT}")
set(Boost_NO_BOOST_CMAKE ON)
endif()
find_package(Boost REQUIRED COMPONENTS iostreams)
include_directories(${Boost_INCLUDE_DIRS})
find_package(yaml-cpp)
include_directories(${YAML_CPP_INCLUDE_DIR})
find_package(QCDloop 2)
if(${QCDloop_FOUND})
set(CMAKE_CXX_FLAGS "${CMAKE_CXX_FLAGS} -DHEJ_BUILD_WITH_QCDLOOP")
include_directories(SYSTEM ${QCDloop_INCLUDE_DIRS})
endif()
## define executable
file(GLOB HEJFOG_source ${CMAKE_CURRENT_SOURCE_DIR}/src/*.cc)
list(REMOVE_ITEM HEJFOG_source ${CMAKE_CURRENT_SOURCE_DIR}/src/main.cc)
add_library(hejfog STATIC ${HEJFOG_source})
add_executable(HEJFOG ${CMAKE_CURRENT_SOURCE_DIR}/src/main.cc)
## link libraries
set(libraries ${CMAKE_DL_LIBS} ${LHAPDF_LIBRARIES} ${CLHEP_LIBRARIES}
${FASTJET_LIBRARIES} ${Boost_LIBRARIES} ${YAML_CPP_LIBRARIES} ${HEJ_LIBRARIES})
if(${QCDloop_FOUND})
list(APPEND libraries ${QCDloop_LIBRARIES} quadmath)
endif()
target_link_libraries(hejfog ${libraries})
target_link_libraries(HEJFOG hejfog)
install(TARGETS HEJFOG DESTINATION bin)
## tests
enable_testing()
set(tst_dir "${CMAKE_CURRENT_SOURCE_DIR}/t")
foreach(tst h_2j h_3j h_5j h_3j_uno1 h_3j_uno2 h_2j_decay 2j 4j W_2j_classify W_nj_classify)
add_executable(test_${tst} ${tst_dir}/${tst}.cc)
target_link_libraries(test_${tst} hejfog)
add_test(NAME t_${tst} COMMAND test_${tst} WORKING_DIRECTORY ${tst_dir})
endforeach()
add_test(
NAME t_main_2j
COMMAND HEJFOG ${tst_dir}/config_2j.yml
)
add_test(
NAME t_main_h2j
COMMAND HEJFOG ${tst_dir}/config_h_2j.yml
)
add_test(
NAME t_main_h2j_decay
COMMAND HEJFOG ${tst_dir}/config_h_2j_decay.yml
)
diff --git a/FixedOrderGen/include/ParticleProperties.hh b/FixedOrderGen/include/ParticleProperties.hh
index 5e72895..08a296d 100644
--- a/FixedOrderGen/include/ParticleProperties.hh
+++ b/FixedOrderGen/include/ParticleProperties.hh
@@ -1,16 +1,23 @@
#pragma once
#include <vector>
#include <unordered_map>
#include "Decay.hh"
namespace HEJFOG{
struct ParticleProperties{
double mass;
double width;
std::vector<Decay> decays;
};
+ #if !defined(__clang__) && defined(__GNUC__) && (__GNUC__ < 6)
+ // gcc version < 6 explicitly needs hash function for enum
+ // see https://gcc.gnu.org/bugzilla/show_bug.cgi?id=60970
+ using ParticlesPropMap
+ = std::unordered_map<HEJ::ParticleID, ParticleProperties, std::hash<int>>;
+ #else
using ParticlesPropMap
= std::unordered_map<HEJ::ParticleID, ParticleProperties>;
+ #endif
}
diff --git a/FixedOrderGen/include/PhaseSpacePoint.hh b/FixedOrderGen/include/PhaseSpacePoint.hh
index cba056e..164c7ae 100644
--- a/FixedOrderGen/include/PhaseSpacePoint.hh
+++ b/FixedOrderGen/include/PhaseSpacePoint.hh
@@ -1,216 +1,216 @@
/** \file PhaseSpacePoint.hh
* \brief Contains the PhaseSpacePoint Class
*/
#pragma once
#include <bitset>
#include <vector>
-#include "HEJ/utility.hh"
#include "HEJ/Event.hh"
-#include "HEJ/PDG_codes.hh"
+#include "HEJ/Particle.hh"
#include "HEJ/PDF.hh"
+#include "HEJ/PDG_codes.hh"
#include "HEJ/RNG.hh"
-#include "Status.hh"
#include "JetParameters.hh"
#include "ParticleProperties.hh"
+#include "Status.hh"
namespace HEJFOG{
class Process;
using HEJ::Particle;
//! A point in resummation phase space
class PhaseSpacePoint{
public:
//! Default PhaseSpacePoint Constructor
PhaseSpacePoint() = default;
//! PhaseSpacePoint Constructor
/**
* @param proc The process to generate
* @param jet_properties Jet defintion & cuts
* @param pdf The pdf set (used for sampling)
* @param E_beam Energie of the beam
* @param subl_chance Chance to turn a potentially unordered
* emission into an actual one
* @param subl_channels Possible subleading channels.
* see HEJFOG::Subleading
* @param particle_properties Properties of producted boson
*
* Initially, only FKL phase space points are generated. subl_chance gives
* the change of turning one emissions into a subleading configuration,
* i.e. either unordered or central quark/anti-quark pair. Unordered
* emissions require that the most extremal emission in any direction is
* a quark or anti-quark and the next emission is a gluon. Quark/anti-quark
* pairs are only generated for W processes. At most one subleading
* emission will be generated in this way.
*/
PhaseSpacePoint(
Process const & proc,
JetParameters const & jet_properties,
HEJ::PDF & pdf, double E_beam,
double subl_chance,
unsigned int subl_channels,
ParticlesPropMap const & particles_properties,
HEJ::RNG & ran
);
//! Get Weight Function
/**
* @returns Weight of Event
*/
double weight() const{
return weight_;
}
Status status() const{
return status_;
}
//! Get Incoming Function
/**
* @returns Incoming Particles
*/
std::array<Particle, 2> const & incoming() const{
return incoming_;
}
//! Get Outgoing Function
/**
* @returns Outgoing Particles
*/
std::vector<Particle> const & outgoing() const{
return outgoing_;
}
std::unordered_map<size_t, std::vector<Particle>> const & decays() const{
return decays_;
}
private:
/**
* @internal
* @brief Generate LO parton momentum
*
* @param count Number of partons to generate
* @param is_pure_jets If true ensures momentum conservation in x and y
* @param jet_param Jet properties to fulfil
* @param max_pt max allowed pt for a parton (typically E_CMS)
* @param ran Random Number Generator
*
* @returns Momentum of partons
*
* Ensures that each parton is in its own jet.
* Generation is independent of parton flavour. Output is sorted in rapidity.
*/
std::vector<fastjet::PseudoJet> gen_LO_partons(
int count, bool is_pure_jets,
JetParameters const & jet_param,
double max_pt,
HEJ::RNG & ran
);
Particle gen_boson(
HEJ::ParticleID bosonid, double mass, double width,
HEJ::RNG & ran
);
template<class ParticleMomenta>
fastjet::PseudoJet gen_last_momentum(
ParticleMomenta const & other_momenta,
double mass_square, double y
) const;
bool jets_ok(
std::vector<fastjet::PseudoJet> const & Born_jets,
std::vector<fastjet::PseudoJet> const & partons
) const;
/**
* @internal
* @brief Generate incoming partons according to the PDF
*
* @param uf Scale used in the PDF
*/
void reconstruct_incoming(
Process const & proc, unsigned int subl_channels,
HEJ::PDF & pdf, double E_beam,
double uf,
HEJ::RNG & ran
);
/**
* @internal
* @brief Returns list of all allowed initial states partons
*/
std::array<std::bitset<11>,2> filter_partons(
Process const & proc, unsigned int const subl_channels,
HEJ::RNG & ran
);
HEJ::ParticleID generate_incoming_id(
size_t beam_idx, double x, double uf, HEJ::PDF & pdf,
std::bitset<11> allowed_partons, HEJ::RNG & ran
);
bool momentum_conserved(double ep) const;
HEJ::Particle const & most_backward_FKL(
std::vector<HEJ::Particle> const & partons
) const;
HEJ::Particle const & most_forward_FKL(
std::vector<HEJ::Particle> const & partons
) const;
HEJ::Particle & most_backward_FKL(std::vector<HEJ::Particle> & partons) const;
HEJ::Particle & most_forward_FKL(std::vector<HEJ::Particle> & partons) const;
bool extremal_FKL_ok(
std::vector<fastjet::PseudoJet> const & partons
) const;
double random_normal(double stddev, HEJ::RNG & ran);
/**
* @internal
* @brief Turns a FKL configuration into a subleading one
*
* @param chance Change to switch to subleading configuration
* @param channels Allowed channels for subleading process
* @param proc Process to decide which subleading
* configurations are allowed
*
* With a chance of "chance" the FKL configuration is either turned into
* a unordered configuration or, for A/W/Z bosons, a configuration with
* a central quark/anti-quark pair.
*/
void maybe_turn_to_subl(double chance, unsigned int channels,
Process const & proc, HEJ::RNG & ran);
void turn_to_uno(bool can_be_uno_backward, bool can_be_uno_forward, HEJ::RNG & ran);
void turn_to_qqx(bool allow_strange, HEJ::RNG & ran);
std::vector<Particle> decay_boson(
HEJ::Particle const & parent,
std::vector<Decay> const & decays,
HEJ::RNG & ran
);
/// @brief setup outgoing partons to ensure correct coupling to boson
void couple_boson(HEJ::ParticleID boson, HEJ::RNG & ran);
Decay select_decay_channel(
std::vector<Decay> const & decays,
HEJ::RNG & ran
);
double gen_hard_pt(
int np, double ptmin, double ptmax, double y,
HEJ::RNG & ran
);
double gen_soft_pt(int np, double ptmax, HEJ::RNG & ran);
double gen_parton_pt(
int count, JetParameters const & jet_param, double ptmax, double y,
HEJ::RNG & ran
);
double weight_;
Status status_;
std::array<Particle, 2> incoming_;
std::vector<Particle> outgoing_;
//! Particle decays in the format {outgoing index, decay products}
std::unordered_map<size_t, std::vector<Particle>> decays_;
};
HEJ::UnclusteredEvent to_UnclusteredEvent(PhaseSpacePoint const & psp);
}
diff --git a/FixedOrderGen/src/EventGenerator.cc b/FixedOrderGen/src/EventGenerator.cc
index 8cfa609..eb99958 100644
--- a/FixedOrderGen/src/EventGenerator.cc
+++ b/FixedOrderGen/src/EventGenerator.cc
@@ -1,80 +1,80 @@
#include "EventGenerator.hh"
#include "Process.hh"
#include "Beam.hh"
#include "JetParameters.hh"
#include "PhaseSpacePoint.hh"
#include "HEJ/Event.hh"
#include "HEJ/config.hh"
namespace HEJFOG{
EventGenerator::EventGenerator(
Process process,
Beam beam,
HEJ::ScaleGenerator scale_gen,
JetParameters jets,
int pdf_id,
double subl_change,
unsigned int subl_channels,
ParticlesPropMap particles_properties,
HEJ::HiggsCouplingSettings Higgs_coupling,
HEJ::RNG & ran
):
pdf_{pdf_id, beam.particles[0], beam.particles[1]},
ME_{
[this](double mu){ return pdf_.Halphas(mu); },
HEJ::MatrixElementConfig{
false,
std::move(Higgs_coupling)
}
},
scale_gen_{std::move(scale_gen)},
process_{std::move(process)},
jets_{std::move(jets)},
beam_{std::move(beam)},
subl_change_{subl_change},
subl_channels_{subl_channels},
particles_properties_{std::move(particles_properties)},
ran_{ran}
{
}
HEJ::Event EventGenerator::gen_event(){
HEJFOG::PhaseSpacePoint psp{
process_,
jets_,
pdf_, beam_.energy,
subl_change_, subl_channels_,
particles_properties_,
ran_
};
status_ = psp.status();
if(status_ != good) return {};
HEJ::Event ev = scale_gen_(
HEJ::Event{
to_UnclusteredEvent(std::move(psp)),
jets_.def, jets_.min_pt
}
);
const double shat = HEJ::shat(ev);
const double xa = (ev.incoming()[0].E()-ev.incoming()[0].pz())/(2.*beam_.energy);
const double xb = (ev.incoming()[1].E()+ev.incoming()[1].pz())/(2.*beam_.energy);
// evaluate matrix element on this point
- const auto ME_weights = ME_.tree(ev, false);
+ const auto ME_weights = ME_.tree(ev);
ev.central().weight *= ME_weights.central/(shat*shat);
ev.central().weight *= pdf_.pdfpt(0,xa,ev.central().muf, ev.incoming()[0].type);
ev.central().weight *= pdf_.pdfpt(0,xb,ev.central().muf, ev.incoming()[1].type);
for(size_t i = 0; i < ev.variations().size(); ++i){
auto & var = ev.variations(i);
var.weight *= ME_weights.variations[i]/(shat*shat);
var.weight *= pdf_.pdfpt(0,xa,var.muf, ev.incoming()[0].type);
var.weight *= pdf_.pdfpt(0,xb,var.muf, ev.incoming()[1].type);
}
return ev;
}
}
diff --git a/FixedOrderGen/src/PhaseSpacePoint.cc b/FixedOrderGen/src/PhaseSpacePoint.cc
index 93ac98c..8969c40 100644
--- a/FixedOrderGen/src/PhaseSpacePoint.cc
+++ b/FixedOrderGen/src/PhaseSpacePoint.cc
@@ -1,663 +1,665 @@
#include "PhaseSpacePoint.hh"
#include <random>
#include <algorithm>
#include "HEJ/Constants.hh"
+#include <CLHEP/Random/Randomize.h>
+#include <CLHEP/Random/RanluxEngine.h>
+
+#include "HEJ/exceptions.hh"
#include "HEJ/kinematics.hh"
+#include "HEJ/Particle.hh"
#include "HEJ/utility.hh"
-#include "HEJ/exceptions.hh"
#include "Process.hh"
#include "Subleading.hh"
-#include <CLHEP/Random/Randomize.h>
-#include <CLHEP/Random/RanluxEngine.h>
using namespace HEJ;
namespace HEJFOG{
static_assert(
std::numeric_limits<double>::has_quiet_NaN,
"no quiet NaN for double"
);
constexpr double NaN = std::numeric_limits<double>::quiet_NaN();
HEJ::UnclusteredEvent to_UnclusteredEvent(PhaseSpacePoint const & psp){
HEJ::UnclusteredEvent result;
result.incoming = psp.incoming();
std::sort(
begin(result.incoming), end(result.incoming),
[](Particle o1, Particle o2){return o1.p.pz()<o2.p.pz();}
);
assert(result.incoming.size() == 2);
result.outgoing = psp.outgoing();
assert(
std::is_sorted(
begin(result.outgoing), end(result.outgoing),
HEJ::rapidity_less{}
)
);
assert(result.outgoing.size() >= 2);
result.decays = psp.decays();
result.central.mur = NaN;
result.central.muf = NaN;
result.central.weight = psp.weight();
return result;
}
namespace{
bool can_swap_to_uno(
HEJ::Particle const & p1, HEJ::Particle const & p2
){
return is_parton(p1)
&& p1.type != pid::gluon
&& p2.type == pid::gluon;
}
size_t count_gluons(std::vector<Particle>::const_iterator first,
std::vector<Particle>::const_iterator last){
return std::count_if(first, last, [](Particle const & p)
{return p.type == pid::gluon;});
}
/** assumes FKL configurations between first and last,
* else there can be a quark in a non-extreme position
* e.g. uno configuration gqg would pass
*/
bool can_change_to_qqx(
std::vector<Particle>::const_iterator first,
std::vector<Particle>::const_iterator last){
return 1 < count_gluons(first,last);
}
bool is_AWZ_proccess(Process const & proc){
return proc.boson && is_AWZ_boson(*proc.boson);
}
bool is_up_type(Particle const & part){
return HEJ::is_anyquark(part) && !(abs(part.type)%2);
}
bool is_down_type(Particle const & part){
return HEJ::is_anyquark(part) && abs(part.type)%2;
}
/// true iff parton can couple to a W
bool can_couple_to_W(Particle const & part, int const sign_W){
return abs(part.type)<5
&& ( (sign_W*part.type > 0 && is_up_type(part))
|| (sign_W*part.type < 0 && is_down_type(part)) );
}
}
void PhaseSpacePoint::maybe_turn_to_subl(
double chance,
unsigned int const channels,
Process const & proc,
HEJ::RNG & ran
){
if(proc.njets <= 2) return;
assert(outgoing_.size() >= 2);
// decide what kind of subleading process is allowed
bool allow_uno = false;
bool allow_strange = true;
const size_t nout = outgoing_.size();
const bool can_be_uno_backward = (channels&Subleading::uno)
&& can_swap_to_uno(outgoing_[0], outgoing_[1]);
const bool can_be_uno_forward = (channels&Subleading::uno)
&& can_swap_to_uno(outgoing_[nout-1], outgoing_[nout-2]);
allow_uno = can_be_uno_backward || can_be_uno_forward;
bool allow_qqx = false;
if(is_AWZ_proccess(proc)) {
allow_qqx = (channels&Subleading::qqx)
&& can_change_to_qqx(outgoing_.cbegin(), outgoing_.cend());
const int sign_W = *proc.boson>0?1:-1;
if(std::none_of(outgoing_.cbegin(), outgoing_.cend(),
[sign_W](Particle const & p){ return can_couple_to_W(p, sign_W);})) {
// enforce qqx if A/W/Z can't couple somewhere else
assert(allow_qqx);
allow_uno = false;
chance = 1.;
// strange not allowed for W
if(abs(*proc.boson)== pid::Wp) allow_strange = false;
}
}
if(!allow_uno && !allow_qqx) return;
if(ran.flat() < chance){
weight_ /= chance;
if(allow_uno && !allow_qqx){
turn_to_uno(can_be_uno_backward, can_be_uno_forward, ran);
} else if (!allow_uno && allow_qqx) {
turn_to_qqx(allow_strange, ran);
} else {
assert( allow_uno && allow_qqx);
if(ran.flat() < 0.5) turn_to_uno(can_be_uno_backward, can_be_uno_forward, ran);
else turn_to_qqx(allow_strange, ran);
weight_ *= 2.;
}
} else weight_ /= 1 - chance;
}
void PhaseSpacePoint::turn_to_uno(
const bool can_be_uno_backward, const bool can_be_uno_forward,
HEJ::RNG & ran
){
if(!can_be_uno_backward && !can_be_uno_forward) return;
const size_t nout = outgoing_.size();
if(can_be_uno_backward && can_be_uno_forward){
if(ran.flat() < 0.5){
std::swap(outgoing_[0].type, outgoing_[1].type);
} else {
std::swap(outgoing_[nout-1].type, outgoing_[nout-2].type);
}
weight_ *= 2.;
} else if(can_be_uno_backward){
std::swap(outgoing_[0].type, outgoing_[1].type);
} else {
assert(can_be_uno_forward);
std::swap(outgoing_[nout-1].type, outgoing_[nout-2].type);
}
}
void PhaseSpacePoint::turn_to_qqx(const bool allow_stange, HEJ::RNG & ran){
/// find first and last gluon in FKL chain
auto first = std::find_if(outgoing_.begin(), outgoing_.end(),
[](Particle const & p){return p.type == pid::gluon;});
std::vector<Particle*> FKL_gluons;
for(auto p = first; p<outgoing_.end(); ++p){
if((*p).type == pid::gluon) FKL_gluons.push_back(&*p);
else if(is_quark(*p) || is_antiquark(*p)) break;
}
const size_t ng = FKL_gluons.size();
if(ng < 2)
throw std::logic_error("not enough gluons to create qqx");
// select flavour of quark
const double r1 = 2.*ran.flat()-1.;
const double max_flavour = allow_stange?n_f:n_f-1;
weight_ *= max_flavour*2;
int flavour = pid::down;
for (double sum = 1./max_flavour; sum < std::abs(r1); sum += 1./max_flavour)
++flavour;
flavour*=r1<0.?-1:1;
// select gluon for switch
const size_t idx = floor((ng-1) * ran.flat());
weight_ *= (ng-1);
FKL_gluons[idx]->type = ParticleID(flavour);
FKL_gluons[idx+1]->type = ParticleID(-flavour);
}
template<class ParticleMomenta>
fastjet::PseudoJet PhaseSpacePoint::gen_last_momentum(
ParticleMomenta const & other_momenta,
const double mass_square, const double y
) const {
std::array<double,2> pt{0.,0.};
for (auto const & p: other_momenta) {
pt[0]-= p.px();
pt[1]-= p.py();
}
const double mperp = sqrt(pt[0]*pt[0]+pt[1]*pt[1]+mass_square);
const double pz=mperp*sinh(y);
const double E=mperp*cosh(y);
return {pt[0], pt[1], pz, E};
}
PhaseSpacePoint::PhaseSpacePoint(
Process const & proc,
JetParameters const & jet_param,
HEJ::PDF & pdf, double E_beam,
double const subl_chance,
unsigned int const subl_channels,
ParticlesPropMap const & particles_properties,
HEJ::RNG & ran
)
{
assert(proc.njets >= 2);
if(proc.boson
&& particles_properties.find(*(proc.boson))
== particles_properties.end())
throw HEJ::missing_option("Boson "
+std::to_string(*(proc.boson))+" can't be generated: missing properties");
status_ = good;
weight_ = 1;
const int nout = proc.njets + (proc.boson?1:0);
outgoing_.reserve(nout);
// generate parton momenta
const bool is_pure_jets = !proc.boson;
auto partons = gen_LO_partons(
proc.njets, is_pure_jets, jet_param, E_beam, ran
);
// pre fill flavour with gluons
for(auto&& p_out: partons) {
outgoing_.emplace_back(Particle{pid::gluon, std::move(p_out)});
}
if(status_ != good) return;
// create boson
if(proc.boson){
const auto & boson_prop = particles_properties.at(*proc.boson);
auto boson(gen_boson(*proc.boson, boson_prop.mass, boson_prop.width, ran));
const auto pos = std::upper_bound(
begin(outgoing_),end(outgoing_),boson,rapidity_less{}
);
outgoing_.insert(pos, std::move(boson));
if(! boson_prop.decays.empty()){
const size_t boson_idx = std::distance(begin(outgoing_), pos);
decays_.emplace(
boson_idx,
decay_boson(outgoing_[boson_idx], boson_prop.decays, ran)
);
}
}
// normalisation of momentum-conserving delta function
weight_ *= pow(2*M_PI, 4);
reconstruct_incoming(proc, subl_channels, pdf,E_beam,jet_param.min_pt, ran);
if(status_ != good) return;
// set outgoing states
most_backward_FKL(outgoing_).type = incoming_[0].type;
most_forward_FKL(outgoing_).type = incoming_[1].type;
maybe_turn_to_subl(subl_chance, subl_channels, proc, ran);
if(proc.boson) couple_boson(*proc.boson, ran);
}
double PhaseSpacePoint::gen_hard_pt(
int np , double ptmin, double ptmax, double y,
HEJ::RNG & ran
) {
// heuristic parameters for pt sampling
const double ptpar = ptmin + np/5.;
const double arg_small_y = atan((ptmax - ptmin)/ptpar);
const double y_cut = 3.;
const double r1 = ran.flat();
if(y < y_cut){
const double pt = ptmin + ptpar*tan(r1*arg_small_y);
const double temp = cos(r1*arg_small_y);
weight_ *= pt*ptpar*arg_small_y/(temp*temp);
return pt;
}
const double ptpar2 = ptpar/(1 + 5*(y-y_cut));
const double temp = 1. - std::exp((ptmin-ptmax)/ptpar2);
const double pt = ptmin - ptpar2*std::log(1-r1*temp);
weight_ *= pt*ptpar2*temp/(1-r1*temp);
return pt;
}
double PhaseSpacePoint::gen_soft_pt(int np, double max_pt, HEJ::RNG & ran) {
constexpr double ptpar = 4.;
const double r = ran.flat();
const double pt = max_pt + ptpar/np*std::log(r);
weight_ *= pt*ptpar/(np*r);
return pt;
}
double PhaseSpacePoint::gen_parton_pt(
int count, JetParameters const & jet_param, double max_pt, double y,
HEJ::RNG & ran
) {
constexpr double p_small_pt = 0.02;
if(! jet_param.peak_pt) {
return gen_hard_pt(count, jet_param.min_pt, max_pt, y, ran);
}
const double r = ran.flat();
if(r > p_small_pt) {
weight_ /= 1. - p_small_pt;
return gen_hard_pt(count, *jet_param.peak_pt, max_pt, y, ran);
}
weight_ /= p_small_pt;
const double pt = gen_soft_pt(count, *jet_param.peak_pt, ran);
if(pt < jet_param.min_pt) {
weight_=0.0;
status_ = not_enough_jets;
return jet_param.min_pt;
}
return pt;
}
std::vector<fastjet::PseudoJet> PhaseSpacePoint::gen_LO_partons(
int np, bool is_pure_jets,
JetParameters const & jet_param,
double max_pt,
HEJ::RNG & ran
){
if (np<2) throw std::invalid_argument{"Not enough partons in gen_LO_partons"};
weight_ /= pow(16.*pow(M_PI,3),np);
weight_ /= std::tgamma(np+1); //remove rapidity ordering
std::vector<fastjet::PseudoJet> partons;
partons.reserve(np);
for(int i = 0; i < np; ++i){
const double y = -jet_param.max_y + 2*jet_param.max_y*ran.flat();
weight_ *= 2*jet_param.max_y;
const bool is_last_parton = i+1 == np;
if(is_pure_jets && is_last_parton) {
constexpr double parton_mass_sq = 0.;
partons.emplace_back(gen_last_momentum(partons, parton_mass_sq, y));
break;
}
const double phi = 2*M_PI*ran.flat();
weight_ *= 2.0*M_PI;
const double pt = gen_parton_pt(np, jet_param, max_pt, y, ran);
if(weight_ == 0.0) return {};
partons.emplace_back(fastjet::PtYPhiM(pt, y, phi));
assert(jet_param.min_pt <= partons[i].pt());
assert(partons[i].pt() <= max_pt+1e-5);
}
// Need to check that at LO, the number of jets = number of partons;
fastjet::ClusterSequence cs(partons, jet_param.def);
auto cluster_jets=cs.inclusive_jets(jet_param.min_pt);
if (cluster_jets.size()!=unsigned(np)){
weight_=0.0;
status_ = not_enough_jets;
return {};
}
std::sort(begin(partons), end(partons), rapidity_less{});
return partons;
}
Particle PhaseSpacePoint::gen_boson(
HEJ::ParticleID bosonid, double mass, double width,
HEJ::RNG & ran
){
// Usual phase space measure
weight_ /= 16.*pow(M_PI, 3);
// Generate a y Gaussian distributed around 0
/// @TODO: magic number only for Higgs
/// @TODO better sampling for W
const double y = random_normal(1.6, ran);
const double r1 = ran.flat();
const double sH = mass*(
mass + width*tan(M_PI/2.*r1 + (r1-1.)*atan(mass/width))
);
auto p = gen_last_momentum(outgoing_, sH, y);
return Particle{bosonid, std::move(p)};
}
Particle const & PhaseSpacePoint::most_backward_FKL(
std::vector<Particle> const & partons
) const{
if(!HEJ::is_parton(partons[0])) return partons[1];
return partons[0];
}
Particle const & PhaseSpacePoint::most_forward_FKL(
std::vector<Particle> const & partons
) const{
const size_t last_idx = partons.size() - 1;
if(!HEJ::is_parton(partons[last_idx])) return partons[last_idx-1];
return partons[last_idx];
}
Particle & PhaseSpacePoint::most_backward_FKL(
std::vector<Particle> & partons
) const{
if(!HEJ::is_parton(partons[0])) return partons[1];
return partons[0];
}
Particle & PhaseSpacePoint::most_forward_FKL(
std::vector<Particle> & partons
) const{
const size_t last_idx = partons.size() - 1;
if(!HEJ::is_parton(partons[last_idx])) return partons[last_idx-1];
return partons[last_idx];
}
namespace {
/// partons are ordered: even = anti, 0 = gluon
ParticleID index_to_pid(size_t i){
if(!i) return pid::gluon;
return static_cast<ParticleID>(i%2?(i+1)/2:-i/2);
}
/// partons are ordered: even = anti, 0 = gluon
size_t pid_to_index(ParticleID id){
if(id==pid::gluon) return 0;
return id>0?id*2-1:abs(id)*2;
}
std::bitset<11> init_allowed(ParticleID const id){
if(abs(id) == pid::proton)
return ~0;
std::bitset<11> out = 0;
if(is_parton(id))
out[pid_to_index(id)] = 1;
return out;
}
/// decides which "index" (see index_to_pid) are allowed for process
std::bitset<11> allowed_quarks(ParticleID const boson){
std::bitset<11> allowed = ~0;
if(abs(boson) == pid::Wp){
// special case W:
// Wp: anti-down or up-type quark, no b/t -> 0001100110(1) = 205
// Wm: down or anti-up-type quark, no b/t -> 0010011001(1) = 307
allowed = boson>0?205:307;
}
return allowed;
}
}
/**
* checks which partons are allowed as initial state:
* 1. only allow what is given in the Runcard (p -> all)
* 2. A/W/Z require something to couple to
* a) no qqx => no incoming gluon
* b) 2j => no incoming gluon
* c) 3j => can couple OR is gluon => 2 gluons become qqx later
*/
std::array<std::bitset<11>,2> PhaseSpacePoint::filter_partons(
Process const & proc, unsigned int const subl_channels, HEJ::RNG & ran
){
std::array<std::bitset<11>,2> allowed_partons{
init_allowed(proc.incoming[0]),
init_allowed(proc.incoming[1])
};
bool const allow_qqx = subl_channels&Subleading::qqx;
// special case A/W/Z
if(is_AWZ_proccess(proc) && ((proc.njets < 4) || !allow_qqx)){
// all possible incoming states
auto allowed(allowed_quarks(*proc.boson));
if(proc.njets == 2 || !allow_qqx) allowed[0]=0;
// possible states per leg
std::array<std::bitset<11>,2> const maybe_partons{
allowed_partons[0]&allowed, allowed_partons[1]&allowed};
if(maybe_partons[0].any() && maybe_partons[1].any()){
// two options to get allowed initial state => choose one at random
const size_t idx = ran.flat() < 0.5;
allowed_partons[idx] = maybe_partons[idx];
// else choose the possible
} else if(maybe_partons[0].any()) {
allowed_partons[0] = maybe_partons[0];
} else if(maybe_partons[1].any()) {
allowed_partons[1] = maybe_partons[1];
} else{
throw std::invalid_argument{"Incoming state not allowed."};
}
}
return allowed_partons;
}
void PhaseSpacePoint::reconstruct_incoming(
Process const & proc, unsigned int const subl_channels,
HEJ::PDF & pdf, double E_beam,
double uf,
HEJ::RNG & ran
){
std::tie(incoming_[0].p, incoming_[1].p) = incoming_momenta(outgoing_);
// calculate xa, xb
const double sqrts=2*E_beam;
const double xa=(incoming_[0].p.e()-incoming_[0].p.pz())/sqrts;
const double xb=(incoming_[1].p.e()+incoming_[1].p.pz())/sqrts;
// abort if phase space point is outside of collider energy reach
if (xa>1. || xb>1.){
weight_=0;
status_ = too_much_energy;
return;
}
// pick pdfs
/** @TODO
* ufa, ufb don't correspond to our final scale choice.
* The HEJ scale generators currently expect a full event as input,
* so fixing this is not completely trivial
*/
auto const & ids = proc.incoming;
std::array<std::bitset<11>,2> allowed_partons(
filter_partons(proc, subl_channels, ran));
for(size_t i = 0; i < 2; ++i){
if(ids[i] == pid::proton || ids[i] == pid::p_bar){
incoming_[i].type =
generate_incoming_id(i, i?xb:xa, uf, pdf, allowed_partons[i], ran);
} else {
assert(allowed_partons[i][pid_to_index(ids[i])]);
incoming_[i].type = ids[i];
}
}
assert(momentum_conserved(1e-7));
}
HEJ::ParticleID PhaseSpacePoint::generate_incoming_id(
size_t const beam_idx, double const x, double const uf,
HEJ::PDF & pdf, std::bitset<11> allowed_partons, HEJ::RNG & ran
){
std::array<double,11> pdf_wt;
pdf_wt[0] = allowed_partons[0]?fabs(pdf.pdfpt(beam_idx,x,uf,pid::gluon)):0.;
double pdftot = pdf_wt[0];
for(size_t i = 1; i < pdf_wt.size(); ++i){
pdf_wt[i] = allowed_partons[i]?4./9.*fabs(pdf.pdfpt(beam_idx,x,uf,index_to_pid(i))):0;
pdftot += pdf_wt[i];
}
const double r1 = pdftot * ran.flat();
double sum = 0;
for(size_t i=0; i < pdf_wt.size(); ++i){
if (r1 < (sum+=pdf_wt[i])){
weight_*= pdftot/pdf_wt[i];
return index_to_pid(i);
}
}
std::cerr << "Error in choosing incoming parton: "<<x<<" "<<uf<<" "
<<sum<<" "<<pdftot<<" "<<r1<<std::endl;
throw std::logic_error{"Failed to choose parton flavour"};
}
void PhaseSpacePoint::couple_boson(
HEJ::ParticleID const boson, HEJ::RNG & ran
){
if(abs(boson) != pid::Wp) return; // only matters for W
/// @TODO this could be use to sanity check gamma and Z
// find all possible quarks
const int sign_W = boson>0?1:-1;
std::vector<Particle*> allowed_parts;
for(auto & part: outgoing_){
// Wp -> up OR anti-down, Wm -> anti-up OR down, no bottom
if ( can_couple_to_W(part, sign_W) )
allowed_parts.push_back(&part);
}
if(allowed_parts.size() == 0){
throw std::logic_error{"Found no parton for coupling with boson"};
}
// select one and flip it
size_t idx = 0;
if(allowed_parts.size() > 1){
/// @TODO more efficient sampling
/// old code: probability[i] = exp(parton[i].y - W.y)
idx = floor(ran.flat()*allowed_parts.size());
weight_ *= allowed_parts.size();
}
allowed_parts[idx]->type =
static_cast<ParticleID>( allowed_parts[idx]->type - sign_W );
}
double PhaseSpacePoint::random_normal(
double stddev,
HEJ::RNG & ran
){
const double r1 = ran.flat();
const double r2 = ran.flat();
const double lninvr1 = -log(r1);
const double result = stddev*sqrt(2.*lninvr1)*cos(2.*M_PI*r2);
weight_ *= exp(result*result/(2*stddev*stddev))*sqrt(2.*M_PI)*stddev;
return result;
}
bool PhaseSpacePoint::momentum_conserved(double ep) const{
fastjet::PseudoJet diff;
for(auto const & in: incoming()) diff += in.p;
for(auto const & out: outgoing()) diff -= out.p;
return nearby_ep(diff, fastjet::PseudoJet{}, ep);
}
Decay PhaseSpacePoint::select_decay_channel(
std::vector<Decay> const & decays,
HEJ::RNG & ran
){
double br_total = 0.;
for(auto const & decay: decays) br_total += decay.branching_ratio;
// adjust weight
// this is given by (channel branching ratio)/(chance to pick channel)
// where (chance to pick channel) =
// (channel branching ratio)/(total branching ratio)
weight_ *= br_total;
const double r1 = br_total*ran.flat();
double br_sum = 0.;
for(auto const & decay: decays){
br_sum += decay.branching_ratio;
if(r1 < br_sum) return decay;
}
throw std::logic_error{"unreachable"};
}
std::vector<Particle> PhaseSpacePoint::decay_boson(
HEJ::Particle const & parent,
std::vector<Decay> const & decays,
HEJ::RNG & ran
){
const auto channel = select_decay_channel(decays, ran);
if(channel.products.size() != 2){
throw HEJ::not_implemented{
"only decays into two particles are implemented"
};
}
std::vector<Particle> decay_products(channel.products.size());
for(size_t i = 0; i < channel.products.size(); ++i){
decay_products[i].type = channel.products[i];
}
// choose polar and azimuth angle in parent rest frame
const double E = parent.m()/2;
const double theta = 2.*M_PI*ran.flat();
const double cos_phi = 2.*ran.flat()-1.;
const double sin_phi = sqrt(1. - cos_phi*cos_phi); // Know 0 < phi < pi
const double px = E*cos(theta)*sin_phi;
const double py = E*sin(theta)*sin_phi;
const double pz = E*cos_phi;
decay_products[0].p.reset(px, py, pz, E);
decay_products[1].p.reset(-px, -py, -pz, E);
for(auto & particle: decay_products) particle.p.boost(parent.p);
return decay_products;
}
}
diff --git a/FixedOrderGen/src/config.cc b/FixedOrderGen/src/config.cc
index 42db1eb..2c53a52 100644
--- a/FixedOrderGen/src/config.cc
+++ b/FixedOrderGen/src/config.cc
@@ -1,360 +1,355 @@
#include "config.hh"
#include <cctype>
#include "Subleading.hh"
#include "HEJ/config.hh"
#include "HEJ/YAMLreader.hh"
namespace HEJFOG{
using HEJ::set_from_yaml;
using HEJ::set_from_yaml_if_defined;
namespace{
//! Get YAML tree of supported options
/**
* The configuration file is checked against this tree of options
* in assert_all_options_known.
*/
YAML::Node const & get_supported_options(){
const static YAML::Node supported = [](){
YAML::Node supported;
static const auto opts = {
"process", "events", "subleading fraction","subleading channels",
"scales", "scale factors", "max scale ratio", "pdf",
"event output", "analysis", "import scales"
};
// add subnodes to "supported" - the assigned value is irrelevant
for(auto && opt: opts) supported[opt] = "";
for(auto && jet_opt: {"min pt", "peak pt", "algorithm", "R", "max rapidity"}){
supported["jets"][jet_opt] = "";
}
- for(auto && particle_type: {"Higgs", "Wp", "Wm", "Z"}){
+ for(auto && particle_type: {"Higgs", "Wp", "W+", "Wm", "W-", "Z"}){
for(auto && particle_opt: {"mass", "width"}){
supported["particle properties"][particle_type][particle_opt] = "";
}
supported["particle properties"][particle_type]["decays"]["into"] = "";
supported["particle properties"][particle_type]["decays"]["branching ratio"] = "";
}
for(auto && opt: {"mt", "use impact factors", "include bottom", "mb"}){
supported["Higgs coupling"][opt] = "";
}
for(auto && beam_opt: {"energy", "particles"}){
supported["beam"][beam_opt] = "";
}
for(auto && unweight_opt: {"sample size", "max deviation"}){
supported["unweight"][unweight_opt] = "";
}
for(auto && opt: {"name", "seed"}){
supported["random generator"][opt] = "";
}
return supported;
}();
return supported;
}
JetParameters get_jet_parameters(
YAML::Node const & node, std::string const & entry
){
const auto p = HEJ::get_jet_parameters(node, entry);
JetParameters result;
result.def = p.def;
result.min_pt = p.min_pt;
set_from_yaml(result.max_y, node, entry, "max rapidity");
set_from_yaml_if_defined(result.peak_pt, node, entry, "peak pt");
return result;
}
Beam get_Beam(
YAML::Node const & node, std::string const & entry
){
Beam beam;
std::vector<HEJ::ParticleID> particles;
set_from_yaml(beam.energy, node, entry, "energy");
set_from_yaml_if_defined(particles, node, entry, "particles");
if(! particles.empty()){
for(HEJ::ParticleID particle: particles){
if(particle != HEJ::pid::p && particle != HEJ::pid::p_bar){
throw std::invalid_argument{
"Unsupported value in option " + entry + ": particles:"
" only proton ('p') and antiproton ('p_bar') beams are supported"
};
}
}
if(particles.size() != 2){
throw std::invalid_argument{"Not exactly two beam particles"};
}
beam.particles.front() = particles.front();
beam.particles.back() = particles.back();
}
return beam;
}
std::vector<std::string> split(
std::string const & str, std::string const & delims
){
std::vector<std::string> result;
for(size_t begin, end = 0; end != str.npos;){
begin = str.find_first_not_of(delims, end);
if(begin == str.npos) break;
end = str.find_first_of(delims, begin + 1);
result.emplace_back(str.substr(begin, end - begin));
}
return result;
}
std::invalid_argument invalid_incoming(std::string const & what){
return std::invalid_argument{
"Incoming particle type " + what + " not supported,"
" incoming particles have to be 'p', 'p_bar' or partons"
};
}
std::invalid_argument invalid_outgoing(std::string const & what){
return std::invalid_argument{
"Outgoing particle type " + what + " not supported,"
" outgoing particles have to be 'j', 'photon', 'W+', 'W-', 'Z', 'H'"
};
}
Process get_process(
YAML::Node const & node, std::string const & entry
){
Process result;
std::string process_string;
set_from_yaml(process_string, node, entry);
assert(! process_string.empty());
const auto particles = split(process_string, " \n\t\v=>");
if(particles.size() < 3){
throw std::invalid_argument{
"Bad format in option process: '" + process_string
+ "', expected format is 'in1 in2 => out1 ...'"
};
}
result.incoming.front() = HEJ::to_ParticleID(particles[0]);
result.incoming.back() = HEJ::to_ParticleID(particles[1]);
for(size_t i = 0; i < result.incoming.size(); ++i){
const HEJ::ParticleID in = result.incoming[i];
if(
in != HEJ::pid::proton && in != HEJ::pid::p_bar
&& !HEJ::is_parton(in)
){
throw invalid_incoming(particles[i]);
}
}
result.njets = 0;
for(size_t i = result.incoming.size(); i < particles.size(); ++i){
assert(! particles[i].empty());
if(particles[i] == "j") ++result.njets;
else if(std::isdigit(particles[i].front())
&& particles[i].back() == 'j')
result.njets += std::stoi(particles[i]);
else{
const auto pid = HEJ::to_ParticleID(particles[i]);
if(!HEJ::is_AWZH_boson(pid)){
throw invalid_outgoing(particles[i]);
}
if(result.boson){
throw std::invalid_argument{
"More than one outgoing boson is not supported"
};
}
result.boson = pid;
}
}
if(result.njets < 2){
throw std::invalid_argument{
"Process has to include at least two jets ('j')"
};
}
return result;
}
HEJFOG::Subleading to_subleading_channel(YAML::Node const & yaml){
std::string name;
using HEJFOG::Subleading;
set_from_yaml(name, yaml);
if(name == "none")
return none;
if(name == "all")
return all;
if(name == "unordered" || name == "uno")
return uno;
if(name == "qqx")
return qqx;
throw HEJ::unknown_option("Unknown subleading channel '"+name+"'");
}
unsigned int get_subleading_channels(YAML::Node const & node){
using YAML::NodeType;
using HEJFOG::Subleading;
// all channels allowed by default
if(!node) return all;
switch(node.Type()){
case NodeType::Undefined:
return all;
case NodeType::Null:
return none;
case NodeType::Scalar:
return to_subleading_channel(node);
case NodeType::Map:
throw HEJ::invalid_type{"map is not a valid option for subleading channels"};
case NodeType::Sequence:
unsigned int channels = HEJFOG::Subleading::none;
for(auto && channel_node: node){
channels |= get_subleading_channels(channel_node);
}
return channels;
}
throw std::logic_error{"unreachable"};
}
Decay get_decay(YAML::Node const & node){
Decay decay;
set_from_yaml(decay.products, node, "into");
set_from_yaml(decay.branching_ratio, node, "branching ratio");
return decay;
}
std::vector<Decay> get_decays(YAML::Node const & node){
using YAML::NodeType;
if(!node) return {};
switch(node.Type()){
case NodeType::Null:
case NodeType::Undefined:
return {};
case NodeType::Scalar:
throw HEJ::invalid_type{"value is not a list of decays"};
case NodeType::Map:
return {get_decay(node)};
case NodeType::Sequence:
std::vector<Decay> result;
for(auto && decay_str: node){
result.emplace_back();
set_from_yaml(result.back().products, decay_str, "into");
set_from_yaml(result.back().branching_ratio, decay_str, "branching ratio");
}
return result;
}
throw std::logic_error{"unreachable"};
}
ParticleProperties get_particle_properties(
YAML::Node const & node, std::string const & entry
){
ParticleProperties result;
set_from_yaml(result.mass, node, entry, "mass");
set_from_yaml(result.width, node, entry, "width");
try{
result.decays = get_decays(node[entry]["decays"]);
}
catch(HEJ::missing_option const & ex){
throw HEJ::missing_option{entry + ": decays: " + ex.what()};
}
catch(HEJ::invalid_type const & ex){
throw HEJ::invalid_type{entry + ": decays: " + ex.what()};
}
return result;
}
ParticlesPropMap get_all_particles_properties(YAML::Node const & node){
ParticlesPropMap result;
- using namespace HEJ;
- // @TODO allow more synonyms
- if(node["Higgs"])
- result[pid::Higgs] = get_particle_properties(node,"Higgs");
- if(node["Wp"])
- result[pid::Wp] = get_particle_properties(node,"Wp");
- if(node["Wm"])
- result[pid::Wm] = get_particle_properties(node,"Wm");
- if(node["Z"])
- result[pid::Z] = get_particle_properties(node,"Z");
+ for(auto const & entry: node) {
+ const auto name = entry.first.as<std::string>();
+ const auto id = HEJ::to_ParticleID(name);
+ result.emplace(id, get_particle_properties(node,name));
+ }
return result;
}
UnweightSettings get_unweight(
YAML::Node const & node, std::string const & entry
){
UnweightSettings result;
set_from_yaml(result.sample_size, node, entry, "sample size");
if(result.sample_size <= 0){
throw std::invalid_argument{
"negative sample size " + std::to_string(result.sample_size)
};
}
set_from_yaml(result.max_dev, node, entry, "max deviation");
return result;
}
Config to_Config(YAML::Node const & yaml){
try{
HEJ::assert_all_options_known(yaml, get_supported_options());
}
catch(HEJ::unknown_option const & ex){
throw HEJ::unknown_option{std::string{"Unknown option '"} + ex.what() + "'"};
}
Config config;
config.process = get_process(yaml, "process");
set_from_yaml(config.events, yaml, "events");
config.jets = get_jet_parameters(yaml, "jets");
config.beam = get_Beam(yaml, "beam");
for(size_t i = 0; i < config.process.incoming.size(); ++i){
const auto & in = config.process.incoming[i];
using namespace HEJ::pid;
if( (in == p || in == p_bar) && in != config.beam.particles[i]){
throw std::invalid_argument{
"Particle type of beam " + std::to_string(i+1) + " incompatible"
+ " with type of incoming particle " + std::to_string(i+1)
};
}
}
set_from_yaml(config.pdf_id, yaml, "pdf");
set_from_yaml(config.subleading_fraction, yaml, "subleading fraction");
if(config.subleading_fraction < 0 || config.subleading_fraction > 1){
throw std::invalid_argument{
"subleading fraction has to be between 0 and 1"
};
}
if(config.subleading_fraction == 0)
config.subleading_channels = Subleading::none;
else
config.subleading_channels = get_subleading_channels(yaml["subleading channels"]);
if(!config.process.boson && config.subleading_channels != Subleading::none)
throw HEJ::not_implemented("Subleading processes for pure Jet production not implemented yet");
if(yaml["particle properties"]){
config.particles_properties = get_all_particles_properties(
yaml["particle properties"]);
}
if(config.process.boson
&& config.particles_properties.find(*(config.process.boson))
== config.particles_properties.end())
throw HEJ::missing_option("Process wants to generate boson "
- +std::to_string(*(config.process.boson))+", but boson properties are missing");
+ +std::to_string(*(config.process.boson))+", but particle properties are missing");
set_from_yaml_if_defined(config.analysis_parameters, yaml, "analysis");
config.scales = HEJ::to_ScaleConfig(yaml);
set_from_yaml_if_defined(config.output, yaml, "event output");
config.rng = HEJ::to_RNGConfig(yaml, "random generator");
config.Higgs_coupling = HEJ::get_Higgs_coupling(yaml, "Higgs coupling");
if(yaml["unweight"]) config.unweight = get_unweight(yaml, "unweight");
return config;
}
} // namespace anonymous
Config load_config(std::string const & config_file){
try{
return to_Config(YAML::LoadFile(config_file));
}
catch(...){
std::cerr << "Error reading " << config_file << ":\n ";
throw;
}
}
}
diff --git a/FixedOrderGen/src/main.cc b/FixedOrderGen/src/main.cc
index 3cbd54b..7e0cdf3 100644
--- a/FixedOrderGen/src/main.cc
+++ b/FixedOrderGen/src/main.cc
@@ -1,248 +1,246 @@
/**
* Name: main.cc
* Authors: Jeppe R. Andersen
*/
-#include <fstream>
#include <algorithm>
-#include <memory>
#include <chrono>
+#include <fstream>
#include <iostream>
#include <map>
+#include <memory>
#include "yaml-cpp/yaml.h"
-#include "config.hh"
-
#include "LHEF/LHEF.h"
+
#include "HEJ/CombinedEventWriter.hh"
#include "HEJ/get_analysis.hh"
-#include "HEJ/utility.hh"
-//#include "HEJ/EventReweighter.hh"
-#include "HEJ/stream.hh"
#include "HEJ/LesHouchesWriter.hh"
-#include "HEJ/ProgressBar.hh"
#include "HEJ/make_RNG.hh"
+#include "HEJ/ProgressBar.hh"
+#include "HEJ/stream.hh"
+#include "config.hh"
+#include "CrossSectionAccumulator.hh"
#include "EventGenerator.hh"
#include "PhaseSpacePoint.hh"
#include "Unweighter.hh"
-#include "CrossSectionAccumulator.hh"
#include "Version.hh"
namespace{
constexpr auto banner =
" __ ___ __ ______ __ __ \n"
" / / / (_)___ _/ /_ / ____/___ ___ _________ ___ __ / /__ / /______ \n"
" / /_/ / / __ `/ __ \\ / __/ / __ \\/ _ \\/ ___/ __ `/ / / / __ / / _ \\/ __/ ___/ \n"
" / __ / / /_/ / / / / / /___/ / / / __/ / / /_/ / /_/ / / /_/ / __/ /_(__ ) \n"
" /_/ /_/_/\\__, /_/ /_/ /_____/_/ /_/\\___/_/ \\__, /\\__, / \\____/\\___/\\__/____/ \n"
" ____///__/ __ ____ ///__//____/ ______ __ \n"
" / ____(_) _____ ____/ / / __ \\_________/ /__ _____ / ____/__ ____ ___ _________ _/ /_____ _____\n"
" / /_ / / |/_/ _ \\/ __ / / / / / ___/ __ / _ \\/ ___/ / / __/ _ \\/ __ \\/ _ \\/ ___/ __ `/ __/ __ \\/ ___/\n"
" / __/ / /> </ __/ /_/ / / /_/ / / / /_/ / __/ / / /_/ / __/ / / / __/ / / /_/ / /_/ /_/ / / \n"
" /_/ /_/_/|_|\\___/\\__,_/ \\____/_/ \\__,_/\\___/_/ \\____/\\___/_/ /_/\\___/_/ \\__,_/\\__/\\____/_/ \n"
;
constexpr double invGeV2_to_pb = 389379292.;
constexpr long long max_warmup_events = 10000;
}
HEJFOG::Config load_config(char const * filename){
try{
return HEJFOG::load_config(filename);
}
catch(std::exception const & exc){
std::cerr << "Error: " << exc.what() << '\n';
std::exit(EXIT_FAILURE);
}
}
std::unique_ptr<HEJ::Analysis> get_analysis(
YAML::Node const & parameters
){
try{
return HEJ::get_analysis(parameters);
}
catch(std::exception const & exc){
std::cerr << "Failed to load analysis: " << exc.what() << '\n';
std::exit(EXIT_FAILURE);
}
}
void rescale_weights(HEJ::Event & ev, double factor) {
ev.central().weight *= factor;
for(auto & var: ev.variations()){
var.weight *= factor;
}
}
int main(int argn, char** argv) {
using namespace std::string_literals;
if (argn < 2) {
- std::cerr << "\n# Usage:\n.FOgen config_file\n";
+ std::cerr << "\n# Usage:\n." << argv[0] << " config_file\n";
return EXIT_FAILURE;
}
std::cout << banner;
std::cout << "Version " << HEJFOG::Version::String()
<< ", revision " << HEJFOG::Version::revision() << std::endl;
fastjet::ClusterSequence::print_banner();
using clock = std::chrono::system_clock;
const auto start_time = clock::now();
// read configuration
auto config = load_config(argv[1]);
std::unique_ptr<HEJ::Analysis> analysis = get_analysis(
config.analysis_parameters
);
assert(analysis != nullptr);
auto ran = HEJ::make_RNG(config.rng.name, config.rng.seed);
assert(ran != nullptr);
HEJ::ScaleGenerator scale_gen{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
std::move(scale_gen),
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
*ran
};
LHEF::HEPRUP heprup;
heprup.IDBMUP=std::pair<long,long>(config.beam.particles[0], config.beam.particles[1]);
heprup.EBMUP=std::make_pair(config.beam.energy, config.beam.energy);
heprup.PDFGUP=std::make_pair(0,0);
heprup.PDFSUP=std::make_pair(config.pdf_id,config.pdf_id);
heprup.NPRUP=1;
heprup.XSECUP=std::vector<double>(1.);
heprup.XERRUP=std::vector<double>(1.);
heprup.LPRUP=std::vector<int>{1};
heprup.generators.emplace_back(LHEF::XMLTag{});
heprup.generators.back().name = HEJFOG::Version::package_name();
heprup.generators.back().version = HEJFOG::Version::String();
HEJ::CombinedEventWriter writer{config.output, heprup};
HEJ::optional<HEJFOG::Unweighter> unweighter{};
std::map<HEJFOG::Status, int> status_counter;
std::vector<HEJ::Event> events;
int trials = 0;
// warm-up phase to train unweighter
if(config.unweight) {
std::cout << "Calibrating unweighting ...\n";
const auto warmup_start = clock::now();
const size_t warmup_events = config.unweight->sample_size;
HEJ::ProgressBar<size_t> warmup_progress{std::cout, warmup_events};
for(; events.size() < warmup_events; ++trials){
auto ev = generator.gen_event();
++status_counter[generator.status()];
if(generator.status() == HEJFOG::good && analysis->pass_cuts(ev, ev)) {
events.emplace_back(std::move(ev));
++warmup_progress;
}
}
std::cout << std::endl;
unweighter = HEJFOG::Unweighter{
begin(events), end(events), config.unweight->max_dev, *ran,
config.jets.peak_pt?(*config.jets.peak_pt):0.
};
std::vector<HEJ::Event> unweighted_events;
for(auto && ev: events) {
auto unweighted = unweighter->unweight(std::move(ev));
if(unweighted) {
unweighted_events.emplace_back(std::move(*unweighted));
}
}
events = std::move(unweighted_events);
if(events.empty()) {
std::cerr <<
"Failed to generate events. Please increase \"unweight: sample size\""
" or reduce \"unweight: max deviation\"\n";
return EXIT_FAILURE;
}
const auto warmup_end = clock::now();
const double completion = static_cast<double>(events.size())/config.events;
const std::chrono::duration<double> remaining_time =
(warmup_end- warmup_start)*(1./completion - 1);
const auto finish = clock::to_time_t(
std::chrono::time_point_cast<std::chrono::seconds>(warmup_end + remaining_time)
);
std::cout
<< "Generated " << events.size() << "/" << config.events << " events ("
<< static_cast<int>(std::round(100*completion)) << "%)\n"
<< "Estimated remaining generation time: "
<< remaining_time.count() << " seconds ("
<< std::put_time(std::localtime(&finish), "%c") << ")\n\n";
}
HEJ::ProgressBar<long long> progress{std::cout, config.events};
progress.increment(events.size());
events.reserve(config.events);
for(; events.size() < static_cast<size_t>(config.events); ++trials){
auto ev = generator.gen_event();
++status_counter[generator.status()];
if(generator.status() == HEJFOG::good && analysis->pass_cuts(ev, ev)) {
if(unweighter) {
auto unweighted = unweighter->unweight(std::move(ev));
if(! unweighted) continue;
ev = std::move(*unweighted);
}
events.emplace_back(std::move(ev));
++progress;
}
}
std::cout << std::endl;
HEJFOG::CrossSectionAccumulator xs;
for(auto & ev: events){
rescale_weights(ev, invGeV2_to_pb/trials);
analysis->fill(ev, ev);
writer.write(ev);
xs.fill(ev);
}
analysis->finalise();
const std::chrono::duration<double> run_time = (clock::now() - start_time);
std::cout << "\nTask Runtime: " << run_time.count() << " seconds.\n\n";
std::cout.precision(10);
std::cout.setf(std::ios::fixed);
std::cout
<< " " << std::left << std::setw(20)
<< "Cross section: " << xs.total().value
<< " +- " << std::sqrt(xs.total().error) << " (pb)\n";
for(auto const & xs_type: xs) {
std::cout
<< " " << std::left << std::setw(20)
<< (HEJ::event_type::names[xs_type.first] + ": "s)
<< xs_type.second.value << " +- "
<< std::sqrt(xs_type.second.error) << " (pb)\n";
}
std::cout << '\n';
for(auto && entry: status_counter){
const double fraction = static_cast<double>(entry.second)/trials;
const int percent = std::round(100*fraction);
std::cout << "status "
<< std::left << std::setw(16) << (to_string(entry.first) + ":")
<< " [";
for(int i = 0; i < percent/2; ++i) std::cout << '#';
for(int i = percent/2; i < 50; ++i) std::cout << ' ';
std::cout << "] " << percent << "%\n";
}
}
diff --git a/FixedOrderGen/t/2j.cc b/FixedOrderGen/t/2j.cc
index 8eabfc4..80bdff3 100644
--- a/FixedOrderGen/t/2j.cc
+++ b/FixedOrderGen/t/2j.cc
@@ -1,58 +1,59 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
#include <algorithm>
#include <cmath>
#include <cassert>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
#include "HEJ/Mixmax.hh"
+#include "HEJ/Event.hh"
#include "HEJ/PDF.hh"
#include "HEJ/MatrixElement.hh"
using namespace HEJFOG;
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 86.42031848*1e6; //calculated with "combined" HEJ svn r3480
auto config = load_config("config_2j.yml");
HEJ::Mixmax ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(generator.status() != good) continue;
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << '\n';
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.01*xs);
}
diff --git a/FixedOrderGen/t/4j.cc b/FixedOrderGen/t/4j.cc
index b459200..5b4e1b4 100644
--- a/FixedOrderGen/t/4j.cc
+++ b/FixedOrderGen/t/4j.cc
@@ -1,59 +1,60 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
#include <algorithm>
#include <cmath>
#include <cassert>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
#include "HEJ/Mixmax.hh"
+#include "HEJ/Event.hh"
#include "HEJ/PDF.hh"
#include "HEJ/MatrixElement.hh"
using namespace HEJFOG;
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 0.81063619*1e6; //calculated with "combined" HEJ svn r3480
auto config = load_config("config_2j.yml");
config.process.njets = 4;
HEJ::Mixmax ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(generator.status() != good) continue;
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << '\n';
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.03*xs);
}
diff --git a/FixedOrderGen/t/h_2j.cc b/FixedOrderGen/t/h_2j.cc
index 26d91c5..3e3135e 100644
--- a/FixedOrderGen/t/h_2j.cc
+++ b/FixedOrderGen/t/h_2j.cc
@@ -1,66 +1,67 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
#include <algorithm>
#include <cmath>
#include <cassert>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
#include "HEJ/Ranlux64.hh"
+#include "HEJ/Event.hh"
#include "HEJ/PDF.hh"
#include "HEJ/MatrixElement.hh"
using namespace HEJFOG;
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 2.04928; // +- 0.00377252
//calculated with HEJ revision 9570e3809613272ac4b8bf3236279ba23cf64d20
auto config = load_config("config_h_2j.yml");
HEJ::Ranlux64 ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(generator.status() != good) continue;
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
const auto the_Higgs = std::find_if(
begin(ev.outgoing()), end(ev.outgoing()),
[](HEJ::Particle const & p){ return p.type == HEJ::ParticleID::h; }
);
assert(the_Higgs != end(ev.outgoing()));
if(std::abs(the_Higgs->rapidity()) > 5.) continue;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << std::endl;
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.01*xs);
}
diff --git a/FixedOrderGen/t/h_2j_decay.cc b/FixedOrderGen/t/h_2j_decay.cc
index 6ecc37c..8454b7b 100644
--- a/FixedOrderGen/t/h_2j_decay.cc
+++ b/FixedOrderGen/t/h_2j_decay.cc
@@ -1,84 +1,86 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
#include <algorithm>
#include <cmath>
#include <cassert>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
-#include "HEJ/Ranlux64.hh"
-#include "HEJ/PDF.hh"
+#include "HEJ/Event.hh"
#include "HEJ/MatrixElement.hh"
+#include "HEJ/Particle.hh"
+#include "HEJ/PDF.hh"
+#include "HEJ/Ranlux64.hh"
#include "HEJ/utility.hh"
using namespace HEJFOG;
bool pass_dR_cut(
std::vector<fastjet::PseudoJet> const & jets,
std::vector<HEJ::Particle> const & photons
){
constexpr double delta_R_min = 0.7;
for(auto const & jet: jets){
for(auto const & photon: photons){
if(jet.delta_R(photon.p) < delta_R_min) return false;
}
}
return true;
}
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 0.00429198; // +- 1.0488e-05
//calculated with HEJ revision 9570e3809613272ac4b8bf3236279ba23cf64d20
auto config = load_config("config_h_2j_decay.yml");
HEJ::Ranlux64 ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(generator.status() != good) continue;
assert(ev.decays().size() == 1);
const auto decay = begin(ev.decays());
assert(ev.outgoing().size() > decay->first);
const auto & the_Higgs = ev.outgoing()[decay->first];
assert(the_Higgs.type == HEJ::pid::Higgs);
assert(decay->second.size() == 2);
auto const & gamma = decay->second;
assert(gamma[0].type == HEJ::pid::photon);
assert(gamma[1].type == HEJ::pid::photon);
assert(HEJ::nearby_ep(gamma[0].p + gamma[1].p, the_Higgs.p, 1e-6));
if(!pass_dR_cut(ev.jets(), gamma)) continue;
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << std::endl;
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.012*xs);
}
diff --git a/FixedOrderGen/t/h_3j.cc b/FixedOrderGen/t/h_3j.cc
index 540be9a..cad089a 100644
--- a/FixedOrderGen/t/h_3j.cc
+++ b/FixedOrderGen/t/h_3j.cc
@@ -1,67 +1,68 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
#include <algorithm>
#include <cmath>
#include <cassert>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
#include "HEJ/Ranlux64.hh"
-#include "HEJ/PDF.hh"
+#include "HEJ/Event.hh"
#include "HEJ/MatrixElement.hh"
+#include "HEJ/PDF.hh"
using namespace HEJFOG;
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 1.07807; // +- 0.0071
//calculated with HEJ revision 93efdc851b02a907a6fcc63956387f9f4c1111c2 +1
auto config = load_config("config_h_2j.yml");
config.process.njets = 3;
HEJ::Ranlux64 ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(generator.status() != good) continue;
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
const auto the_Higgs = std::find_if(
begin(ev.outgoing()), end(ev.outgoing()),
[](HEJ::Particle const & p){ return p.type == HEJ::ParticleID::h; }
);
assert(the_Higgs != end(ev.outgoing()));
if(std::abs(the_Higgs->rapidity()) > 5.) continue;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << std::endl;
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.02*xs);
}
diff --git a/FixedOrderGen/t/h_3j_uno1.cc b/FixedOrderGen/t/h_3j_uno1.cc
index ee60d97..4c0f6f3 100644
--- a/FixedOrderGen/t/h_3j_uno1.cc
+++ b/FixedOrderGen/t/h_3j_uno1.cc
@@ -1,71 +1,72 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
// check that adding uno emissions doesn't change the FKL cross section
#include <algorithm>
-#include <cmath>
#include <cassert>
+#include <cmath>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
-#include "Subleading.hh"
#include "HEJ/Ranlux64.hh"
+#include "Subleading.hh"
-#include "HEJ/PDF.hh"
+#include "HEJ/Event.hh"
#include "HEJ/MatrixElement.hh"
+#include "HEJ/PDF.hh"
using namespace HEJFOG;
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 0.0243548; // +- 0.000119862
//calculated with HEJ revision 9570e3809613272ac4b8bf3236279ba23cf64d20
auto config = load_config("config_h_2j.yml");
config.process.njets = 3;
config.process.incoming = {HEJ::pid::u, HEJ::pid::u};
config.subleading_channels = HEJFOG::Subleading::uno;
HEJ::Ranlux64 ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
int uno_found = 0;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(generator.status() != good) continue;
if(ev.type() != HEJ::event_type::FKL){
++uno_found;
continue;
}
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << '\n';
std::cout << uno_found << " events with unordered emission" << std::endl;
assert(uno_found > 0);
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.05*xs);
}
diff --git a/FixedOrderGen/t/h_3j_uno2.cc b/FixedOrderGen/t/h_3j_uno2.cc
index cf28f57..5c6c409 100644
--- a/FixedOrderGen/t/h_3j_uno2.cc
+++ b/FixedOrderGen/t/h_3j_uno2.cc
@@ -1,66 +1,67 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
// check uno cross section
#include <algorithm>
-#include <cmath>
#include <cassert>
+#include <cmath>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
-#include "Subleading.hh"
#include "HEJ/Ranlux64.hh"
+#include "Subleading.hh"
-#include "HEJ/PDF.hh"
+#include "HEJ/Event.hh"
#include "HEJ/MatrixElement.hh"
+#include "HEJ/PDF.hh"
using namespace HEJFOG;
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 0.00347538; // +- 3.85875e-05
//calculated with HEJ revision 9570e3809613272ac4b8bf3236279ba23cf64d20
auto config = load_config("config_h_2j.yml");
config.process.njets = 3;
config.process.incoming = {HEJ::pid::u, HEJ::pid::u};
config.subleading_fraction = 1.;
config.subleading_channels = HEJFOG::Subleading::uno;
HEJ::Ranlux64 ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(ev.type() == HEJ::event_type::FKL) continue;
if(generator.status() != good) continue;
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << std::endl;
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.05*xs);
}
diff --git a/FixedOrderGen/t/h_5j.cc b/FixedOrderGen/t/h_5j.cc
index 6bd9e41..6aa3d40 100644
--- a/FixedOrderGen/t/h_5j.cc
+++ b/FixedOrderGen/t/h_5j.cc
@@ -1,62 +1,63 @@
#ifdef NDEBUG
#undef NDEBUG
#endif
// This is a regression test
// the reference cross section has not been checked against any other program
#include <algorithm>
-#include <cmath>
#include <cassert>
+#include <cmath>
#include <iostream>
#include "config.hh"
#include "EventGenerator.hh"
#include "HEJ/Ranlux64.hh"
-#include "HEJ/PDF.hh"
+#include "HEJ/Event.hh"
#include "HEJ/MatrixElement.hh"
+#include "HEJ/PDF.hh"
using namespace HEJFOG;
int main(){
constexpr double invGeV2_to_pb = 389379292.;
constexpr double xs_ref = 0.252273; // +- 0.00657742
//calculated with HEJ revision 9570e3809613272ac4b8bf3236279ba23cf64d20
auto config = load_config("config_h_2j.yml");
config.process.njets = 5;
HEJ::Ranlux64 ran{};
HEJFOG::EventGenerator generator{
config.process,
config.beam,
HEJ::ScaleGenerator{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
},
config.jets,
config.pdf_id,
config.subleading_fraction,
config.subleading_channels,
config.particles_properties,
config.Higgs_coupling,
ran
};
double xs = 0., xs_err = 0.;
for (int trials = 0; trials < config.events; ++trials){
auto ev = generator.gen_event();
if(generator.status() != good) continue;
ev.central().weight *= invGeV2_to_pb;
ev.central().weight /= config.events;
xs += ev.central().weight;
xs_err += ev.central().weight*ev.central().weight;
}
xs_err = std::sqrt(xs_err);
std::cout << xs_ref << " ~ " << xs << " +- " << xs_err << std::endl;
assert(std::abs(xs - xs_ref) < 3*xs_err);
assert(xs_err < 0.06*xs);
}
diff --git a/cmake/Modules/FindHepMC.cmake b/cmake/Modules/FindHepMC.cmake
index 97ec9ba..a311f15 100644
--- a/cmake/Modules/FindHepMC.cmake
+++ b/cmake/Modules/FindHepMC.cmake
@@ -1,228 +1,218 @@
# Distributed under the OSI-approved BSD 3-Clause License. See accompanying
# file Copyright.txt or https://cmake.org/licensing for details.
# This is a slightly modified version of FindGSL.cmake taken from cmake 3.7
#.rst:
# FindHepMC
# --------
#
# Find the native HepMC includes and libraries.
#
# HepMC package is an object oriented, C++ event record for High Energy
# Physics Monte Carlo generators and simulation. It is free software
# under the GNU General Public License.
#
# Imported Targets
# ^^^^^^^^^^^^^^^^
#
# If HepMC is found, this module defines the following
# :prop_tgt:`IMPORTED` target::
#
# HepMC::HepMC - The main HepMC library.
#
# Result Variables
# ^^^^^^^^^^^^^^^^
#
# This module will set the following variables in your project::
#
# HepMC_FOUND - True if HepMC found on the local system
# HepMC_INCLUDE_DIRS - Location of HepMC header files.
# HepMC_LIBRARIES - The HepMC libraries.
# HepMC_VERSION - The version of the discovered HepMC install.
#
# Hints
# ^^^^^
#
# Set ``HepMC_ROOT_DIR`` to a directory that contains a HepMC installation.
#
# This script expects to find libraries at ``$HepMC_ROOT_DIR/lib`` and the HepMC
# headers at ``$HepMC_ROOT_DIR/include/HepMC``. The library directory may
# optionally provide Release and Debug folders. For Unix-like systems, this
# script will use ``$HepMC_ROOT_DIR/bin/HepMC-config`` (if found) to aid in the
# discovery HepMC.
#
# Cache Variables
# ^^^^^^^^^^^^^^^
#
# This module may set the following variables depending on platform and type
# of HepMC installation discovered. These variables may optionally be set to
# help this module find the correct files::
#
# HepMC_CONFIG_EXECUTABLE - Location of the ``HepMC-config`` script (if any).
# HepMC_LIBRARY - Location of the HepMC library.
# HepMC_LIBRARY_DEBUG - Location of the debug HepMC library (if any).
#
# Include these modules to handle the QUIETLY and REQUIRED arguments.
include(FindPackageHandleStandardArgs)
#=============================================================================
# If the user has provided ``HepMC_ROOT_DIR``, use it! Choose items found
# at this location over system locations.
if( EXISTS "$ENV{HepMC_ROOT_DIR}" )
file( TO_CMAKE_PATH "$ENV{HepMC_ROOT_DIR}" HepMC_ROOT_DIR )
set( HepMC_ROOT_DIR "${HepMC_ROOT_DIR}" CACHE PATH "Prefix for HepMC installation." )
endif()
if( NOT EXISTS "${HepMC_ROOT_DIR}" )
set( HepMC_USE_PKGCONFIG ON )
endif()
#=============================================================================
# As a first try, use the PkgConfig module. This will work on many
# *NIX systems. See :module:`findpkgconfig`
# This will return ``HepMC_INCLUDEDIR`` and ``HepMC_LIBDIR`` used below.
if( HepMC_USE_PKGCONFIG )
find_package(PkgConfig)
pkg_check_modules( HepMC QUIET HepMC )
if( EXISTS "${HepMC_INCLUDEDIR}" )
get_filename_component( HepMC_ROOT_DIR "${HepMC_INCLUDEDIR}" DIRECTORY CACHE)
endif()
endif()
#=============================================================================
# Set HepMC_INCLUDE_DIRS and HepMC_LIBRARIES. If we skipped the PkgConfig step, try
# to find the libraries at $HepMC_ROOT_DIR (if provided), in the directory
# suggested by HepMC-config (if available), or in standard system
# locations. These find_library and find_path calls will prefer custom
# locations over standard locations (HINTS). If the requested file is found
# neither at the HINTS location nor via HepMC-config, standard system locations
# will be still be searched (/usr/lib64 (Redhat), lib/i386-linux-gnu (Debian)).
# If we didn't use PkgConfig, try to find the version via HepMC-config
if( NOT HepMC_VERSION )
find_program( HepMC_CONFIG_EXECUTABLE
NAMES HepMC-config
HINTS "${HepMC_ROOT_DIR}/bin"
)
if( EXISTS "${HepMC_CONFIG_EXECUTABLE}" )
execute_process(
COMMAND "${HepMC_CONFIG_EXECUTABLE}" --version
OUTPUT_VARIABLE HepMC_VERSION
OUTPUT_STRIP_TRAILING_WHITESPACE )
execute_process(
COMMAND "${HepMC_CONFIG_EXECUTABLE}" --incdir
OUTPUT_VARIABLE HepMC_CONFIG_INCLUDEDIR
OUTPUT_STRIP_TRAILING_WHITESPACE )
execute_process(
COMMAND "${HepMC_CONFIG_EXECUTABLE}" --libdir
OUTPUT_VARIABLE HepMC_CONFIG_LIBDIR
OUTPUT_STRIP_TRAILING_WHITESPACE )
endif()
endif()
find_path( HepMC_INCLUDE_DIR
NAMES HepMC/HepMC.h HepMC/HepMCDefs.h
HINTS ${HepMC_ROOT_DIR}/include ${HepMC_INCLUDEDIR} ${HepMC_CONFIG_INCLUDEDIR}
)
find_library( HepMC_LIBRARY
NAMES HepMC
HINTS ${HepMC_ROOT_DIR}/lib ${HepMC_LIBDIR} ${HepMC_CONFIG_LIBDIR}
PATH_SUFFIXES Release Debug
)
# Do we also have debug versions?
find_library( HepMC_LIBRARY_DEBUG
NAMES HepMC
HINTS ${HepMC_ROOT_DIR}/lib ${HepMC_LIBDIR} ${HepMC_CONFIG_LIBDIR}
PATH_SUFFIXES Debug
)
set( HepMC_INCLUDE_DIRS ${HepMC_INCLUDE_DIR} )
set( HepMC_LIBRARIES ${HepMC_LIBRARY} )
if( NOT HepMC_VERSION )
if(IS_DIRECTORY ${HepMC_INCLUDE_DIR})
file(STRINGS "${HepMC_INCLUDE_DIR}/HepMC/HepMCDefs.h" _HepMC_DEFS)
file(STRINGS "${HepMC_INCLUDE_DIR}/HepMC/Version.h" _HepMC_VERS)
string(
REGEX MATCH
"#define *HEPMC_VERSION *\"[^\"]*\""
_HepMC_VERSION_STR "${_HepMC_DEFS} ${_HepMC_VERS}"
)
string(
REGEX MATCH
"[0-9]*\\.[0-9]*\\.[0-9]*"
HepMC_VERSION ${_HepMC_VERSION_STR}
)
endif()
endif()
if( HepMC_VERSION )
- string(
- REGEX MATCH
- "^[0-9]*"
- HepMC_VERSION_MAJOR ${HepMC_VERSION}
- )
- string(
- REGEX REPLACE
- "^[0-9]*\\.([0-9]*)" "\\1"
- HepMC_VERSION_MINOR ${HepMC_VERSION}
- )
- string(
- REGEX MATCH
- "[0-9]*$"
- HepMC_VERSION_PATCH ${HepMC_VERSION}
- )
+ string(REPLACE "." ";" t_list ${HepMC_VERSION})
+ list(APPEND t_list 0 0) # add a buffer in case supversion not set
+ list(GET t_list 0 HepMC_VERSION_MAJOR)
+ list(GET t_list 1 HepMC_VERSION_MINOR)
+ list(GET t_list 2 HepMC_VERSION_PATCH)
endif()
#=============================================================================
# handle the QUIETLY and REQUIRED arguments and set HepMC_FOUND to TRUE if all
# listed variables are TRUE
find_package_handle_standard_args( HepMC
FOUND_VAR
HepMC_FOUND
REQUIRED_VARS
HepMC_INCLUDE_DIR
HepMC_LIBRARY
VERSION_VAR
HepMC_VERSION
)
mark_as_advanced( HepMC_ROOT_DIR HepMC_VERSION HepMC_LIBRARY HepMC_INCLUDE_DIR
HepMC_LIBRARY_DEBUG HepMC_USE_PKGCONFIG HepMC_CONFIG )
#=============================================================================
# Register imported libraries:
# 1. If we can find a Windows .dll file (or if we can find both Debug and
# Release libraries), we will set appropriate target properties for these.
# 2. However, for most systems, we will only register the import location and
# include directory.
# Look for dlls, or Release and Debug libraries.
if(WIN32)
string( REPLACE ".lib" ".dll" HepMC_LIBRARY_DLL "${HepMC_LIBRARY}" )
string( REPLACE ".lib" ".dll" HepMC_LIBRARY_DEBUG_DLL "${HepMC_LIBRARY_DEBUG}" )
endif()
if( HepMC_FOUND AND NOT TARGET HepMC::HepMC )
if( EXISTS "${HepMC_LIBRARY_DLL}")
# Windows systems with dll libraries.
add_library( HepMC::HepMC SHARED IMPORTED )
add_library( HepMC::HepMCcblas SHARED IMPORTED )
# Windows with dlls, but only Release libraries.
set_target_properties( HepMC::HepMC PROPERTIES
IMPORTED_LOCATION_RELEASE "${HepMC_LIBRARY_DLL}"
IMPORTED_IMPLIB "${HepMC_LIBRARY}"
INTERFACE_INCLUDE_DIRECTORIES "${HepMC_INCLUDE_DIRS}"
IMPORTED_CONFIGURATIONS Release
IMPORTED_LINK_INTERFACE_LANGUAGES "CXX"
)
# If we have both Debug and Release libraries
if( EXISTS "${HepMC_LIBRARY_DEBUG_DLL}")
set_property( TARGET HepMC::HepMC APPEND PROPERTY IMPORTED_CONFIGURATIONS Debug )
set_target_properties( HepMC::HepMC PROPERTIES
IMPORTED_LOCATION_DEBUG "${HepMC_LIBRARY_DEBUG_DLL}"
IMPORTED_IMPLIB_DEBUG "${HepMC_LIBRARY_DEBUG}" )
endif()
else()
# For all other environments (ones without dll libraries), create
# the imported library targets.
add_library( HepMC::HepMC UNKNOWN IMPORTED )
set_target_properties( HepMC::HepMC PROPERTIES
IMPORTED_LOCATION "${HepMC_LIBRARY}"
INTERFACE_INCLUDE_DIRECTORIES "${HepMC_INCLUDE_DIRS}"
IMPORTED_LINK_INTERFACE_LANGUAGES "CXX"
)
endif()
endif()
diff --git a/cmake/Modules/FindQCDloop.cmake b/cmake/Modules/FindQCDloop.cmake
index 063ef5b..5b05fc9 100644
--- a/cmake/Modules/FindQCDloop.cmake
+++ b/cmake/Modules/FindQCDloop.cmake
@@ -1,200 +1,205 @@
# Distributed under the OSI-approved BSD 3-Clause License. See accompanying
# file Copyright.txt or https://cmake.org/licensing for details.
# This is a slightly modified version of FindGSL.cmake taken from cmake 3.7
#.rst:
# FindQCDloop
# --------
#
# Find the native QCDloop includes and libraries.
#
# QCDLoop is a library for one-loop scalar Feynman integrals. It is free
# software under the GNU General Public License.
#
# Imported Targets
# ^^^^^^^^^^^^^^^^
#
# If QCDloop is found, this module defines the following
# :prop_tgt:`IMPORTED` target::
#
# QCDloop::qcdloop - The main QCDloop library.
#
# Result Variables
# ^^^^^^^^^^^^^^^^
#
# This module will set the following variables in your project::
#
# QCDloop_FOUND - True if QCDloop found on the local system
# QCDloop_INCLUDE_DIRS - Location of QCDloop header files.
# QCDloop_LIBRARIES - The QCDloop libraries.
# QCDloop_VERSION - The version of the discovered QCDloop install.
#
# Hints
# ^^^^^
#
# Set ``QCDloop_ROOT_DIR`` to a directory that contains a QCDloop installation.
#
# This script expects to find libraries at ``$QCDloop_ROOT_DIR/lib`` and the QCDloop
# headers at ``$QCDloop_ROOT_DIR/include/qcdloop``. The library directory may
# optionally provide Release and Debug folders. For Unix-like systems, this
# script will use ``$QCDloop_ROOT_DIR/bin/qcdloop-config`` (if found) to aid in the
# discovery QCDloop.
#
# Cache Variables
# ^^^^^^^^^^^^^^^
#
# This module may set the following variables depending on platform and type
# of QCDloop installation discovered. These variables may optionally be set to
# help this module find the correct files::
#
# QCDloop_CONFIG_EXECUTABLE - Location of the ``qcdloop-config`` script (if any).
# QCDloop_LIBRARY - Location of the QCDloop library.
# QCDloop_LIBRARY_DEBUG - Location of the debug QCDloop library (if any).
#
# Include these modules to handle the QUIETLY and REQUIRED arguments.
include(FindPackageHandleStandardArgs)
#=============================================================================
# If the user has provided ``QCDloop_ROOT_DIR``, use it! Choose items found
# at this location over system locations.
if( EXISTS "$ENV{QCDloop_ROOT_DIR}" )
file( TO_CMAKE_PATH "$ENV{QCDloop_ROOT_DIR}" QCDloop_ROOT_DIR )
set( QCDloop_ROOT_DIR "${QCDloop_ROOT_DIR}" CACHE PATH "Prefix for QCDloop installation." )
endif()
if( NOT EXISTS "${QCDloop_ROOT_DIR}" )
set( QCDloop_USE_PKGCONFIG ON )
endif()
#=============================================================================
# As a first try, use the PkgConfig module. This will work on many
# *NIX systems. See :module:`findpkgconfig`
# This will return ``QCDloop_INCLUDEDIR`` and ``QCDloop_LIBDIR`` used below.
if( QCDloop_USE_PKGCONFIG )
find_package(PkgConfig)
pkg_check_modules( QCDloop QUIET qcdloop )
if( EXISTS "${QCDloop_INCLUDEDIR}" )
get_filename_component( QCDloop_ROOT_DIR "${QCDloop_INCLUDEDIR}" DIRECTORY CACHE)
endif()
endif()
#=============================================================================
# Set QCDloop_INCLUDE_DIRS and QCDloop_LIBRARIES. If we skipped the PkgConfig step, try
# to find the libraries at $QCDloop_ROOT_DIR (if provided), in the directory
# suggested by qcdloop-config (if available), or in standard system
# locations. These find_library and find_path calls will prefer custom
# locations over standard locations (HINTS). If the requested file is found
# neither at the HINTS location nor via qcdloop-config, standard system locations
# will be still be searched (/usr/lib64 (Redhat), lib/i386-linux-gnu (Debian)).
# If we didn't use PkgConfig, try to find the version via qcdloop-config
if( NOT QCDloop_VERSION )
find_program( QCDloop_CONFIG_EXECUTABLE
NAMES qcdloop-config
HINTS "${QCDloop_ROOT_DIR}/bin"
)
if( EXISTS "${QCDloop_CONFIG_EXECUTABLE}" )
execute_process(
COMMAND "${QCDloop_CONFIG_EXECUTABLE}" --version
OUTPUT_VARIABLE QCDloop_VERSION
OUTPUT_STRIP_TRAILING_WHITESPACE )
execute_process(
COMMAND "${QCDloop_CONFIG_EXECUTABLE}" --incdir
OUTPUT_VARIABLE QCDloop_CONFIG_INCLUDEDIR
OUTPUT_STRIP_TRAILING_WHITESPACE )
execute_process(
COMMAND "${QCDloop_CONFIG_EXECUTABLE}" --libdir
OUTPUT_VARIABLE QCDloop_CONFIG_LIBDIR
OUTPUT_STRIP_TRAILING_WHITESPACE )
endif()
endif()
find_path( QCDloop_INCLUDE_DIR
NAMES qcdloop/qcdloop.h
HINTS ${QCDloop_ROOT_DIR}/include ${QCDloop_INCLUDEDIR} ${QCDloop_CONFIG_INCLUDEDIR}
)
find_library( QCDloop_LIBRARY
NAMES qcdloop
HINTS ${QCDloop_ROOT_DIR}/lib ${QCDloop_LIBDIR} ${QCDloop_CONFIG_LIBDIR}
PATH_SUFFIXES Release Debug
)
# Do we also have debug versions?
find_library( QCDloop_LIBRARY_DEBUG
NAMES qcdloop
HINTS ${QCDloop_ROOT_DIR}/lib ${QCDloop_LIBDIR} ${QCDloop_CONFIG_LIBDIR}
PATH_SUFFIXES Debug
)
set( QCDloop_INCLUDE_DIRS ${QCDloop_INCLUDE_DIR} )
set( QCDloop_LIBRARIES ${QCDloop_LIBRARY} )
if( QCDloop_VERSION )# remove "" in QCDloop version
string(REGEX REPLACE "\"" "" QCDloop_VERSION ${QCDloop_VERSION})
+ string(REPLACE "." ";" t_list ${QCDloop_VERSION})
+ list(APPEND t_list 0 0) # add a buffer in case supversion not set
+ list(GET t_list 0 QCDloop_VERSION_MAJOR)
+ list(GET t_list 1 QCDloop_VERSION_MINOR)
+ list(GET t_list 2 QCDloop_VERSION_PATCH)
endif()
#=============================================================================
# handle the QUIETLY and REQUIRED arguments and set QCDloop_FOUND to TRUE if all
# listed variables are TRUE
find_package_handle_standard_args( QCDloop
FOUND_VAR
QCDloop_FOUND
REQUIRED_VARS
QCDloop_INCLUDE_DIR
QCDloop_LIBRARY
VERSION_VAR
QCDloop_VERSION
)
mark_as_advanced( QCDloop_ROOT_DIR QCDloop_VERSION QCDloop_LIBRARY QCDloop_INCLUDE_DIR
QCDloop_LIBRARY_DEBUG QCDloop_USE_PKGCONFIG QCDloop_CONFIG )
#=============================================================================
# Register imported libraries:
# 1. If we can find a Windows .dll file (or if we can find both Debug and
# Release libraries), we will set appropriate target properties for these.
# 2. However, for most systems, we will only register the import location and
# include directory.
# Look for dlls, or Release and Debug libraries.
if(WIN32)
string( REPLACE ".lib" ".dll" QCDloop_LIBRARY_DLL "${QCDloop_LIBRARY}" )
string( REPLACE ".lib" ".dll" QCDloop_LIBRARY_DEBUG_DLL "${QCDloop_LIBRARY_DEBUG}" )
endif()
if( QCDloop_FOUND AND NOT TARGET QCDloop::qcdloop )
if( EXISTS "${QCDloop_LIBRARY_DLL}")
# Windows systems with dll libraries.
add_library( QCDloop::qcdloop SHARED IMPORTED )
add_library( QCDloop::qcdloopcblas SHARED IMPORTED )
# Windows with dlls, but only Release libraries.
set_target_properties( QCDloop::qcdloop PROPERTIES
IMPORTED_LOCATION_RELEASE "${QCDloop_LIBRARY_DLL}"
IMPORTED_IMPLIB "${QCDloop_LIBRARY}"
INTERFACE_INCLUDE_DIRECTORIES "${QCDloop_INCLUDE_DIRS}"
IMPORTED_CONFIGURATIONS Release
IMPORTED_LINK_INTERFACE_LANGUAGES "CXX"
)
# If we have both Debug and Release libraries
if( EXISTS "${QCDloop_LIBRARY_DEBUG_DLL}")
set_property( TARGET QCDloop::qcdloop APPEND PROPERTY IMPORTED_CONFIGURATIONS Debug )
set_target_properties( QCDloop::qcdloop PROPERTIES
IMPORTED_LOCATION_DEBUG "${QCDloop_LIBRARY_DEBUG_DLL}"
IMPORTED_IMPLIB_DEBUG "${QCDloop_LIBRARY_DEBUG}" )
endif()
else()
# For all other environments (ones without dll libraries), create
# the imported library targets.
add_library( QCDloop::qcdloop UNKNOWN IMPORTED )
set_target_properties( QCDloop::qcdloop PROPERTIES
IMPORTED_LOCATION "${QCDloop_LIBRARY}"
INTERFACE_INCLUDE_DIRECTORIES "${QCDloop_INCLUDE_DIRS}"
IMPORTED_LINK_INTERFACE_LANGUAGES "CXX"
)
endif()
endif()
diff --git a/cmake/Modules/Findclhep.cmake b/cmake/Modules/Findclhep.cmake
index c0f91c9..6e4943a 100644
--- a/cmake/Modules/Findclhep.cmake
+++ b/cmake/Modules/Findclhep.cmake
@@ -1,29 +1,35 @@
include (FindPackageMessage)
+include(FindPackageHandleStandardArgs)
message (STATUS "Detecting clhep installation")
execute_process (COMMAND clhep-config --prefix
OUTPUT_VARIABLE clhep_PREFIX
)
if (clhep_PREFIX)
string (REGEX REPLACE "\"\(.*\)\"[ \t\r\n]*$" "\\1" clhep_PREFIX ${clhep_PREFIX} )
message (STATUS "clhep installation found: ${clhep_PREFIX}")
EXECUTE_PROCESS(COMMAND clhep-config --libs OUTPUT_VARIABLE
CLHEP_LIBRARIES OUTPUT_STRIP_TRAILING_WHITESPACE)
- set (clhep_INCLUDE_PATH ${clhep_PREFIX}/include)
+ EXECUTE_PROCESS(COMMAND clhep-config --version OUTPUT_VARIABLE
+ clhep_VERSION OUTPUT_STRIP_TRAILING_WHITESPACE)
+ string(REGEX REPLACE "CLHEP " "" clhep_VERSION ${clhep_VERSION})
+ set (CLHEP_INCLUDE_PATH ${clhep_PREFIX}/include)
set (clhep_FOUND TRUE)
else (clhep_PREFIX)
set (clhep_FOUND FALSE)
endif (clhep_PREFIX)
-
-if (NOT clhep_FOUND)
- message(FATAL_ERROR "clhep installation not found!")
-endif (NOT clhep_FOUND)
+find_package_handle_standard_args(clhep
+ FOUND_VAR
+ clhep_FOUND
+ REQUIRED_VARS
+ CLHEP_INCLUDE_PATH
+ CLHEP_LIBRARIES
+ VERSION_VAR
+ clhep_VERSION
+ )
mark_as_advanced(
- clhep_INCLUDE_PATH
- clhep_LIBRARIES
+ CLHEP_INCLUDE_PATH
+ CLHEP_LIBRARIES
)
-
-
-
diff --git a/cmake/Modules/Findrivet.cmake b/cmake/Modules/Findrivet.cmake
index 05ab9fb..27f99b4 100644
--- a/cmake/Modules/Findrivet.cmake
+++ b/cmake/Modules/Findrivet.cmake
@@ -1,227 +1,217 @@
# Distributed under the OSI-approved BSD 3-Clause License. See accompanying
# file Copyright.txt or https://cmake.org/licensing for details.
# This is a slightly modified version of FindGSL.cmake taken from cmake 3.7
#.rst:
# Findrivet
# --------
#
# Find the native rivet includes and libraries.
#
# rivet package is an object oriented, C++ analysis tool for High Energy
# Physics Monte Carlo generators and simulation. It is free software
# under the GNU General Public License.
#
# Imported Targets
# ^^^^^^^^^^^^^^^^
#
# If rivet is found, this module defines the following
# :prop_tgt:`IMPORTED` target::
#
# rivet::rivet - The main rivet library.
#
# Result Variables
# ^^^^^^^^^^^^^^^^
#
# This module will set the following variables in your project::
#
# rivet_FOUND - True if rivet found on the local system
# rivet_INCLUDE_DIRS - Location of rivet header files.
# rivet_LIBRARIES - The rivet libraries.
# rivet_VERSION - The version of the discovered rivet install.
#
# Hints
# ^^^^^
#
# Set ``rivet_ROOT_DIR`` to a directory that contains a rivet installation.
#
# This script expects to find libraries at ``$rivet_ROOT_DIR/lib`` and the rivet
# headers at ``$rivet_ROOT_DIR/include/rivet``. The library directory may
# optionally provide Release and Debug folders. For Unix-like systems, this
# script will use ``$rivet_ROOT_DIR/bin/rivet-config`` (if found) to aid in the
# discovery rivet.
#
# Cache Variables
# ^^^^^^^^^^^^^^^
#
# This module may set the following variables depending on platform and type
# of rivet installation discovered. These variables may optionally be set to
# help this module find the correct files::
#
# rivet_CONFIG_EXECUTABLE - Location of the ``rivet-config`` script (if any).
# rivet_LIBRARY - Location of the rivet library.
# rivet_LIBRARY_DEBUG - Location of the debug rivet library (if any).
#
# Include these modules to handle the QUIETLY and REQUIRED arguments.
include(FindPackageHandleStandardArgs)
#=============================================================================
# If the user has provided ``rivet_ROOT_DIR``, use it! Choose items found
# at this location over system locations.
if( EXISTS "$ENV{rivet_ROOT_DIR}" )
file( TO_CMAKE_PATH "$ENV{rivet_ROOT_DIR}" rivet_ROOT_DIR )
set( rivet_ROOT_DIR "${rivet_ROOT_DIR}" CACHE PATH "Prefix for rivet installation." )
endif()
if( NOT EXISTS "${rivet_ROOT_DIR}" )
set( rivet_USE_PKGCONFIG ON )
endif()
#=============================================================================
# As a first try, use the PkgConfig module. This will work on many
# *NIX systems. See :module:`findpkgconfig`
# This will return ``rivet_INCLUDEDIR`` and ``rivet_LIBDIR`` used below.
if( rivet_USE_PKGCONFIG )
find_package(PkgConfig)
pkg_check_modules( rivet QUIET rivet )
if( EXISTS "${rivet_INCLUDEDIR}" )
get_filename_component( rivet_ROOT_DIR "${rivet_INCLUDEDIR}" DIRECTORY CACHE)
endif()
endif()
#=============================================================================
# Set rivet_INCLUDE_DIRS and rivet_LIBRARIES. If we skipped the PkgConfig step, try
# to find the libraries at $rivet_ROOT_DIR (if provided), in the directory
# suggested by rivet-config (if available), or in standard system
# locations. These find_library and find_path calls will prefer custom
# locations over standard locations (HINTS). If the requested file is found
# neither at the HINTS location nor via rivet-config, standard system locations
# will be still be searched (/usr/lib64 (Redhat), lib/i386-linux-gnu (Debian)).
# If we didn't use PkgConfig, try to find the version via rivet-config
if( NOT rivet_VERSION )
find_program( rivet_CONFIG_EXECUTABLE
NAMES rivet-config
HINTS "${rivet_ROOT_DIR}/bin"
)
if( EXISTS "${rivet_CONFIG_EXECUTABLE}" )
execute_process(
COMMAND "${rivet_CONFIG_EXECUTABLE}" --version
OUTPUT_VARIABLE rivet_VERSION
OUTPUT_STRIP_TRAILING_WHITESPACE )
execute_process(
COMMAND "${rivet_CONFIG_EXECUTABLE}" --includedir
OUTPUT_VARIABLE rivet_CONFIG_INCLUDEDIR
OUTPUT_STRIP_TRAILING_WHITESPACE )
execute_process(
COMMAND "${rivet_CONFIG_EXECUTABLE}" --libdir
OUTPUT_VARIABLE rivet_CONFIG_LIBDIR
OUTPUT_STRIP_TRAILING_WHITESPACE )
endif()
endif()
find_path( rivet_INCLUDE_DIR
NAMES Rivet/Rivet.hh
HINTS ${rivet_ROOT_DIR}/include ${rivet_INCLUDEDIR} ${rivet_CONFIG_INCLUDEDIR}
)
find_library( rivet_LIBRARY
NAMES Rivet
HINTS ${rivet_ROOT_DIR}/lib ${rivet_LIBDIR} ${rivet_CONFIG_LIBDIR}
PATH_SUFFIXES Release Debug
)
# Do we also have debug versions?
find_library( rivet_LIBRARY_DEBUG
NAMES Rivet
HINTS ${rivet_ROOT_DIR}/lib ${rivet_LIBDIR} ${rivet_CONFIG_LIBDIR}
PATH_SUFFIXES Debug
)
set( rivet_INCLUDE_DIRS ${rivet_INCLUDE_DIR} )
set( rivet_LIBRARIES ${rivet_LIBRARY} )
if( NOT rivet_VERSION )
if(IS_DIRECTORY ${rivet_INCLUDE_DIR})
file(STRINGS "${rivet_INCLUDE_DIR}/Rivet/Config/RivetConfig.hh" _rivet_VERS)
string(
REGEX MATCH
"#define *RIVET_VERSION *\"[^\"]*\""
_rivet_VERSION_STR "${_rivet_VERS}"
)
string(
REGEX MATCH
"[0-9]*\\.[0-9]*\\.[0-9]*"
rivet_VERSION ${_rivet_VERSION_STR}
)
endif()
endif()
if( rivet_VERSION )
- string(
- REGEX MATCH
- "^[0-9]*"
- rivet_VERSION_MAJOR ${rivet_VERSION}
- )
- string(
- REGEX REPLACE
- "^[0-9]*\\.([0-9]*)" "\\1"
- rivet_VERSION_MINOR ${rivet_VERSION}
- )
- string(
- REGEX MATCH
- "[0-9]*$"
- rivet_VERSION_PATCH ${rivet_VERSION}
- )
+ string(REPLACE "." ";" t_list ${rivet_VERSION})
+ list(APPEND t_list 0 0) # add a buffer in case supversion not set
+ list(GET t_list 0 rivet_VERSION_MAJOR)
+ list(GET t_list 1 rivet_VERSION_MINOR)
+ list(GET t_list 2 rivet_VERSION_PATCH)
endif()
#=============================================================================
# handle the QUIETLY and REQUIRED arguments and set rivet_FOUND to TRUE if all
# listed variables are TRUE
find_package_handle_standard_args( rivet
FOUND_VAR
rivet_FOUND
REQUIRED_VARS
rivet_INCLUDE_DIR
rivet_LIBRARY
VERSION_VAR
rivet_VERSION
)
mark_as_advanced( rivet_ROOT_DIR rivet_VERSION rivet_LIBRARY rivet_INCLUDE_DIR
rivet_LIBRARY_DEBUG rivet_USE_PKGCONFIG rivet_CONFIG )
#=============================================================================
# Register imported libraries:
# 1. If we can find a Windows .dll file (or if we can find both Debug and
# Release libraries), we will set appropriate target properties for these.
# 2. However, for most systems, we will only register the import location and
# include directory.
# Look for dlls, or Release and Debug libraries.
if(WIN32)
string( REPLACE ".lib" ".dll" rivet_LIBRARY_DLL "${rivet_LIBRARY}" )
string( REPLACE ".lib" ".dll" rivet_LIBRARY_DEBUG_DLL "${rivet_LIBRARY_DEBUG}" )
endif()
if( rivet_FOUND AND NOT TARGET rivet::rivet )
if( EXISTS "${rivet_LIBRARY_DLL}")
# Windows systems with dll libraries.
add_library( rivet::rivet SHARED IMPORTED )
add_library( rivet::rivetcblas SHARED IMPORTED )
# Windows with dlls, but only Release libraries.
set_target_properties( rivet::rivet PROPERTIES
IMPORTED_LOCATION_RELEASE "${rivet_LIBRARY_DLL}"
IMPORTED_IMPLIB "${rivet_LIBRARY}"
INTERFACE_INCLUDE_DIRECTORIES "${rivet_INCLUDE_DIRS}"
IMPORTED_CONFIGURATIONS Release
IMPORTED_LINK_INTERFACE_LANGUAGES "CXX"
)
# If we have both Debug and Release libraries
if( EXISTS "${rivet_LIBRARY_DEBUG_DLL}")
set_property( TARGET rivet::rivet APPEND PROPERTY IMPORTED_CONFIGURATIONS Debug )
set_target_properties( rivet::rivet PROPERTIES
IMPORTED_LOCATION_DEBUG "${rivet_LIBRARY_DEBUG_DLL}"
IMPORTED_IMPLIB_DEBUG "${rivet_LIBRARY_DEBUG}" )
endif()
else()
# For all other environments (ones without dll libraries), create
# the imported library targets.
add_library( rivet::rivet UNKNOWN IMPORTED )
set_target_properties( rivet::rivet PROPERTIES
IMPORTED_LOCATION "${rivet_LIBRARY}"
INTERFACE_INCLUDE_DIRECTORIES "${rivet_INCLUDE_DIRS}"
IMPORTED_LINK_INTERFACE_LANGUAGES "CXX"
)
endif()
endif()
diff --git a/cmake/Templates/Version.hh.in b/cmake/Templates/Version.hh.in
index 6babcbe..7e26936 100644
--- a/cmake/Templates/Version.hh.in
+++ b/cmake/Templates/Version.hh.in
@@ -1,47 +1,85 @@
/** \file Version.hh
* \brief The file gives the current HEJ Version
*/
#pragma once
#include <string>
/// @brief Full name of this package.
#define HEJ_PACKAGE_NAME "@PROJECT_NAME@"
/// @brief HEJ version string
#define HEJ_VERSION "@PROJECT_VERSION@"
/// @brief Full name and version of this package.
#define HEJ_PACKAGE_STRING "@PROJECT_NAME@ @PROJECT_VERSION@"
/// @brief Major version of this package
#define HEJ_VERSION_MAJOR @PROJECT_VERSION_MAJOR@
/// @brief Minor version of this package
#define HEJ_VERSION_MINOR @PROJECT_VERSION_MINOR@
/// @brief Patch version of this package
#define HEJ_VERSION_PATCH @PROJECT_VERSION_PATCH@
/// @brief Git revision of this package
#define HEJ_GIT_revision "@PROJECT_GIT_REVISION@"
/// @brief Git branch name of this package
#define HEJ_GIT_branch "@PROJECT_GIT_BRANCH@"
namespace HEJ {
namespace Version {
inline std::string String() { return HEJ_VERSION; }
inline std::string package_name() { return HEJ_PACKAGE_NAME; }
inline std::string package_name_full() { return HEJ_PACKAGE_STRING; }
inline int Major() { return HEJ_VERSION_MAJOR; }
inline int Minor() { return HEJ_VERSION_MINOR; }
inline int Patch() { return HEJ_VERSION_PATCH; }
inline std::string revision() { return HEJ_GIT_revision; }
+ inline std::string logo(){
+ return "\n\
+ .;l: \n \
+ .lxxddl. \n HH HH EEEEEE JJJJJJ .kkOkxdoo' \
+ \n HH HH EE JJ ;xOOOkxooodl \n HHHHHH EEEE JJ\
+ ;dx00OOkdooddxl \n HH HH EE JJ JJ cddk0OOkxolddxxx\
+ \n HH HH EEEEEE JJJJ ,dddxOOOkddllddxxx \n \
+ .,xOOkkkkOkkxddlllodxd \n .,oxkOOOkkOOOOOxxdool\
+lood: \n .... .'lxkOOOO0O00OO00000Okxdoooood \n .:odxxddxxxd\
+odkkkOOOOOOOOO00000K0KKKK0kxkkodd \n ;cdxkkkxxxkkkxxkOOOOO00OOkO0O0KKKKKKK\
+KKKK0OO' \n ;cdxxddddddddxdxkOO0OOOOOkOO00000KKKKKXKKKKK0c \n .;oddocc:\
+;;;;coxkOOOOOOOOOOOO0000KKKKXXXXXXXXKc \n cdxxdol:;...,okOOkkkkkOkOOOO00K0\
+KKXXXXXKXXXXd \n ;dkkkddl:...:dxkkkkkkOOkkOOO000KKKXXXXKKXXXK' \n .;\
+ododoc,':loxkkkOOOOOOkkOOO00000OkkOKKXXKXl \n .clol::lollodxxkkkkkOOOkk\
+OO000x'..;KXXXKKk \n ,;cldxdllllooxkkkxdkOkxkO0KKx;.,kXKKKKKk \n \
+ .;:lodolcclloddol::ldxkkOO0KK0O0KKKK000d \n .',;:loolc:::cloo' ..\
+;xkOOOO0000000KK000, \n .;;;;:clll:;,;:clodc;:;cdxkOOkOO0000000000. \n \
+ ,;;;;;::clc:;;clcloddo:codkkkkkkO00K00OO0O. \n .;:::;;;;;lc::;;::;:c\
+lc;;ldxxkkxxkO00KK0OOx \n ';::::::::::ccc:;;;;;;;;,':ldxkdllcclo0KK0Od \
+\n .;:::ccc:::cclolccc;,',,,,',:odoc,.....c0K00d \n .;:::cccc:lllloodoo\
+c:,,',,,,:ldo. .lO0O0d \n ,:::::clccolollodollcc;,,,;;;:lol;'...;oxO00\
+x \n .;:::::cllllllodooolllc:::;:;:cccloolloxkOO00d \n .;:::::clollloooo\
+oollllccccclloddxxkkOOO00O0Od \n .;;:::::cloodddddddolooooolloodxxxkkOOOOOOO\
+OOO: \n .;;;;;:::clooodddxxxdodoodoodddxxkkkkOOOOOOOOOo \n ;:;;;;;;::cllodd\
+ddddddddddddxdxxkkkkkkOOkkkkkk; \n.;::;;;;;;;:cllooooodddddddoddddkkkkkkkkkk\
+xkkkk' \n ,:::;;;,,,::ccllooodododdooooooxxxkkxxxkxkkkkx \n .;:c:;,,,,:cc\
+cclllooooloolllllloddxxxddxkkkkk: \n .;::;,,,,;cclllllooooollllllloooddooo\
+dxxkkkkd \n .',,'',;:clllloddddolllolllooooc::lddxxkxxd \n ....\
+.,:clllodddddlcclcclllc,..;lodxxxkxd \n .,:lllodddddo:;:;:cc. \
+ 'clodxxxxd \n 'cclloodddd;...... .;cloddddx. \n \
+ ,c::cloddo. .:lodxxxkc \n '::ccloddo. \
+ ,codxxkkk, \n ;cclodxxd; .codddxxxx, \n \
+ .clodddddo. ,cllcloodd'\n .clodooool; \
+ ,cl:lollo'\n :cllllcllo, ',,:c:,' \n \
+ .cclc;llc:. \n ,::,cc, \
+ "
+;
+ }
};
}
diff --git a/config.yml b/config.yml
index 9db2b9f..e289b78 100644
--- a/config.yml
+++ b/config.yml
@@ -1,91 +1,90 @@
# number of attempted resummation phase space points for each input event
trials: 10
min extparton pt: 30 # minimum transverse momentum of extremal partons
# maximum soft transverse momentum fraction in extremal jets
#
# max ext soft pt fraction: 0.1
resummation jets: # resummation jet properties
min pt: 35 # minimum jet transverse momentum
algorithm: antikt # jet clustering algorithm
R: 0.4 # jet R parameter
fixed order jets: # properties of input jets
min pt: 30
# by default, algorithm and R are like for resummation jets
# treatment of he various event classes
# the supported settings are: reweight, keep, discard
# non-HEJ events cannot be reweighted
FKL: reweight
unordered: keep
qqx: keep
non-HEJ: keep
# central scale choice or choices
#
# scales: [125, max jet pperp, H_T/2, 2*jet invariant mass, m_j1j2]
scales: 91.188
# factors by which the central scales should be multiplied
# renormalisation and factorisation scales are varied independently
#
# scale factors: [0.5, 0.7071, 1, 1.41421, 2]
# maximum ratio between renormalisation and factorisation scale
#
# max scale ratio: 2.0001
# import scale setting functions
#
# import scales:
# lib_my_scales.so: [scale0,scale1]
log correction: false # whether or not to include higher order logs
-unweight: false # TODO: whether or not to unweight events
# event output files
#
# the supported formats are
# - Les Houches (suffix .lhe)
# - HepMC (suffix .hepmc3)
# TODO: - ROOT ntuples (suffix .root)
#
# An output file's format is deduced either automatically from the suffix
# or from an explicit specification, e.g.
# - Les Houches: outfile
event output:
- HEJ.lhe
# - HEJ_events.hepmc
# to use a rivet analysis
#
# analysis:
# rivet: MC_XS # rivet analysis name
# output: HEJ # name of the yoda files, ".yoda" and scale suffix will be added
#
# to use a custom analysis
#
# analysis:
# plugin: /path/to/libmyanalysis.so
# my analysis parameter: some value
# selection of random number generator and seed
# the choices are
# - mixmax (seed is an integer)
# - ranlux64 (seed is a filename containing parameters)
random generator:
name: mixmax
# seed: 1
# parameters for Higgs-gluon couplings
# this requires compilation with qcdloop
#
# Higgs coupling:
# use impact factors: false
# mt: 174
# include bottom: true
# mb: 4.7
diff --git a/doc/developer_manual/developer_manual.tex b/doc/developer_manual/developer_manual.tex
index 76c7670..4ad120b 100644
--- a/doc/developer_manual/developer_manual.tex
+++ b/doc/developer_manual/developer_manual.tex
@@ -1,1168 +1,1382 @@
\documentclass[a4paper,11pt]{article}
\usepackage{fourier}
\usepackage[T1]{fontenc}
\usepackage{microtype}
\usepackage{geometry}
\usepackage{enumitem}
\setlist[description]{leftmargin=\parindent,labelindent=\parindent}
\usepackage{amsmath}
\usepackage{amssymb}
\usepackage[utf8x]{inputenc}
\usepackage{graphicx}
\usepackage{xcolor}
\usepackage{todonotes}
\usepackage{listings}
\usepackage{xspace}
\usepackage{tikz}
\usetikzlibrary{arrows.meta}
\usetikzlibrary{shapes}
\usetikzlibrary{calc}
\usepackage[colorlinks,linkcolor={blue!50!black}]{hyperref}
\graphicspath{{build/figures/}{figures/}}
\emergencystretch \hsize
\newcommand{\HEJ}{{\tt HEJ}\xspace}
\newcommand{\HIGHEJ}{\emph{High Energy Jets}\xspace}
\newcommand{\cmake}{\href{https://cmake.org/}{cmake}\xspace}
\newcommand{\html}{\href{https://www.w3.org/html/}{html}\xspace}
\newcommand{\YAML}{\href{http://yaml.org/}{YAML}\xspace}
\newcommand{\QCDloop}{\href{https://github.com/scarrazza/qcdloop}{QCDloop}\xspace}
\newcommand{\as}{\alpha_s}
\DeclareRobustCommand{\mathgraphics}[1]{\vcenter{\hbox{\includegraphics{#1}}}}
\def\spa#1.#2{\left\langle#1\,#2\right\rangle}
\def\spb#1.#2{\left[#1\,#2\right]} \def\spaa#1.#2.#3{\langle\mskip-1mu{#1} |
#2 | {#3}\mskip-1mu\rangle} \def\spbb#1.#2.#3{[\mskip-1mu{#1} | #2 |
{#3}\mskip-1mu]} \def\spab#1.#2.#3{\langle\mskip-1mu{#1} | #2 |
{#3}\mskip-1mu\rangle} \def\spba#1.#2.#3{\langle\mskip-1mu{#1}^+ | #2 |
{#3}^+\mskip-1mu\rangle} \def\spav#1.#2.#3{\|\mskip-1mu{#1} | #2 |
{#3}\mskip-1mu\|^2} \def\jc#1.#2.#3{j^{#1}_{#2#3}}
\definecolor{darkgreen}{rgb}{0,0.4,0}
\lstset{ %
backgroundcolor=\color{lightgray}, % choose the background color; you must add \usepackage{color} or \usepackage{xcolor}
basicstyle=\footnotesize\usefont{T1}{DejaVuSansMono-TLF}{m}{n}, % the size of the fonts that are used for the code
breakatwhitespace=false, % sets if automatic breaks should only happen at whitespace
breaklines=false, % sets automatic line breaking
captionpos=t, % sets the caption-position to bottom
commentstyle=\color{red}, % comment style
deletekeywords={...}, % if you want to delete keywords from the given language
escapeinside={\%*}{*)}, % if you want to add LaTeX within your code
extendedchars=true, % lets you use non-ASCII characters; for 8-bits encodings only, does not work with UTF-8
frame=false, % adds a frame around the code
keepspaces=true, % keeps spaces in text, useful for keeping indentation of code (possibly needs columns=flexible)
keywordstyle=\color{blue}, % keyword style
otherkeywords={}, % if you want to add more keywords to the set
numbers=none, % where to put the line-numbers; possible values are (none, left, right)
numbersep=5pt, % how far the line-numbers are from the code
rulecolor=\color{black}, % if not set, the frame-color may be changed on line-breaks within not-black text (e.g. comments (green here))
showspaces=false, % show spaces everywhere adding particular underscores; it overrides 'showstringspaces'
showstringspaces=false, % underline spaces within strings only
showtabs=false, % show tabs within strings adding particular underscores
stepnumber=2, % the step between two line-numbers. If it's 1, each line will be numbered
stringstyle=\color{gray}, % string literal style
tabsize=2, % sets default tabsize to 2 spaces
title=\lstname,
emph={},
emphstyle=\color{darkgreen}
}
\begin{document}
\tikzstyle{mynode}=[rectangle split,rectangle split parts=2, draw,rectangle split part fill={lightgray, none}]
\title{HEJ 2 developer manual}
\author{}
\maketitle
\tableofcontents
\newpage
\section{Overview}
\label{sec:overview}
HEJ 2 is a C++ program and library implementing an algorithm to
apply \HIGHEJ resummation~\cite{Andersen:2008ue,Andersen:2008gc} to
pre-generated fixed-order events. This document is intended to give an
overview over the concepts and structure of this implementation.
\subsection{Project structure}
\label{sec:project}
HEJ 2 is developed under the \href{https://git-scm.com/}{git}
version control system. The main repository is on the IPPP
\href{https://gitlab.com/}{gitlab} server under
\url{https://gitlab.dur.scotgrid.ac.uk/hej/hej}. To get a local
copy, get an account on the gitlab server and use
\begin{lstlisting}[language=sh,caption={}]
git clone git@gitlab.dur.scotgrid.ac.uk:hej/hej.git
\end{lstlisting}
This should create a directory \texttt{hej} with the following
contents:
\begin{description}
\item[doc:] Contains additional documentation, see section~\ref{sec:doc}.
\item[include:] Contains the C++ header files.
\item[src:] Contains the C++ source files.
\item[t:] Contains the source code for the automated tests.
\item[CMakeLists.txt:] Configuration file for the \cmake build
system. See section~\ref{sec:cmake}.
\item[cmake:] Auxiliary files for \cmake. This includes modules for
finding installed software in \texttt{cmake/Modules} and templates for
code generation during the build process in \texttt{cmake/Templates}.
\item[config.yml:] Sample configuration file for running HEJ 2.
\item[events.lhe:] Fixed-order event sample that can be used as input
for HEJ 2.
\item[FixedOrderGen:] Contains the code for the fixed-order generator,
see section~\ref{sec:HEJFOG}.
\end{description}
In the following all paths are given relative to the
\texttt{hej} directory.
\subsection{Documentation}
\label{sec:doc}
The \texttt{doc} directory contains user documentation in
\texttt{doc/sphinx} and the configuration to generate source code
documentation in \texttt{doc/doxygen}.
The user documentation explains how to install and run HEJ 2. The
format is
\href{http://docutils.sourceforge.net/rst.html}{reStructuredText}, which
is mostly human-readable. Other formats, like \html, can be generated with the
\href{http://www.sphinx-doc.org/en/master/}{sphinx} generator with
\begin{lstlisting}[language=sh,caption={}]
make html
\end{lstlisting}
To document the source code we use
\href{https://www.stack.nl/~dimitri/doxygen/}{doxygen}. To generate
\html documentation, use the command
\begin{lstlisting}[language=sh,caption={}]
doxygen Doxyfile
\end{lstlisting}
in the \texttt{doc/doxygen} directory.
\subsection{Build system}
\label{sec:cmake}
For the most part, HEJ 2 is a library providing classes and
functions that can be used to add resummation to fixed-order events. In
addition, there is a relatively small executable program leveraging this
library to read in events from an input file and produce resummation
events. Both the library and the program are built and installed with
the help of \cmake.
Debug information can be turned on by using
\begin{lstlisting}[language=sh,caption={}]
cmake base/directory -DCMAKE_BUILD_TYPE=Debug
make install
\end{lstlisting}
This facilitates the use of debuggers like \href{https://www.gnu.org/software/gdb/}{gdb}.
The main \cmake configuration file is \texttt{CMakeLists.txt}. It defines the
compiler flags, software prerequisites, header and source files used to
build HEJ 2, and the automated tests.
\texttt{cmake/Modules} contains module files that help with the
detection of the software prerequisites and \texttt{cmake/Templates}
template files for the automatic generation of header and
source files. For example, this allows to only keep the version
information in one central location (\texttt{CMakeLists.txt}) and
automatically generate a header file from the template \texttt{Version.hh.in} to propagate this to the C++ code.
\subsection{General coding guidelines}
\label{sec:notes}
The goal is to make the HEJ 2 code well-structured and
readable. Here are a number of guidelines to this end.
\begin{description}
\item[Observe the boy scout rule.] Always leave the code cleaner
than how you found it. Ugly hacks can be useful for testing, but
shouldn't make their way into the main branch.
\item[Ask if something is unclear.] Often there is a good reason why
code is written the way it is. Sometimes that reason is only obvious to
the original author (use \lstinline!git blame! to find them), in which
case they should be poked to add a comment. Sometimes there is no good
reason, but nobody has had the time to come up with something better,
yet. In some places the code might just be bad.
\item[Don't break tests.] There are a number of tests in the \texttt{t}
directory, which can be run with \lstinline!make test!. Ideally, all
tests should run successfully in each git revision. If your latest
commit broke a test and you haven't pushed to the central repository
yet, you can fix it with \lstinline!git commit --amend!. If an earlier
local commit broke a test, you can use \lstinline!git rebase -i! if
you feel confident.
\item[Test your new code.] When you add some new functionality, also add an
automated test. This can be useful even if you don't know the
``correct'' result because it prevents the code from changing its behaviour
silently in the future. \href{http://www.valgrind.org/}{valgrind} is a
very useful tool to detect potential memory leaks.
\item[Stick to the coding style.] It is somewhat easier to read code
that has a uniform coding and indentation style. We don't have a
strict style, but it helps if your code looks similar to what is
already there.
\end{description}
\section{Program flow}
\label{sec:flow}
A run of the HEJ 2 program has three stages: initialisation,
event processing, and cleanup. The following sections outline these
stages and their relations to the various classes and functions in the
code. Unless denoted otherwise, all classes and functions are part of
the \lstinline!HEJ! namespace. The code for the HEJ 2 program is
in \texttt{src/main.cc}, all other code comprises the HEJ 2
library. Classes and free functions are usually implemented in header
and source files with a corresponding name, i.e. the code for
\lstinline!MyClass! can usually be found in
\texttt{include/HEJ/MyClass.hh} and \texttt{src/MyClass.cc}.
\subsection{Initialisation}
\label{sec:init}
The first step is to load and parse the \YAML configuration file. The
entry point for this is the \lstinline!load_config! function and the
related code can be found in \texttt{include/HEJ/YAMLreader.hh},
\texttt{include/HEJ/config.hh} and the corresponding \texttt{.cc} files
in the \texttt{src} directory. The implementation is based on the
\href{https://github.com/jbeder/yaml-cpp}{yaml-cpp} library.
The \lstinline!load_config! function returns a \lstinline!Config! object
containing all settings. To detect potential mistakes as early as
possible, we throw an exception whenever one of the following errors
occurs:
\begin{itemize}
\item There is an unknown option in the \YAML file.
\item A setting is invalid, for example a string is given where a number
would be expected.
\item An option value is not set.
\end{itemize}
The third rule is sometimes relaxed for ``advanced'' settings with an
obvious default, like for importing custom scales or analyses.
The information stored in the \lstinline!Config! object is then used to
initialise various objects required for the event processing stage
described in section~\ref{sec:processing}. First, the
\lstinline!get_analysis! function creates an object that inherits from
the \lstinline!Analysis! interface.\footnote{In the context of C++ the
proper technical expression is ``pure abstract class''.} Using an
interface allows us to decide the concrete type of the analysis at run
time instead of having to make a compile-time decision. Depending on the
settings, \lstinline!get_analysis! creates either a user-defined
analysis loaded from an external library (see the user documentation
-\todo{link}) or the default \lstinline!EmptyAnalysis!, which does
+\url{https://hej.web.cern.ch/HEJ/doc/current/user/}) or the default \lstinline!EmptyAnalysis!, which does
nothing.
Together with a number of further objects, whose roles are described in
section~\ref{sec:processing}, we also initialise the global random
number generator. We again use an interface to defer deciding the
concrete type until the program is actually run. Currently, we support the
\href{https://mixmax.hepforge.org/}{MIXMAX}
(\texttt{include/HEJ/Mixmax.hh}) and Ranlux64
(\texttt{include/HEJ/Ranlux64.hh}) random number generators, both are provided
by \href{http://proj-clhep.web.cern.ch/}{CLHEP}.
We also set up a \lstinline!LHEF::Reader! object (see
\href{http://home.thep.lu.se/~leif/LHEF/}{\texttt{include/LHEF/LHEF.h}}) for
reading events from a file in the Les
Houches event file format~\cite{Alwall:2006yp}. A small wrapper around
the
\href{https://www.boost.org/doc/libs/1_67_0/libs/iostreams/doc/index.html}{boost
iostreams} library allows us to also read event files compressed with
\href{https://www.gnu.org/software/gzip/}{gzip}. The wrapper code is in
\texttt{include/HEJ/stream.hh} and the \texttt{src/stream.cc}.
\subsection{Event processing}
\label{sec:processing}
In the second stage events are continously read from the event
file. After jet clustering, a number of corresponding resummation events
are generated for each input event and fed into the analysis and a
number of output files. The roles of various classes and functions are
illustrated in the following flow chart:
\begin{center}
\begin{tikzpicture}[node distance=2cm and 5mm]
\node (reader) [mynode]
{\lstinline!LHEF::Reader::readEvent!\nodepart{second}{read event}};
\node
(cluster) [mynode,below=of reader]
{\lstinline!Event! constructor\nodepart{second}{cluster jets}};
\node
(resum) [mynode,below=of cluster]
{\lstinline!EventReweighter::reweight!\nodepart{second}{perform resummation}};
\node
(cut) [mynode,below=of resum]
{\lstinline!Analysis::pass_cuts!\nodepart{second}{apply cuts}};
\node
(fill) [mynode,below left=of cut]
{\lstinline!Analysis::fill!\nodepart{second}{analyse event}};
\node
(write) [mynode,below right=of cut]
{\lstinline!CombinedEventWriter::write!\nodepart{second}{write out event}};
\node
(control) [below=of cut] {};
\draw[-{Latex[length=3mm, width=1.5mm]}]
(reader.south) -- node[left] {\lstinline!LHEF::HEPEUP!} (cluster.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
(cluster.south) -- node[left] {\lstinline!Event!} (resum.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
(resum.south) -- (cut.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(resum.south)+(7mm, 0cm)$) -- ($(cut.north)+(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(resum.south)-(7mm, 0cm)$) -- node[left] {\lstinline!Event!} ($(cut.north)-(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(cut.south)-(3mm,0mm)$) .. controls ($(control)-(3mm,0mm)$) ..node[left] {\lstinline!Event!} (fill.east);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(cut.south)-(3mm,0mm)$) .. controls ($(control)-(3mm,0mm)$) .. (write.west);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(cut.south)+(3mm,0mm)$) .. controls ($(control)+(3mm,0mm)$) .. (fill.east);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(cut.south)+(3mm,0mm)$) .. controls ($(control)+(3mm,0mm)$) ..node[right] {\lstinline!Event!} (write.west);
\end{tikzpicture}
\end{center}
The resummation is performed by the \lstinline!EventReweighter! class,
which is described in more detail in section~\ref{sec:resum}. The
\lstinline!CombinedEventWriter! writes events to zero or more output
files. To this end, it contains a number of objects implementing the
\lstinline!EventWriter! interface. These event writers typically write
the events to a file in a given format. We currently have the
\lstinline!LesHouchesWriter! for event files in the Les Houches Event
File format and the \lstinline!HepMCWriter! for the
\href{https://hepmc.web.cern.ch/hepmc/}{HepMC} format (Version 2 and 3).
\subsection{Resummation}
\label{sec:resum}
In the \lstinline!EventReweighter::reweight! member function, we first
classify the input fixed-order event (FKL, unordered, non-HEJ, \dots)
and decide according to the user settings whether to discard, keep, or
resum the event. If we perform resummation for the given event, we
generate a number of trial \lstinline!PhaseSpacePoint! objects. Phase
space generation is discussed in more detail in
section~\ref{sec:pspgen}. We then perform jet clustering according to
the settings for the resummation jets on each
\lstinline!PhaseSpacePoint!, update the factorisation and
renormalisation scale in the resulting \lstinline!Event! and reweight it
according to the ratio of pdf factors and \HEJ matrix elements between
resummation and original fixed-order event:
\begin{center}
\begin{tikzpicture}[node distance=2cm and 5mm]
\node (in) {};
\node (treat) [diamond,draw,below=of in,minimum size=3.5cm,
label={[anchor=west, inner sep=8pt]west:discard},
label={[anchor=east, inner sep=14pt]east:keep},
label={[anchor=south, inner sep=20pt]south:reweight}
] {};
\draw (treat.north west) -- (treat.south east);
\draw (treat.north east) -- (treat.south west);
\node
(psp) [mynode,below=of treat]
{\lstinline!PhaseSpacePoint! constructor};
\node
(cluster) [mynode,below=of psp]
{\lstinline!Event! constructor\nodepart{second}{cluster jets}};
\node
(gen_scales) [mynode,below=of cluster]
{\lstinline!ScaleGenerator::operator()!\nodepart{second}{update scales}};
\node
(rescale) [mynode,below=of gen_scales]
{\lstinline!PDF::pdfpt!,
\lstinline!MatrixElement!\nodepart{second}{reweight}};
\node (out) [below of=rescale] {};
\draw[-{Latex[length=3mm, width=1.5mm]}]
(in.south) -- node[left] {\lstinline!Event!} (treat.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
(treat.south) -- node[left] {\lstinline!Event!} (psp.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
(psp.south) -- (cluster.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(psp.south)+(7mm, 0cm)$) -- ($(cluster.north)+(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(psp.south)-(7mm, 0cm)$) -- node[left]
{\lstinline!PhaseSpacePoint!} ($(cluster.north)-(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
(cluster.south) -- (gen_scales.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(cluster.south)+(7mm, 0cm)$) -- ($(gen_scales.north)+(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(cluster.south)-(7mm, 0cm)$) -- node[left]
{\lstinline!Event!} ($(gen_scales.north)-(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
(gen_scales.south) -- (rescale.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(gen_scales.south)+(7mm, 0cm)$) -- ($(rescale.north)+(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(gen_scales.south)-(7mm, 0cm)$) -- node[left]
{\lstinline!Event!} ($(rescale.north)-(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
(rescale.south) -- (out.north);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(rescale.south)+(7mm, 0cm)$) -- ($(out.north)+(7mm, 0cm)$);
\draw[-{Latex[length=3mm, width=1.5mm]}]
($(rescale.south)-(7mm, 0cm)$) -- node[left]
{\lstinline!Event!} ($(out.north)-(7mm, 0cm)$);
\node (helper) at ($(treat.east) + (15mm,0cm)$) {};
\draw[-{Latex[length=3mm, width=1.5mm]}]
(treat.east) -- ($(treat.east) + (15mm,0cm)$)
-- node[left] {\lstinline!Event!} (helper |- gen_scales.east) -- (gen_scales.east)
;
\end{tikzpicture}
\end{center}
\subsection{Phase space point generation}
\label{sec:pspgen}
The resummed and matched \HEJ cross section for pure jet production of
FKL configurations is given by (cf. eq. (3) of~\cite{Andersen:2018tnm})
\begin{align}
\label{eq:resumdijetFKLmatched2}
% \begin{split}
\sigma&_{2j}^\mathrm{resum, match}=\sum_{f_1, f_2}\ \sum_m
\prod_{j=1}^m\left(
\int_{p_{j\perp}^B=0}^{p_{j\perp}^B=\infty}
\frac{\mathrm{d}^2\mathbf{p}_{j\perp}^B}{(2\pi)^3}\ \int
\frac{\mathrm{d} y_j^B}{2} \right) \
(2\pi)^4\ \delta^{(2)}\!\!\left(\sum_{k=1}^{m}
\mathbf{p}_{k\perp}^B\right)\nonumber\\
&\times\ x_a^B\ f_{a, f_1}(x_a^B, Q_a^B)\ x_b^B\ f_{b, f_2}(x_b^B, Q_b^B)\
\frac{\overline{\left|\mathcal{M}_\text{LO}^{f_1f_2\to f_1g\cdots
gf_2}\big(\big\{p^B_j\big\}\big)\right|}^2}{(\hat {s}^B)^2}\nonumber\\
& \times (2\pi)^{-4+3m}\ 2^m \nonumber\\
&\times\ \sum_{n=2}^\infty\
\int_{p_{1\perp}=p_{\perp,\mathrm{min}} }^{p_{1\perp}=\infty}
\frac{\mathrm{d}^2\mathbf{p}_{1\perp}}{(2\pi)^3}\
\int_{p_{n\perp}=p_{\perp,\mathrm{min}}}^{p_{n\perp}=\infty}
\frac{\mathrm{d}^2\mathbf{p}_{n\perp}}{(2\pi)^3}\
\prod_{i=2}^{n-1}\int_{p_{i\perp}=\lambda}^{p_{i\perp}=\infty}
\frac{\mathrm{d}^2\mathbf{p}_{i\perp}}{(2\pi)^3}\ (2\pi)^4\ \delta^{(2)}\!\!\left(\sum_{k=1}^n
\mathbf{p}_{k\perp}\right )\\
&\times \ \mathbf{T}_y \prod_{i=1}^n
\left(\int \frac{\mathrm{d} y_i}{2}\right)\
\mathcal{O}_{mj}^e\
\left(\prod_{l=1}^{m-1}\delta^{(2)}(\mathbf{p}_{\mathcal{J}_{l}\perp}^B -
\mathbf{j}_{l\perp})\right)\
\left(\prod_{l=1}^m\delta(y^B_{\mathcal{J}_l}-y_{\mathcal{J}_l})\right)
\ \mathcal{O}_{2j}(\{p_i\})\nonumber\\
&\times \frac{(\hat{s}^B)^2}{\hat{s}^2}\ \frac{x_a f_{a,f_1}(x_a, Q_a)\ x_b f_{b,f_2}(x_b, Q_b)}{x_a^B\ f_{a,f_1}(x_a^B, Q_a^B)\ x_b^B\ f_{b,f_2}(x_b^B, Q_b^B)}\ \frac{\overline{\left|\mathcal{M}_{\mathrm{HEJ}}^{f_1 f_2\to f_1 g\cdots
gf_2}(\{ p_i\})\right|}^2}{\overline{\left|\mathcal{M}_\text{LO, HEJ}^{f_1f_2\to f_1g\cdots
gf_2}\big(\big\{p^B_j\big\}\big)\right|}^{2}} \,.\nonumber
% \end{split}
\end{align}
The first two lines correspond to the generation of the fixed-order
input events with incoming partons $f_1, f_2$ and outgoing momenta
$p_j^B$, where $\mathbf{p}_{j\perp}^B$ and $y_j^B$ denote the respective
transverse momentum and rapidity. Note that, at leading order, these
coincide with the fixed-order jet momenta $p_{\mathcal{J}_j}^B$.
$f_{a,f_1}(x_a, Q_a),f_{b,f_2}(x_b, Q_b)$ are the pdf factors for the incoming partons with
momentum fractions $x_a$ and $x_b$. The square of the partonic
centre-of-mass energy is denoted by $\hat{s}^B$ and
$\mathcal{M}_\text{LO}^{f_1f_2\to f_1g\cdots gf_2}$ is the
leading-order matrix element.
The third line is a factor accounting for the different multiplicities
between fixed-order and resummation events. Lines four and five are
the integration over the resummation phase space described in this
section. $p_i$ are the momenta of the outgoing partons in resummation
phase space. $\mathbf{T}_y$ denotes rapidity
ordering and $\mathcal{O}_{mj}^e$ projects out the exclusive $m$-jet
component. The relation between resummation and fixed-order momenta is
fixed by the $\delta$ functions. The first sets each transverse fixed-order jet
momentum to some function $\mathbf{j_{l\perp}}$ of the resummation
momenta. The exact form is described in section~\ref{sec:ptj_res}. The second
$\delta$ forces the rapidities of resummation and fixed-order jets to be
the same. Finally, the last line is the reweighting of pdf and matrix
element factors already shown in section~\ref{sec:resum}.
There are two kinds of cut-off in the integration over the resummation
partons. $\lambda$ is a technical cut-off connected to the cancellation
of infrared divergencies between real and virtual corrections. Its
numerical value is set in
\texttt{include/HEJ/Constants.h}. $p_{\perp,\mathrm{min}}$ regulates
and \emph{uncancelled} divergence in the extremal parton momenta. Its
-size is set by the user configuration \todo{link}.
+size is set by the user configuration \url{https://hej.web.cern.ch/HEJ/doc/current/user/HEJ.html#settings}.
It is straightforward to generalise eq.~(\ref{eq:resumdijetFKLmatched2})
to unordered configurations and processes with additional colourless
emissions, for example a Higgs or electroweak boson. In the latter case only
the fixed-order integration and the matrix elements change.
\subsubsection{Gluon Multiplicity}
\label{sec:psp_ng}
The first step in evaluating the resummation phase space in
eq.~(\ref{eq:resumdijetFKLmatched2}) is to randomly pick terms in the
sum over the number of emissions. This sampling of the gluon
multiplicity is done in the \lstinline!PhaseSpacePoint::sample_ng!
function in \texttt{src/PhaseSpacePoint.cc}.
The typical number of extra emissions depends strongly on the rapidity
span of the underlying fixed-order event. Let us, for example, consider
a fixed-order FKL-type multi-jet configuration with rapidities
$y_{j_f},\,y_{j_b}$ of the most forward and backward jets,
respectively. By eq.~(\ref{eq:resumdijetFKLmatched2}), the jet
multiplicity and the rapidity of each jet are conserved when adding
resummation. This implies that additional hard radiation is restricted
to rapidities $y$ within a region $y_{j_b} \lesssim y \lesssim
y_{j_f}$. Within \HEJ, we require the most forward and most backward
emissions to be hard \todo{specify how hard} in order to avoid divergences, so this constraint
in fact applies to \emph{all} additional radiation.
To simplify the remaining discussion, let us remove the FKL rapidity
ordering
\begin{equation}
\label{eq:remove_y_order}
\mathbf{T}_y \prod_{i=1}^n\int \frac{\mathrm{d}y_i}{2} =
\frac{1}{n!}\prod_{i=1}^n\int
\frac{\mathrm{d}y_i}{2}\,,
\end{equation}
where all rapidity integrals now cover a region which is approximately
bounded by $y_{j_b}$ and $y_{j_f}$. Each of the $m$ jets has to contain at least
one parton; selecting random emissions we can rewrite the phase space
integrals as
\begin{equation}
\label{eq:select_jets}
\frac{1}{n!}\prod_{i=1}^n\int [\mathrm{d}p_i] =
\left(\prod_{i=1}^{m}\int [\mathrm{d}p_i]\ {\cal J}_i(p_i)\right)
\frac{1}{n_g!}\prod_{i=m+1}^{m+n_g}\int [\mathrm{d}p_i]
\end{equation}
with jet selection functions
\begin{equation}
\label{eq:def_jet_selection}
{\cal J}_i(p) =
\begin{cases}
1 &p\text{ clustered into jet }i\\
0 & \text{otherwise}
\end{cases}
\end{equation}
and $n_g \equiv n - m$. Here and in the following we use the short-hand
notation $[\mathrm{d}p_i]$ to denote the phase-space measure for parton
$i$. As is evident from eq.~\eqref{eq:select_jets}, adding an extra emission
$n_g+1$ introduces a suppression factor $\tfrac{1}{n_g+1}$. However, the
additional phase space integral also results in an enhancement proportional
to $\Delta y_{j_f j_b} = y_{j_f} - y_{j_b}$. This is a result of the
rapidity-independence of the MRK limit of the integrand, consisting of the
matrix elements divided by the flux factor. Indeed, we observe that the
typical number of gluon emissions is to a good approximation proportional to
the rapidity separation and the phase space integral is dominated by events
with $n_g \approx \Delta y_{j_f j_b}$.
For the actual phase space sampling, we assume a Poisson distribution
and extract the mean number of gluon emissions in different rapidity
bins and fit the results to a linear function in $\Delta y_{j_f j_b}$,
finding a coefficient of $0.975$ for the inclusive production of a Higgs
boson with two jets. Here are the observed and fitted average gluon
multiplicities as a function of $\Delta y_{j_f j_b}$:
\begin{center}
\includegraphics[width=.75\textwidth]{ng_mean}
\end{center}
As shown for two rapidity slices the assumption of a Poisson
distribution is also a good approximation:
\begin{center}
\includegraphics[width=.49\textwidth]{{ng_1.5}.pdf}\hfill
\includegraphics[width=.49\textwidth]{{ng_5.5}.pdf}
\end{center}
\subsubsection{Number of Gluons inside Jets}
\label{sec:psp_ng_jet}
For each of the $n_g$ gluon emissions we can split the phase-space
integral into a (disconnected) region inside the jets and a remainder:
\begin{equation}
\label{eq:psp_split}
\int [\mathrm{d}p_i] = \int [\mathrm{d}p_i]\,
\theta\bigg(\sum_{j=1}^{m}{\cal J}_j(p_i)\bigg) + \int [\mathrm{d}p_i]\,
\bigg[1-\theta\bigg(\sum_{j=1}^{m}{\cal J}_j(p_i)\bigg)\bigg]\,.
\end{equation}
The next step is to decide how many of the gluons will form part of a
jet. This is done in the \lstinline!PhaseSpacePoint::sample_ng_jets!
function.
We choose an importance sampling which is flat in the plane
spanned by the azimuthal angle $\phi$ and the rapidity $y$. This is
observed in BFKL and valid in the limit of Multi-Regge-Kinematics
(MRK). Furthermore, we assume anti-$k_t$ jets, which cover an area of
$\pi R^2$.
In principle, the total accessible area in the $y$-$\phi$ plane is given
by $2\pi \Delta y_{fb}$, where $\Delta y_{fb}\geq \Delta y_{j_f j_b}$ is
the a priori unknown rapidity separation between the most forward and
backward partons. In most cases the extremal jets consist of single
partons, so that $\Delta y_{fb} = \Delta y_{j_f j_b}$. For the less common
case of two partons forming a jet we observe a maximum distance of $R$
between the constituents and the jet centre. In rare cases jets have
more than two constituents. Empirically, they are always within a
distance of $\tfrac{5}{3}R$ to the centre of the jet, so
$\Delta y_{fb} \leq \Delta y_{j_f j_b} + \tfrac{10}{3} R$. In practice, the
extremal partons are required to carry a large fraction of the jet
transverse momentum and will therefore be much closer to the jet axis.
In summary, for sufficiently large rapidity separations we can use the
approximation $\Delta y_{fb} \approx \Delta y_{j_f j_b}$. This scenario
is depicted here:
\begin{center}
\includegraphics[width=0.5\linewidth]{ps_large_y}
\end{center}
If there is no overlap between jets, the probability $p_{\cal J, >}$ for
an extra gluon to end up inside a jet is then given by
\begin{equation}
\label{eq:p_J_large}
p_{\cal J, >} = \frac{(m - 1)\*R^2}{2\Delta y_{j_f j_b}}\,.
\end{equation}
For a very small rapidity separation, eq.~\eqref{eq:p_J_large}
obviously overestimates the true probability. The maximum phase space
covered by jets in the limit of a vanishing rapidity distance between
all partons is $2mR \Delta y_{fb}$:
\begin{center}
\includegraphics[width=0.5\linewidth]{ps_small_y}
\end{center}
We therefore estimate the probability for a parton to end up inside a jet as
\begin{equation}
\label{eq:p_J}
p_{\cal J} = \min\bigg(\frac{(m - 1)\*R^2}{2\Delta y_{j_f j_b}}, \frac{mR}{\pi}\bigg)\,.
\end{equation}
Here we compare this estimate with the actually observed
fraction of additional emissions into jets as a function of the rapidity
separation:
\begin{center}
\includegraphics[width=0.75\linewidth]{pJ}
\end{center}
\subsubsection{Gluons outside Jets}
\label{sec:gluons_nonjet}
Using our estimate for the probability of a gluon to be a jet
constituent, we choose a number $n_{g,{\cal J}}$ of gluons inside
jets, which also fixes the number $n_g - n_{g,{\cal J}}$ of gluons
outside jets. As explained later on, we need to generate the momenta of
the gluons outside jets first. This is done in
\lstinline!PhaseSpacePoint::gen_non_jet!.
The azimuthal angle $\phi$ is generated flat within $0\leq \phi \leq 2
\pi$. The allowed rapidity interval is set by the most forward and
backward partons, which are necessarily inside jets. Since these parton
rapidities are not known at this point, we also have to postpone the
rapidity generation for the gluons outside jets. For the scalar
transverse momentum $p_\perp = |\mathbf{p}_\perp|$ of a gluon outside
jets we use the parametrisation
\begin{equation}
\label{eq:p_nonjet}
p_\perp = \lambda + \tilde{p}_\perp\*\tan(\tau\*r)\,, \qquad
\tau = \arctan\bigg(\frac{p_{\perp{\cal J}_\text{min}} - \lambda}{\tilde{p}_\perp}\bigg)\,.
\end{equation}
For $r \in [0,1)$, $p_\perp$ is always less than the minimum momentum
$p_{\perp{\cal J}_\text{min}}$ required for a jet. $\tilde{p}_\perp$ is
a free parameter, a good empirical value is $\tilde{p}_\perp = [1.3 +
0.2\*(n_g - n_{g,\cal J})]\,$GeV
\subsubsection{Resummation jet momenta}
\label{sec:ptj_res}
On the one hand, each jet momentum is given by the sum of its
constituent momenta. On the other hand, the resummation jet momenta are
fixed by the constraints in line five of the master
equation~\eqref{eq:resumdijetFKLmatched2}. We therefore have to
calculate the resummation jet momenta from these constraints before
generating the momenta of the gluons inside jets. This is done in
\lstinline!PhaseSpacePoint::reshuffle! and in the free
\lstinline!resummation_jet_momenta! function (declared in \texttt{resummation\_jet.hh}).
The resummation jet momenta are determined by the $\delta$ functions in
line five of eq.~(\ref{eq:resumdijetFKLmatched2}). The rapidities are
fixed to the rapidities of the jets in the input fixed-order events, so
that the FKL ordering is guaranteed to be preserved.
In traditional \HEJ reshuffling the transverse momentum are given through
\begin{equation}
\label{eq:ptreassign_old}
\mathbf{p}^B_{\mathcal{J}_{l\perp}} = \mathbf{j}_{l\perp} \equiv \mathbf{p}_{\mathcal{J}_{l}\perp}
+ \mathbf{q}_\perp \,\frac{|\mathbf{p}_{\mathcal{J}_{l}\perp}|}{P_\perp},
\end{equation}
where $\mathbf{q}_\perp = \sum_{j=1}^n \mathbf{p}_{i\perp}
\bigg[1-\theta\bigg(\sum_{j=1}^{m}{\cal J}_j(p_i)\bigg)\bigg] $ is the
total transverse momentum of all partons \emph{outside} jets and
$P_\perp = \sum_{j=1}^m |\mathbf{p}_{\mathcal{J}_{j}\perp}|$. Since the
total transverse momentum of an event vanishes, we can also use
$\mathbf{q}_\perp = - \sum_{j=1}^m
\mathbf{p}_{\mathcal{J}_{j}\perp}$. Eq.~(\ref{eq:ptreassign}) is a
non-linear system of equations in the resummation jet momenta
$\mathbf{p}_{\mathcal{J}_{l}\perp}$. Hence we would have to solve
\begin{equation}
\label{eq:ptreassign_eq}
\mathbf{p}_{\mathcal{J}_{l}\perp}=\mathbf{j}^B_{l\perp} \equiv\mathbf{j}_{l\perp}^{-1}
\left(\mathbf{p}^B_{\mathcal{J}_{l\perp}}\right)
\end{equation}
numerically.
Since solving such a system is computationally expensive, we instead
change the reshuffling around to be linear in the resummation jet
momenta. Hence~\eqref{eq:ptreassign_eq} gets replaces by
\begin{equation}
\label{eq:ptreassign}
\mathbf{p}_{\mathcal{J}_{l\perp}} = \mathbf{j}^B_{l\perp} \equiv \mathbf{p}^B_{\mathcal{J}_{l}\perp}
- \mathbf{q}_\perp \,\frac{|\mathbf{p}^B_{\mathcal{J}_{l}\perp}|}{P^B_\perp},
\end{equation}
which is linear in the resummation momentum. Consequently the equivalent
of~\eqref{eq:ptreassign_old} is non-linear in the Born momentum. However
the exact form of~\eqref{eq:ptreassign_old} is not relevant for the resummation.
Both methods have been tested for two and three jets with the \textsc{rivet}
standard analysis \texttt{MC\_JETS}. They didn't show any differences even
after $10^9$ events.
The reshuffling relation~\eqref{eq:ptreassign} allows the transverse
momenta $p^B_{\mathcal{J}_{l\perp}}$ of the fixed-order jets to be
somewhat below the minimum transverse momentum of resummation jets. It
is crucial that this difference does not become too large, as the
fixed-order cross section diverges for vanishing transverse momenta. In
the production of a Higgs boson with resummation jets above $30\,$GeV we observe
that the contribution from fixed-order events with jets softer than
about $20\,$GeV can be safely neglected. This is shown in the following
plot of the differential cross section over the transverse momentum of
the softest fixed-order jet:
\begin{center}
\includegraphics[width=.75\textwidth]{ptBMin}
\end{center}
Finally, we have to account for the fact that the reshuffling
relation~\eqref{eq:ptreassign} is non-linear in the Born momenta. To
arrive at the master formula~\eqref{eq:resumdijetFKLmatched2} for the
cross section, we have introduced unity in the form of an integral over
the Born momenta with $\delta$ functions in the integrand, that is
\begin{equation}
\label{eq:delta_intro}
1 = \int_{p_{j\perp}^B=0}^{p_{j\perp}^B=\infty}
\mathrm{d}^2\mathbf{p}_{j\perp}^B\delta^{(2)}(\mathbf{p}_{\mathcal{J}_{j\perp}}^B -
\mathbf{j}_{j\perp})\,.
\end{equation}
If the arguments of the $\delta$ functions are not linear in the Born
momenta, we have to compensate with additional Jacobians as
factors. Explicitly, for the reshuffling relation~\eqref{eq:ptreassign}
we have
\begin{equation}
\label{eq:delta_rewrite}
\prod_{l=1}^m \delta^{(2)}(\mathbf{p}_{\mathcal{J}_{l\perp}}^B -
\mathbf{j}_{l\perp}) = \Delta \prod_{l=1}^m \delta^{(2)}(\mathbf{p}_{\mathcal{J}_{l\perp}} -
\mathbf{j}_{l\perp}^B)\,,
\end{equation}
where $\mathbf{j}_{l\perp}^B$ is given by~\eqref{eq:ptreassign_eq} and only
depends on the Born momenta. We have extended the product to run to $m$
instead of $m-1$ by eliminating the last $\delta$ function
$\delta^{(2)}\!\!\left(\sum_{k=1}^n \mathbf{p}_{k\perp}\right )$.
The Jacobian $\Delta$ is the determinant of a $2m \times 2m$ matrix with $l, l' = 1,\dots,m$
and $X, X' = x,y$.
\begin{equation}
\label{eq:jacobian}
\Delta = \left|\frac{\partial\,\mathbf{j}^B_{l'\perp}}{\partial\, \mathbf{p}^B_{{\cal J}_l \perp}} \right|
= \left| \delta_{l l'} \delta_{X X'} - \frac{q_X\, p^B_{{\cal
J}_{l'}X'}}{\left|\mathbf{p}^B_{{\cal J}_{l'} \perp}\right| P^B_\perp}\left(\delta_{l l'}
- \frac{\left|\mathbf{p}^B_{{\cal J}_l \perp}\right|}{P^B_\perp}\right)\right|\,.
\end{equation}
The determinant is calculated in \lstinline!resummation_jet_weight!,
again coming from the \texttt{resummation\_jet.hh} header.
Having to introduce this Jacobian is not a disadvantage specific to the new
reshuffling. If we instead use the old reshuffling
relation~\eqref{eq:ptreassign_old} we \emph{also} have to introduce a
similar Jacobian since we actually want to integrate over the
resummation phase space and need to transform the argument of the
$\delta$ function to be linear in the resummation momenta for this.
\subsubsection{Gluons inside Jets}
\label{sec:gluons_jet}
After the steps outlined in section~\ref{sec:psp_ng_jet}, we have a
total number of $m + n_{g,{\cal J}}$ constituents. In
\lstinline!PhaseSpacePoint::distribute_jet_partons! we distribute them
randomly among the jets such that each jet has at least one
constituent. We then generate their momenta in
\lstinline!PhaseSpacePoint::split! using the \lstinline!Splitter! class.
The phase space integral for a jet ${\cal J}$ is given by
\begin{equation}
\label{eq:ps_jetparton} \prod_{i\text{ in }{\cal J}} \bigg(\int
\mathrm{d}\mathbf{p}_{i\perp}\ \int \mathrm{d} y_i
\bigg)\delta^{(2)}\Big(\sum_{i\text{ in }{\cal J}} \mathbf{p}_{i\perp} -
\mathbf{j}_{\perp}^B\Big)\delta(y_{\mathcal{J}}-y^B_{\mathcal{J}})\,.
\end{equation}
For jets with a single constituent, the parton momentum is obiously equal to the
jet momentum. In the case of two constituents, we observe that the
partons are always inside the jet cone with radius $R$ and often very
close to the jet centre. The following plots show the typical relative
distance $\Delta R/R$ for this scenario:
\begin{center}
\includegraphics[width=0.45\linewidth]{dR_2}
\includegraphics[width=0.45\linewidth]{dR_2_small}
\end{center}
According to this preference for small values of $\Delta R$, we
parametrise the $\Delta R$ integrals as
\begin{equation}
\label{eq:dR_sampling}
\frac{\Delta R}{R} =
\begin{cases}
0.25\,x_R & x_R < 0.4 \\
1.5\,x_R - 0.5 & x_R \geq 0.4
\end{cases}\,.
\end{equation}
Next, we generate $\Theta_1 \equiv \Theta$ and use the constraint $\Theta_2 = \Theta
\pm \pi$. The transverse momentum of the first parton is then given by
\begin{equation}
\label{eq:delta_constraints}
p_{1\perp} =
\frac{p_{\mathcal{J} y} - \tan(\phi_2) p_{\mathcal{J} x}}{\sin(\phi_1)
- \tan(\phi_2)\cos(\phi_1)}\,.
\end{equation}
We get $p_{2\perp}$ by exchanging $1 \leftrightarrow 2$ in the
indices. To obtain the Jacobian of the transformation, we start from the
single jet phase space eq.~(\ref{eq:ps_jetparton}) with the rapidity
delta function already rewritten to be linear in the rapidity of the
last parton, i.e.
\begin{equation}
\label{eq:jet_2p}
\prod_{i=1,2} \bigg(\int
\mathrm{d}\mathbf{p}_{i\perp}\ \int \mathrm{d} y_i
\bigg)\delta^{(2)}\Big(\mathbf{p}_{1\perp} + \mathbf{p}_{2\perp} -
\mathbf{j}_{\perp}^B\Big)\delta(y_2- \dots)\,.
\end{equation}
The integral over the second parton momentum is now trivial; we can just replace
the integral over $y_2$ with the equivalent constraint
\begin{equation}
\label{eq:R2}
\int \mathrm{d}R_2 \ \delta\bigg(R_2 - \bigg[\phi_{\cal J} - \arctan
\bigg(\frac{p_{{\cal J}y} - p_{1y}}{p_{{\cal J}x} -
p_{1x}}\bigg)\bigg]/\cos \Theta\bigg) \,.
\end{equation}
In order to fix the integral over $p_{1\perp}$ instead, we rewrite this
$\delta$ function. This introduces the Jacobian
\begin{equation}
\label{eq:jac_pt1}
\bigg|\frac{\partial p_{1\perp}}{\partial R_2} \bigg| =
\frac{\cos(\Theta)\mathbf{p}_{2\perp}^2}{p_{{\cal J}\perp}\sin(\phi_{\cal J}-\phi_1)}\,.
\end{equation}
The final form of the integral over the two parton momenta is then
\begin{equation}
\label{eq:ps_jet_2p}
\int \mathrm{d}R_1\ R_1 \int \mathrm{d}R_2 \int \mathrm{d}x_\Theta\ 2\pi \int
\mathrm{d}p_{1\perp}\ p_{1\perp} \int \mathrm{d}p_{2\perp}
\ \bigg|\frac{\partial p_{1\perp}}{\partial R_2} \bigg|\delta(p_{1\perp}
-\dots) \delta(p_{2\perp} - \dots)\,.
\end{equation}
As is evident from section~\ref{sec:psp_ng_jet}, jets with three or more
constituents are rare and an efficient phase-space sampling is less
important. For such jets, we exploit the observation that partons with a
distance larger than $R_{\text{max}} = \tfrac{5}{3} R$ to
the jet centre are never clustered into the jet. Assuming $N$
constituents, we generate all components
for the first $N-1$ partons and fix the remaining parton with the
$\delta$-functional. In order to end up inside the jet, we use the
parametrisation
\begin{align}
\label{eq:ps_jet_param}
\phi_i ={}& \phi_{\cal J} + \Delta \phi_i\,, & \Delta \phi_i ={}& \Delta
R_i
\cos(\Theta_i)\,, \\
y_i ={}& y_{\cal J} + \Delta y_i\,, & \Delta y_i ={}& \Delta
R_i
\sin(\Theta_i)\,,
\end{align}
and generate $\Theta_i$ and $\Delta R_i$ randomly with $\Delta R_i \leq
R_{\text{max}}$ and the empiric value $R_{\text{max}} = 5\*R/3$. We can
then write the phase space integral for a single parton as $(p_\perp = |\mathbf{p}_\perp|)$
\begin{equation}
\label{eq:ps_jetparton_x}
\int \mathrm{d}\mathbf{p}_{\perp}\ \int
\mathrm{d} y \approx \int_{\Box} \mathrm{d}x_{\perp}
\mathrm{d}x_{ R}
\mathrm{d}x_{\theta}\
2\*\pi\,\*R_{\text{max}}^2\,\*x_{R}\,\*p_{\perp}\,\*(p_{\perp,\text{max}}
- p_{\perp,\text{min}})
\end{equation}
with
\begin{align}
\label{eq:ps_jetparton_parameters}
\Delta \phi ={}& R_{\text{max}}\*x_{R}\*\cos(2\*\pi\*x_\theta)\,,&
\Delta y ={}& R_{\text{max}}\*x_{R}\*\sin(2\*\pi\*x_\theta)\,, \\
p_{\perp} ={}& (p_{\perp,\text{max}} - p_{\perp,\text{min}})\*x_\perp +
p_{\perp,\text{min}}\,.
\end{align}
$p_{\perp,\text{max}}$ is determined from the requirement that the total
contribution from the first $n-1$ partons --- i.e. the projection onto the
jet $p_{\perp}$ axis --- must never exceed the jet $p_\perp$. This gives
\todo{This bound is too high}
\begin{equation}
\label{eq:pt_max}
p_{i\perp,\text{max}} = \frac{p_{{\cal J}\perp} - \sum_{j<i} p_{j\perp}
\cos \Delta
\phi_j}{\cos \Delta
\phi_i}\,.
\end{equation}
The $x$ and $y$ components of the last parton follow immediately from
the first $\delta$ function. The last rapidity is fixed by the condition that
the jet rapidity is kept fixed by the reshuffling, i.e.
\begin{equation}
\label{eq:yJ_delta}
y^B_{\cal J} = y_{\cal J} = \frac 1 2 \ln \frac{\sum_{i=1}^n E_i+ p_{iz}}{\sum_{i=1}^n E_i - p_{iz}}\,.
\end{equation}
With $E_n \pm p_{nz} = p_{n\perp}\exp(\pm y_n)$ this can be rewritten to
\begin{equation}
\label{eq:yn_quad_eq}
\exp(2y_{\cal J}) = \frac{\sum_{i=1}^{n-1} E_i+ p_{iz}+p_{n\perp} \exp(y_n)}{\sum_{i=1}^{n-1} E_i - p_{iz}+p_{n\perp} \exp(-y_n)}\,,
\end{equation}
which is a quadratic equation in $\exp(y_n)$. The physical solution is
\begin{align}
\label{eq:yn}
y_n ={}& \log\Big(-b + \sqrt{b^2 + \exp(2y_{\cal J})}\,\Big)\,,\\
b ={}& \bigg(\sum_{i=1}^{n-1} E_i + p_{iz} - \exp(2y_{\cal J})
\sum_{i=1}^{n-1} E_i - p_{iz}\bigg)/(2 p_{n\perp})\,.
\end{align}
\todo{what's wrong with the following?} To eliminate the remaining rapidity
integral, we transform the $\delta$ function to be linear in the
rapidity $y$ of the last parton. The corresponding Jacobian is
\begin{equation}
\label{eq:jacobian_y}
\bigg|\frac{\partial y_{\cal J}}{\partial y_n}\bigg|^{-1} = 2 \bigg( \frac{E_n +
p_{nz}}{E_{\cal J} + p_{{\cal J}z}} + \frac{E_n - p_{nz}}{E_{\cal J} -
p_{{\cal J}z}}\bigg)^{-1}\,.
\end{equation}
Finally, we check that all designated constituents are actually
clustered into the considered jet.
\subsubsection{Final steps}
\label{sec:final}
Knowing the rapidity span covered by the extremal partons, we can now
generate the rapdities for the partons outside jets. We perform jet
clustering on all partons and check in
\lstinline!PhaseSpacePoint::jets_ok! that all the following criteria are
fulfilled:
\begin{itemize}
\item The number of resummation jets must match the number of
fixed-order jets.
\item No partons designated to be outside jets may end up inside jets.
\item All other outgoing partons \emph{must} end up inside jets.
\item The extremal (in rapidity) partons must be inside the extremal
jets. If there is, for example, an unordered forward emission, the
most forward parton must end up inside the most forward jet and the
next parton must end up inside second jet.
\item The rapidities of fixed-order and resummation jets must match.
\end{itemize}
After this, we adjust the phase-space normalisation according to the
third line of eq.~(\ref{eq:resumdijetFKLmatched2}), determine the
flavours of the outgoing partons, and adopt any additional colourless
bosons from the fixed-order input event. Finally, we use momentum
conservation to reconstruct the momenta of the incoming partons.
\subsection{The matrix element }
\label{sec:ME}
The derivation of the \HEJ matrix element is explained in some detail
in~\cite{Andersen:2017kfc}, where also results for leading and
subleading matrix elements for pure multijet production and production
of a Higgs boson with at least two associated jets are listed. Matrix
elements for $W$ and $Z/\gamma^*$ production together with jets are
given in~\cite{Andersen:2012gk,Andersen:2016vkp}, but not yet included.
The matrix elements are implemented in the \lstinline!MatrixElement!
-class. To discuss the structure, let us consider the matrix element for
-FKL multijet production:
+class. To discuss the structure, let us consider the squared matrix
+element for FKL multijet production with $n$ final-state partons:
\begin{align}
\label{eq:ME}
\begin{split}
\overline{\left|\mathcal{M}_\text{HEJ}^{f_1 f_2 \to f_1
- g\cdots g f_2}\right|}^2 = \ &\frac 1 {4\
- (N_c^2-1)}\ \left\|S_{f_1 f_2\to f_1 f_2}\right\|^2\\
- &\cdot\ \left(g_s^2 K_{f_1}\ \frac 1 {t_1}\right) \cdot\ \left(g_s^2\ K_{f_2}\ \frac 1
- {t_{n-1}}\right)\\
- & \cdot \prod_{i=1}^{n-2} \left( \frac{-g_s^2 C_A}{t_it_{i+1}}\
- V^\mu(q_i,q_{i+1})V_\mu(q_i,q_{i+1}) \right)\\
- & \cdot \prod_{j=1}^{n-1} \exp\left[\omega^0(q_{j\perp})(y_{j+1}-y_j)\right].
+ g\cdots g f_2}\right|}^2 = \ &\frac {(4\pi\alpha_s)^n} {4\ (N_c^2-1)}
+ \cdot\ \textcolor{blue}{\frac {K_{f_1}(p_1^-, p_a^-)} {t_1}\ \cdot\ \frac{K_{f_2}(p_n^+, p_b^+)}{t_{n-1}}\ \cdot\ \left\|S_{f_1 f_2\to f_1 f_2}\right\|^2}\\
+ & \cdot \prod_{i=1}^{n-2} \textcolor{gray}{\left( \frac{-C_A}{t_it_{i+1}}\
+ V^\mu(q_i,q_{i+1})V_\mu(q_i,q_{i+1}) \right)}\\
+ & \cdot \prod_{j=1}^{n-1} \textcolor{red}{\exp\left[\omega^0(q_{j\perp})(y_{j+1}-y_j)\right]}.
\end{split}
\end{align}
-The square of the complete matrix element as given in eq.~(\ref{eq:ME})
-is calculated by \lstinline!MatrixElement::operator()!. The last line
-of eq.~\eqref{eq:ME} constitutes the all-order virtual correction,
-implemented in \lstinline!MatrixElement::virtual_corrections!. The
-remaining parts, which correspond to the square of the leading-order HEJ
-matrix element $\overline{\left|\mathcal{M}_\text{LO, HEJ}^{f_1f_2\to
-f_1g\cdots gf_2}\big(\big\{p^B_j\big\}\big)\right|}^{2}$, are computed
-in \lstinline!MatrixElement::tree!. We can further factor off the
+The structure and momentum assignment of the unsquared matrix element is
+as illustrated here:
+\begin{center}
+ \includegraphics{HEJ_amplitude}
+\end{center}
+The square
+of the complete matrix element as given in eq.~(\ref{eq:ME}) is
+calculated by \lstinline!MatrixElement::operator()!. The \textcolor{red}{last line} of
+eq.~\eqref{eq:ME} constitutes the all-order virtual correction,
+implemented in
+\lstinline!MatrixElement::virtual_corrections!.
+$\omega^0$ is the
+\textit{regularised Regge trajectory}
+\begin{equation}
+ \label{eq:omega_0}
+ \omega^0(q_\perp) = - C_A \frac{\alpha_s}{\pi} \log \left(\frac{q_\perp^2}{\lambda^2}\right)\,,
+\end{equation}
+where $\lambda$ is the slicing parameter limiting the softness of real
+gluon emissions, cf. eq.~(\ref{eq:resumdijetFKLmatched2}).
+
+The remaining parts, which correspond to the square of the leading-order
+HEJ matrix element $\overline{\left|\mathcal{M}_\text{LO,
+HEJ}^{f_1f_2\to f_1g\cdots
+gf_2}\big(\big\{p^B_j\big\}\big)\right|}^{2}$, are computed in
+\lstinline!MatrixElement::tree!. We can further factor off the
scale-dependent ``parametric'' part
\lstinline!MatrixElement::tree_param! containing all factors of the
-strong coupling $g_s$. Using this function saves some CPU time when
-adjusting the renormalisation scale, see section~\ref{sec:resum}.
+strong coupling $4\pi\alpha_s$. Using this function saves some CPU time
+when adjusting the renormalisation scale, see
+section~\ref{sec:resum}. The remaining ``kinematic'' factors are
+calculated in \lstinline!MatrixElement::kin!.
+
+\subsubsection{Matrix elements for Higgs plus dijet}
+\label{sec:ME_h_jets}
+
+In the production of a Higgs boson together with jets The parametric
+parts and the virtual corrections only require minor changes in the
+respective functions. However, in the ``kinematic'' parts we have to
+distinguish between several cases, which is done in
+\lstinline!MatrixElement::tree_kin_Higgs!. The Higgs boson can be
+\emph{central}, i.e. inside the rapidity range spanned by the extremal
+partons (\lstinline!MatrixElement::tree_kin_Higgs_central!) or
+\emph{peripheral} and outside this range
+(\lstinline!MatrixElement::tree_kin_Higgs_first! or
+\lstinline!MatrixElement::tree_kin_Higgs_last!). In case there is also
+an unordered gluon emission, we always consider the Higgs boson to be
+central.\todo{Why again?}
+
+If a Higgs boson with momentum $p_H$ is emitted centrally, after parton
+$j$ in rapidity, the matrix element reads
+\begin{equation}
+ \label{eq:ME_h_jets_central}
+ \begin{split}
+ \overline{\left|\mathcal{M}_\text{HEJ}^{f_1 f_2 \to f_1 g\cdot H
+ \cdot g f_2}\right|}^2 = \ &\frac {\alpha_s^2 (4\pi\alpha_s)^n} {4\ (N_c^2-1)}
+ \cdot\ \textcolor{blue}{\frac {K_{f_1}(p_1^-, p_a^-)} {t_1}\
+\cdot\ \frac{1}{t_j t_{j+1}} \cdot\ \frac{K_{f_2}(p_n^+, p_b^+)}{t_{n}}\ \cdot\ \left\|S_{f_1
+ f_2\to f_1 H f_2}\right\|^2}\\
+ & \cdot \prod_{\substack{i=1\\i \neq j}}^{n-1} \textcolor{gray}{\left( \frac{-C_A}{t_it_{i+1}}\
+ V^\mu(q_i,q_{i+1})V_\mu(q_i,q_{i+1}) \right)}\\
+ & \cdot \textcolor{red}{\prod_{i=1}^{n-1}
+ \exp\left[\omega^0(q_{i\perp})\Delta y_i\right]}
+ \end{split}
+\end{equation}
+with the momentum definitions
+\begin{center}
+ \includegraphics{HEJ_central_Higgs_amplitude}
+\end{center}
+$q_i$ is the $i$th $t$-channel momentum and $\Delta y_i$ the rapidity
+gap between outgoing \emph{particles} (not partons) $i$ and $i+1$ in
+rapidity ordering.
+
+For \emph{peripheral} emission in the backward direction
+(\lstinline!MatrixElement::tree_kin_Higgs_first!) we first check whether
+the most backward parton is a gluon or an (anti-)quark. In the latter
+case the leading contribution to the matrix element arises through
+emission off the $t$-channel gluons and we can use the same formula
+eq.~(\ref{eq:ME_h_jets_central}) as for central emission. If the most
+backward parton is a gluon, the square of the matrix element can be
+written as
+\begin{equation}
+ \label{eq:ME_h_jets_peripheral}
+ \begin{split}
+ \overline{\left|\mathcal{M}_\text{HEJ}^{g f_2 \to H g\cdot g f_2}\right|}^2 = \ &\frac {\alpha_s^2 (4\pi\alpha_s)^n} {\textcolor{blue}{4\ (N_c^2-1)}}
+ \textcolor{blue}{\cdot\ K_{H}\
+ \frac{K_{f_2}(p_n^+, p_b^+)}{t_{n-1}}\ \cdot\ \left\|S_{g
+ f_2\to H g f_2}\right\|^2}\\
+ & \cdot \prod_{\substack{i=1}}^{n-2} \textcolor{gray}{\left( \frac{-C_A}{t_it_{i+1}}\
+ V^\mu(q_i,q_{i+1})V_\mu(q_i,q_{i+1}) \right)}\\
+ & \cdot \textcolor{red}{\prod_{i=1}^{n-1}
+ \exp\left[\omega^0(q_{i\perp}) (y_{i+1} - y_i)\right]}
+ \end{split}
+\end{equation}
+with the momenta as follows:
+\begin{center}
+ \includegraphics{HEJ_peripheral_Higgs_amplitude}
+\end{center}
+The \textcolor{blue}{blue part} is implemented in
+\lstinline!MatrixElement::MH2_forwardH!. All other building blocks are
+already available.\todo{Impact factors} The actual current contraction
+is calculated in \lstinline!MH2gq_outsideH! inside
+\lstinline!currents.cc!, which corresponds to $\tfrac{16 \pi^2}{t_1} \left\|S_{g
+ f_2\to H g f_2}\right\|^2$.\todo{Fix this insane normalisation}
+
+The forward emission of a Higgs boson is completely analogous. We can
+use the same function \lstinline!MatrixElement::MH2_forwardH!, swapping
+$p_1 \leftrightarrow p_n,\,p_a \leftrightarrow p_b$.
-The remaining ``kinematic'' factors are calculated in
-\lstinline!MatrixElement::kin!. The currents $\frac{K_{f_1}K_{f_2}}{t_1
-t_{n-1}}\left\|S_{f_1 f_2\to f_1 f_2}\right\|^2$ are implemented in the
-\lstinline!jM2!$\dots$ functions of \texttt{src/currents.cc}
-\footnote{The current implementation for Higgs production in
-\texttt{src/currents.cc} includes the $1/4$ factor inside $S$, opposing
-to~\eqref{eq:ME}. Thus the overall normalisation is unaffected.}.
+\subsubsection{FKL ladder and Lipatov vertices}
+\label{sec:FKL_ladder}
+
+The ``FKL ladder'' is the product
+\begin{equation}
+ \label{eq:FKL_ladder}
+ \prod_{i=1}^{n-2} \left( \frac{-C_A}{t_it_{i+1}}\
+ V^\mu(q_i,q_{i+1})V_\mu(q_i,q_{i+1}) \right)
+\end{equation}
+appearing in the square of the matrix element for $n$ parton production,
+cf. eq.~(\ref{eq:ME}), and implemented in
+\lstinline!MatrixElement::FKL_ladder_weight!. The Lipatov vertex contraction
+$V^\mu(q_i,q_{i+1})V_\mu(q_i,q_{i+1})$ is implemented \lstinline!C2Lipatovots!.
+It is given by \todo{equation} \todo{mention difference between the two versions
+of \lstinline!C2Lipatovots!, maybe even get rid of one}.
+
+\subsubsection{Currents}
+\label{sec:currents}
+
+The current factors $\frac{K_{f_1}K_{f_2}}{t_1 t_{n-1}}\left\|S_{f_1
+f_2\to f_1 f_2}\right\|^2$ and their extensions for unordered and Higgs
+boson emissions are implemented in the \lstinline!jM2!$\dots$ functions
+of \texttt{src/currents.cc}. \todo{Only $\|S\|^2$ should be in currents}
+\footnote{The current implementation for
+Higgs production in \texttt{src/currents.cc} includes the $1/4$ factor
+inside $S$, opposing to~\eqref{eq:ME}. Thus the overall normalisation is
+unaffected.} The ``colour acceleration multiplier'' (CAM) $K_{f}$
+for a parton $f\in\{g,q,\bar{q}\}$ is defined as
+\begin{align}
+ \label{eq:K_g}
+ K_g(p_1^-, p_a^-) ={}& \frac{1}{2}\left(\frac{p_1^-}{p_a^-} + \frac{p_a^-}{p_1^-}\right)\left(C_A -
+ \frac{1}{C_A}\right)+\frac{1}{C_A}\\
+ \label{eq:K_q}
+ K_q(p_1^-, p_a^-) ={}&K_{\bar{q}}(p_1^-, p_a^-) = C_F\,.
+\end{align}
+The Higgs current CAM used in eq.~(\ref{eq:ME_h_jets_peripheral}) is
+\begin{equation}
+ \label{eq:K_H}
+ K_H = C_A\,.
+\end{equation}
+The current contractions are given by\todo{check all this
+ carefully!}
+\begin{align}
+ \label{eq:S}
+ \left\|S_{f_1 f_2\to f_1 f_2}\right\|^2 ={}& \sum_{\substack{\lambda_a =
+ +,-\\\lambda_b = +,-}} \left|j^{\lambda_a}_\mu(p_1, p_a)\
+j^{\lambda_b\,\mu}(p_n, p_b)\right|^2 = 2\sum_{\lambda =
+ +,-} \left|j^{-}_\mu(p_1, p_a)\ j^{\lambda\,\mu}(p_n, p_b)\right|^2\,,\\
+ \left\|S_{f_1 f_2\to f_1 H f_2}\right\|^2 ={}& \sum_{\substack{\lambda_a =
+ +,-\\\lambda_b = +,-}} \left|j^{\lambda_a}_\mu(p_1, p_a)V_H^{\mu\nu}(q_j, q_{j+1})\
+ j^{\lambda_b}_\nu(p_n, p_b)\right|^2\,,\\
+ \left\|S_{g f_2 \to H g f_2}\right\|^2 ={}& \sum_{
+ \substack{
+ \lambda_{a} = +,-\\
+ \lambda_{1} =+,-\\
+ \lambda_{b} = +,-
+ }}
+ \left|j^{\lambda_a\lambda_1}_{H\,\mu}(p_1, p_a, p_H)\ j^{\lambda_b\,\mu}(p_n, p_b)\right|^2\,.
+\end{align}
+The ``basic'' currents $j$ are independent of the parton flavour and read
+\begin{equation}
+ \label{eq:j}
+ j^\pm_\mu(p, q) = u^{\pm,\dagger}(p)\ \sigma^\pm_\mu\ u^{\pm}(q)\,,
+\end{equation}
+where $\sigma_\mu^\pm = (1, \pm \sigma_i)$ and $\sigma_i$ are the Pauli
+matrices
+\begin{equation}
+ \label{eq:Pauli_matrices}
+ \sigma_1 =
+ \begin{pmatrix}
+ 0 & 1\\ 1 & 0
+ \end{pmatrix}
+\,,
+ \qquad \sigma_2 =
+ \begin{pmatrix}
+ 0 & -i\\ i & 0
+ \end{pmatrix}
+\,,
+ \qquad \sigma_3 =
+ \begin{pmatrix}
+ 1 & 0\\ 0 & -1
+ \end{pmatrix}
+\,.
+\end{equation}
+The two-component chiral spinors are given by
+\begin{align}
+ \label{eq:u_plus}
+ u^+(p)={}& \left(\sqrt{p^+}, \sqrt{p^-} \hat{p}_\perp \right) \,,\\
+ \label{eq:u_minus}
+ u^-(p)={}& \left(\sqrt{p^-} \hat{p}^*_\perp, -\sqrt{p^+}\right)\,,
+\end{align}
+with $p^\pm = E\pm p_z,\, \hat{p}_\perp = \tfrac{p_\perp}{|p_\perp|},\,
+p_\perp = p_x + i p_y$. The spinors for vanishing transverse momentum
+are obtained by replacing $\hat{p_\perp} \to -1$.
+
+Explicitly, the currents read
+\begin{align}
+ \label{eq:j-_explicit}
+ j^-_\mu(p, q) ={}&
+ \begin{pmatrix}
+ \sqrt{p^+\,q^+} + \sqrt{p^-\,q^-} \hat{p}_{\perp} \hat{q}_{\perp}^*\\
+ \sqrt{p^-\,q^+}\, \hat{p}_{\perp} + \sqrt{p^+\,q^-}\,\hat{q}_{\perp}^*\\
+ -i \sqrt{p^-\,q^+}\, \hat{p}_{\perp} + i \sqrt{p^+\,q^-}\, \hat{q}_{\perp}^*\\
+ \sqrt{p^+\,q^+} - \sqrt{p^-\,q^-}\, \hat{p}_{\perp}\, \hat{q}_{\perp}^*
+ \end{pmatrix}\\
+ j^+_\mu(p, q) ={}&\big(j^-_\mu(p, q)\big)^*
+\end{align}
+If $q= p_{\text{in}}$ is the momentum of an incoming parton, we have
+$\hat{p}_{\text{in} \perp} = -1$ and either $p_{\text{in}}^+ = 0$ or
+$p_{\text{in}}^- = 0$. The current simplifies further:\todo{Helicities flipped w.r.t code}
+\begin{align}
+ \label{eq:j_explicit}
+ j^-_\mu(p_{\text{out}}, p_{\text{in}}) ={}&
+ \begin{pmatrix}
+ \sqrt{p_{\text{in}}^+\,p_{\text{out}}^+}\\
+ \sqrt{p_{\text{in}}^+\,p_{\text{out}}^-} \ \hat{p}_{\text{out}\,\perp}\\
+ -i\,j^-_1\\
+ j^-_0
+ \end{pmatrix}
+& p_{\text{in}\,z} > 0\,,\\
+ j^-_\mu(p_{\text{out}}, p_{\text{in}}) ={}&
+ \begin{pmatrix}
+ -\sqrt{p_{\text{in}}^-\,p_{\text{out}}^{-\phantom{+}}} \ \hat{p}_{\text{out}\,\perp}\\
+ - \sqrt{p_{\text{in}}^-\,p_{\text{out}}^+}\\
+ i\,j^-_1\\
+ -j^-_0
+ \end{pmatrix} & p_{\text{in}\,z} < 0\,.
+\end{align}
\section{The fixed-order generator}
\label{sec:HEJFOG}
Even at leading order, standard fixed-order generators can only generate
events with a limited number of final-state particles within reasonable
CPU time. The purpose of the fixed-order generator is to supplement this
with high-multiplicity input events according to the first two lines of
eq.~\eqref{eq:resumdijetFKLmatched2} with the \HEJ approximation
$\mathcal{M}_\text{LO, HEJ}^{f_1f_2\to f_1g\cdots gf_2}$ instead of the
full fixed-order matrix element $\mathcal{M}_\text{LO}^{f_1f_2\to
f_1g\cdots gf_2}$. Its usage is described in the user
-documentation\todo{link}.
+documentation \url{https://hej.web.cern.ch/HEJ/doc/current/user/HEJFOG.html}.
\subsection{File structure}
\label{sec:HEJFOG_structure}
The code for the fixed-order generator is in the \texttt{FixedOrderGen}
directory, which contains the following:
\begin{description}
\item[include:] Contains the C++ header files.
\item[src:] Contains the C++ source files.
\item[t:] Contains the source code for the automated tests.
\item[CMakeLists.txt:] Configuration file for the \cmake build system.
\item[configFO.yml:] Sample configuration file for the fixed-order generator.
\end{description}
The code is generally in the \lstinline!HEJFOG! namespace. Functions and
classes \lstinline!MyClass! are usually declared in
\texttt{include/MyClass.hh} and implemented in \texttt{src/MyClass.cc}.
\subsection{Program flow}
\label{sec:prog_flow}
A single run of the fixed-order generator consists of three or four
stages.
First, we perform initialisation similar to HEJ 2, see
section~\ref{sec:init}. Since there is a lot of overlap we frequently
reuse classes and functions from HEJ 2, i.e. from the
\lstinline!HEJ! namespace. The code for parsing the configuration file
is in \texttt{include/config.hh} and implemented in
\texttt{src/config.cc}.
-If partial unweighting is requested in the user settings \todo{link},
+If partial unweighting is requested in the user settings \url{https://hej.web.cern.ch/HEJ/doc/current/user/HEJFOG.html#settings},
the initialisation is followed by a calibration phase. We use a
\lstinline!EventGenerator! to produce a number of trial
events. We use these to calibrate the \lstinline!Unweighter! in
its constructor and produce a first batch of partially unweighted
events. This also allows us to estimate our unweighting efficiency.
In the next step, we continue to generate events and potentially
unweight them. Once the user-defined target number of events is reached,
we adjust their weights according to the number of required trials. As
in HEJ 2 (see section~\ref{sec:processing}), we pass the final
events to a \lstinline!HEJ::Analysis! and a
\lstinline!HEJ::CombinedEventWriter!.
\subsection{Event generation}
\label{sec:evgen}
Event generation is performed by the
\lstinline!EventGenerator::gen_event! member function. We begin by generating a
\lstinline!PhaseSpacePoint!. This is not to be confused with
the resummation phase space points represented by
\lstinline!HEJ::PhaseSpacePoint!! After jet clustering, we compute the
leading-order matrix element (see section~\ref{sec:ME}) and pdf factors.
The phase space point generation is performed in the
\lstinline!PhaseSpacePoint! constructor. We first construct the
user-defined number of $n_p$ partons (by default gluons) in
\lstinline!PhaseSpacePoint::gen_LO_partons!. We use flat sampling in
rapidity and azimuthal angle. For the scalar transverse momenta, we
distinguish between two cases. By default, they are generated based on a
random variable $x_{p_\perp}$ according to
\begin{equation}
\label{eq:pt_sampling}
p_\perp = p_{\perp,\text{min}} +
\begin{cases}
p_{\perp,\text{par}}
\tan\left(
x_{p_\perp}
\arctan\left(
\frac{p_{\perp,\text{max}} - p_{\perp,\text{min}}}{p_{\perp,\text{par}}}
\right)
\right)
& y < y_\text{cut}
\\
- \tilde{p}_{\perp,\text{par}}\log\left(1 - x_{p_\perp}\left[1 -
\exp\left(\frac{p_{\perp,\text{min}} -
p_{\perp,\text{max}}}{\tilde{p}_{\perp,\text{par}}}\right)\right]\right)
& y \geq y_\text{cut}
\end{cases}\,,
\end{equation}
where $p_{\perp,\text{min}}$ is the minimum jet transverse momentum,
$p_{\perp,\text{max}}$ is the maximum transverse parton momentum,
tentatively set to the beam energy, and $y_\text{cut}$, $p_{\perp,\text{par}}$
and $\tilde{p}_{\perp,\text{par}}$ are generation parameters set to
heuristically determined values of
\begin{align}
y_\text{cut}&=3,\\
p_{\perp,\text{par}}&=p_{\perp,\min}+\frac{n_p}{5}, \\
\tilde{p}_{\perp,\text{par}}&=\frac{p_{\perp,\text{par}}}{1 +
5(y-y_\text{cut})}.
\end{align}
The problem with this generation is that the transverse momenta peak at
the minimum transverse momentum required for fixed-order jets. However,
if we use the generated events as input for \HEJ resummation, events
with such soft transverse momenta hardly contribute, see
section~\ref{sec:ptj_res}. To generate efficient input for resummation,
there is the user option \texttt{peak pt}, which specifies the
dominant transverse momentum for resummation jets. If this option is
set, most jets will be generated as above, but with
$p_{\perp,\text{min}}$ set to the peak transverse momentum $p_{\perp,
\text{peak}}$. In addition, there is a small chance of around $2\%$ to
generate softer jets. The heuristic ansatz for the transverse momentum
distribution in the ``soft'' region is
\begin{equation}
\label{FO_pt_soft}
\frac{\partial \sigma}{\partial p_\perp} \propto e^{n_p\frac{p_\perp- p_{\perp,
\text{peak}}}{\bar{p}_\perp}}\,,
\end{equation}
where $n_p$ is the number of partons and $\bar{p}_\perp \approx
4\,$GeV. To achieve this distribution, we use
\begin{equation}
\label{eq:FO_pt_soft_sampling}
p_\perp = p_{\perp, \text{peak}} + \bar{p}_\perp \frac{\log x_{p_\perp}}{n_p}
\end{equation}
and discard the phase space point if the parton is too soft, i.e. below the threshold for
fixed-order jets.
After ensuring that all partons form separate jets, we generate any
potential colourless emissions. We then determine the incoming momenta
and flavours in \lstinline!PhaseSpacePoint::reconstruct_incoming! and
adjust the outgoing flavours to ensure an FKL configuration. Finally, we
may reassign outgoing flavours to generate suppressed (for example
unordered) configurations.
\subsection{Unweighting}
\label{sec:unweight}
Straightforward event generation tends to produce many events with small
weights. Those events have a negligible contribution to the final
observables, but can take up considerable storage space and CPU time in
later processing stages. This problem can be addressed by unweighting.
For naive unweighting, one would determine the maximum weight
$w_\text{max}$ of all events, discard each event with weight $w$ with a
probability $p=w/w_\text{max}$, and set the weights of all remaining
events to $w_\text{max}$. The downside to this procedure is that it also
eliminates a sizeable fraction of events with moderate weight, so that
the statistical convergence deteriorates.
To ameliorate this problem, we perform unweighting only for events with
sufficiently small weights. This is done by the
\lstinline!Unweighter! class. In the constructor we estimate the
mean and width of the weight-weight distribution from a sample of
events. We use these estimates to determine the maximum weight below
which unweighting is performed. The actual unweighting is the done in
the \lstinline!Unweighter::unweight! function.
\input{currents}
\bibliographystyle{JHEP}
\bibliography{biblio}
\end{document}
diff --git a/doc/developer_manual/src/HEJ_amplitude.asy b/doc/developer_manual/src/HEJ_amplitude.asy
new file mode 100644
index 0000000..f6fd9ca
--- /dev/null
+++ b/doc/developer_manual/src/HEJ_amplitude.asy
@@ -0,0 +1,87 @@
+import feynman;
+usepackage("fourier");
+// usepackage("sansmathfonts");
+// texpreamble("\renewcommand{\familydefault}{\sfdefault}");
+
+defaultpen(fontsize(8));
+
+path zigzag(path g, real step=2, real distance=2) {
+ real len = arclength(g);
+ int state = 0;
+ path zig;
+ for (real u = 0; u < len; u += step) {
+ real t = arctime(g, u);
+ pair p = point(g, t);
+ pair norm = unit(rotate(90) * dir(g, t));
+ if (state == 1)
+ p = p + distance * norm;
+ else if (state == 3)
+ p = p - distance * norm;
+ zig = zig -- p;
+ state = (state + 1) % 4;
+ }
+ zig = zig -- point(g, length(g));
+ return zig;
+}
+
+real h = 80;
+real w = 60;
+real arrsize = 15;
+real arrdist = 7;
+real vxsize=7;
+
+pair[] v = {
+ (0,h), (0,h/3), (0,-h/3), (0,-h)
+};
+
+path box = scale(vxsize)*shift(SW/sqrt(2))*unitsquare;
+path triangle = scale(vxsize)*(E -- N/2 -- S/2 --cycle);
+
+path pa = (-w,h)--(-2*vxsize,h);
+draw(pa, currentpen+1);
+draw(gluon(pa));
+draw("$p_a$", shift(arrdist*S)*((midpoint(pa)+arrsize/2*W) -- (midpoint(pa)+arrsize/2*E)), Arrow(4));
+path p1 = (w,h)--(2*vxsize,h);
+draw(p1, currentpen+1);
+draw(gluon(p1));
+draw("$p_1$", shift(arrdist*S)*((midpoint(p1)+arrsize/2*W) -- (midpoint(p1)+arrsize/2*E)), Arrow(4));
+path pb = (-w,-h)--(-2*vxsize,-h);
+draw(pb, currentpen+1);
+draw(gluon(pb));
+draw(Label("$p_b$", MidPoint, N), shift(arrdist*N)*((midpoint(pb)+arrsize/2*W) -- (midpoint(pb)+arrsize/2*E)), Arrow(4));
+path pn = (w,-h)--(2*vxsize,-h);
+draw(pn, currentpen+1);
+draw(gluon(pn));
+draw(Label("$p_n$", MidPoint, N), shift(arrdist*N)*((midpoint(pn)+arrsize/2*W) -- (midpoint(pn)+arrsize/2*E)), Arrow(4));
+path q1 = v[0]-(0,vxsize/2)--v[1]+(0,vxsize/2);
+draw(zigzag(q1), red);
+draw(Label("$q_1$", MidPoint, E), shift(arrdist*E)*((midpoint(q1)+arrsize/2*N) -- (midpoint(q1)+arrsize/2*S)), red, Arrow(4));
+draw(
+ zigzag(v[1]-(0,vxsize/2)--v[1]-(0,vxsize/2)+7S),
+ red
+ );
+draw(v[1]-(0,vxsize/2)+7S --v[2]+(0,vxsize/2)+7N, red+Dotted);
+draw(
+ zigzag(v[2]+(0,vxsize/2)+7N--v[2]+(0,vxsize/2)),
+ red
+ );
+path qn = v[2]-(0,vxsize/2)--v[3]+(0,vxsize/2);
+draw(zigzag(qn), red);
+draw(Label("$q_{n-1}$", MidPoint, E), shift(arrdist*E)*((midpoint(qn)+arrsize/2*N) -- (midpoint(qn)+arrsize/2*S)), red, Arrow(4));
+
+
+draw(gluon(v[1]+(vxsize/2,0)--(w,v[1].y)));
+filldraw(shift(v[1])*box,grey);
+draw(gluon(v[2]+(vxsize/2,0)--(w,v[2].y)));
+filldraw(shift(v[2])*box,grey);
+
+draw(rotate(90)*"Increasing rapidity", (1.5w,h)--(1.5w,-h),Arrow);
+
+filldraw(shift(0, h)*xscale(7)*box, blue);
+label("Current", (0,h+vxsize/2), N, blue);
+
+label("``Reggeised gluon\"", (v[0]+v[1])/2, W, red);
+
+label("Lipatov vertex", v[2]+vxsize/2*W, W, grey);
+
+filldraw(shift(0, -h)*xscale(7)*box, blue);
diff --git a/doc/developer_manual/src/HEJ_central_Higgs_amplitude.asy b/doc/developer_manual/src/HEJ_central_Higgs_amplitude.asy
new file mode 100644
index 0000000..512332b
--- /dev/null
+++ b/doc/developer_manual/src/HEJ_central_Higgs_amplitude.asy
@@ -0,0 +1,106 @@
+import feynman;
+usepackage("fourier");
+// usepackage("sansmathfonts");
+// texpreamble("\renewcommand{\familydefault}{\sfdefault}");
+
+defaultpen(fontsize(8));
+
+path zigzag(path g, real step=2, real distance=2) {
+ real len = arclength(g);
+ int state = 0;
+ path zig;
+ for (real u = 0; u < len; u += step) {
+ real t = arctime(g, u);
+ pair p = point(g, t);
+ pair norm = unit(rotate(90) * dir(g, t));
+ if (state == 1)
+ p = p + distance * norm;
+ else if (state == 3)
+ p = p - distance * norm;
+ zig = zig -- p;
+ state = (state + 1) % 4;
+ }
+ zig = zig -- point(g, length(g));
+ return zig;
+}
+
+real h = 80;
+real w = 60;
+real arrsize = 15;
+real arrdist = 7;
+real vxsize=7;
+
+pair[] v = {
+ (0,h), (0,3h/5), (0,h/5), (0,-h/5), (0,-3h/5), (0,-h)
+};
+
+path box = scale(vxsize)*shift(SW/sqrt(2))*unitsquare;
+path triangle = scale(vxsize)*(E -- N/2 -- S/2 --cycle);
+
+path pa = (-w,h)--(-2*vxsize,h);
+draw(pa, currentpen+1);
+draw(gluon(pa));
+draw("$p_a$", shift(arrdist*S)*((midpoint(pa)+arrsize/2*W) -- (midpoint(pa)+arrsize/2*E)), Arrow(4));
+path p1 = (w,h)--(2*vxsize,h);
+draw(p1, currentpen+1);
+draw(gluon(p1));
+draw("$p_1$", shift(arrdist*S)*((midpoint(p1)+arrsize/2*W) -- (midpoint(p1)+arrsize/2*E)), Arrow(4));
+path pb = (-w,-h)--(-2*vxsize,-h);
+draw(pb, currentpen+1);
+draw(gluon(pb));
+draw(Label("$p_b$", MidPoint, N), shift(arrdist*N)*((midpoint(pb)+arrsize/2*W) -- (midpoint(pb)+arrsize/2*E)), Arrow(4));
+path pn = (w,-h)--(2*vxsize,-h);
+draw(pn, currentpen+1);
+draw(gluon(pn));
+draw(Label("$p_n$", MidPoint, N), shift(arrdist*N)*((midpoint(pn)+arrsize/2*W) -- (midpoint(pn)+arrsize/2*E)), Arrow(4));
+path q1 = v[0]-(0,vxsize/2)--v[1]+(0,vxsize/2);
+draw(zigzag(q1), red);
+draw(Label("$q_1$", MidPoint, E), shift(arrdist*E)*((midpoint(q1)+arrsize/2*N) -- (midpoint(q1)+arrsize/2*S)), red, Arrow(4));
+draw(
+ zigzag(v[1]-(0,vxsize/2)--v[1]-(0,vxsize/2)+7S),
+ red
+ );
+draw(v[1]-(0,vxsize/2)+7S --v[2]+(0,vxsize/2)+7N, red+Dotted);
+draw(
+ zigzag(v[2]+vxsize/2*N--v[2]+(vxsize/2+7)*N),
+ red
+ );
+path qjp1 = v[2]-(0,vxsize/2)--v[3]+(0,vxsize/2);
+draw(zigzag(qjp1), red);
+draw(Label("$q_{j+1}$", MidPoint, E), shift(arrdist*E)*((midpoint(qjp1)+arrsize/2*N) -- (midpoint(qjp1)+arrsize/2*S)), red, Arrow(4));
+draw(v[3]-(0,vxsize/2)+7S --v[4]+(0,vxsize/2)+7N, red+Dotted);
+draw(
+ zigzag(v[3]-(0,vxsize/2)--v[3]-(0,vxsize/2)+7S),
+ red
+ );
+draw(
+ zigzag(v[4]+(0,vxsize/2)+7N--v[4]+(0,vxsize/2)),
+ red
+ );
+path qn = v[4]-(0,vxsize/2)--v[5]+(0,vxsize/2);
+draw(zigzag(qn), red);
+draw(Label("$q_n$", MidPoint, E), shift(arrdist*E)*((midpoint(qn)+arrsize/2*N) -- (midpoint(qn)+arrsize/2*S)), red, Arrow(4));
+
+
+draw(gluon(v[1]+(vxsize/2,0)--(w,v[1].y)));
+filldraw(shift(v[1])*box,grey);
+path pH = v[2]+(vxsize/2,0)--(w,v[2].y);
+draw(pH, dashed);
+draw("$p_H$", shift(arrdist*S)*((midpoint(pH)+arrsize/2*W) -- (midpoint(pH)+arrsize/2*E)), Arrow(4));
+filldraw(shift(v[2])*triangle,green);
+draw(gluon(v[3]+(vxsize/2,0)--(w,v[3].y)));
+filldraw(shift(v[3])*box,grey);
+draw(gluon(v[4]+(vxsize/2,0)--(w,v[4].y)));
+filldraw(shift(v[4])*box,grey);
+
+label("$\Delta y_1$", (w, (v[0].y+v[1].y)/2), red);
+label("$\Delta y_{j+1}$", (w, (v[2].y+v[3].y)/2), red);
+label("$\Delta y_{n}$", (w, (v[4].y+v[5].y)/2), red);
+
+
+draw(rotate(90)*"Increasing rapidity", (1.8w,h)--(1.8w,-h),Arrow);
+
+filldraw(shift(0, h)*xscale(7)*box, blue);
+label("Current", (0,h+vxsize/2), N, blue);
+
+filldraw(shift(0, -h)*xscale(7)*box, blue);
diff --git a/doc/developer_manual/src/HEJ_peripheral_Higgs_amplitude.asy b/doc/developer_manual/src/HEJ_peripheral_Higgs_amplitude.asy
new file mode 100644
index 0000000..c9d685c
--- /dev/null
+++ b/doc/developer_manual/src/HEJ_peripheral_Higgs_amplitude.asy
@@ -0,0 +1,93 @@
+import feynman;
+usepackage("fourier");
+// usepackage("sansmathfonts");
+// texpreamble("\renewcommand{\familydefault}{\sfdefault}");
+
+defaultpen(fontsize(8));
+
+path zigzag(path g, real step=2, real distance=2) {
+ real len = arclength(g);
+ int state = 0;
+ path zig;
+ for (real u = 0; u < len; u += step) {
+ real t = arctime(g, u);
+ pair p = point(g, t);
+ pair norm = unit(rotate(90) * dir(g, t));
+ if (state == 1)
+ p = p + distance * norm;
+ else if (state == 3)
+ p = p - distance * norm;
+ zig = zig -- p;
+ state = (state + 1) % 4;
+ }
+ zig = zig -- point(g, length(g));
+ return zig;
+}
+
+real h = 80;
+real w = 60;
+real arrsize = 15;
+real arrdist = 7;
+real vxsize=7;
+
+pair[] v = {
+ (0,h), (0,h/3), (0,-h/3), (0,-h)
+};
+
+path box = scale(vxsize)*shift(SW/sqrt(2))*unitsquare;
+path triangle = scale(vxsize)*(E -- N/2 -- S/2 --cycle);
+
+path pa = (-w,h)--(-2*vxsize,h);
+draw(pa, currentpen+1);
+draw(gluon(pa));
+draw("$p_a$", shift(arrdist*S)*((midpoint(pa)+arrsize/2*W) -- (midpoint(pa)+arrsize/2*E)), Arrow(4));
+path p1 = (w,h)--(2*vxsize,h);
+draw(p1, currentpen+1);
+draw(gluon(p1));
+draw("$p_1$", shift(arrdist*S)*((midpoint(p1)+arrsize/2*W) -- (midpoint(p1)+arrsize/2*E)), Arrow(4));
+path pb = (-w,-h)--(-2*vxsize,-h);
+draw(pb, currentpen+1);
+draw(gluon(pb));
+draw(Label("$p_b$", MidPoint, N), shift(arrdist*N)*((midpoint(pb)+arrsize/2*W) -- (midpoint(pb)+arrsize/2*E)), Arrow(4));
+path pn = (w,-h)--(2*vxsize,-h);
+draw(pn, currentpen+1);
+draw(gluon(pn));
+draw(Label("$p_n$", MidPoint, N), shift(arrdist*N)*((midpoint(pn)+arrsize/2*W) -- (midpoint(pn)+arrsize/2*E)), Arrow(4));
+path q1 = v[0]-(0,vxsize/2)--v[1]+(0,vxsize/2);
+draw(zigzag(q1), red);
+draw(Label("$q_1$", MidPoint, E), shift(arrdist*E)*((midpoint(q1)+arrsize/2*N) -- (midpoint(q1)+arrsize/2*S)), red, Arrow(4));
+draw(
+ zigzag(v[1]-(0,vxsize/2)--v[1]-(0,vxsize/2)+7S),
+ red
+ );
+draw(v[1]-(0,vxsize/2)+7S --v[2]+(0,vxsize/2)+7N, red+Dotted);
+draw(
+ zigzag(v[2]+(0,vxsize/2)+7N--v[2]+(0,vxsize/2)),
+ red
+ );
+path qn = v[2]-(0,vxsize/2)--v[3]+(0,vxsize/2);
+draw(zigzag(qn), red);
+draw(Label("$q_{n-1}$", MidPoint, E), shift(arrdist*E)*((midpoint(qn)+arrsize/2*N) -- (midpoint(qn)+arrsize/2*S)), red, Arrow(4));
+
+
+draw(gluon(v[1]+(vxsize/2,0)--(w,v[1].y)));
+filldraw(shift(v[1])*box,grey);
+draw(gluon(v[2]+(vxsize/2,0)--(w,v[2].y)));
+filldraw(shift(v[2])*box,grey);
+
+draw(rotate(90)*"Increasing rapidity", (1.5w,h)--(1.5w,-h),Arrow);
+
+filldraw(shift(0, h)*xscale(7)*box, blue);
+
+filldraw(shift(0, -h)*xscale(7)*box, blue);
+
+path pH = (0,h)+vxsize/2*N -- (w,4/3*h);
+draw(pH, dashed);
+draw(
+ Label(rotate(degrees(dir(pH)))*"$p_H$", MidPoint, N),
+ shift(arrdist*(rotate(90)*dir(pH)))*
+ shift(midpoint(pH))*
+ rotate(degrees(dir(pH)))*
+ (arrdist*W--arrdist*E),
+ Arrow(4)
+ );
diff --git a/doc/doxygen/Doxyfile b/doc/doxygen/Doxyfile
index 25b5e53..b1df074 100644
--- a/doc/doxygen/Doxyfile
+++ b/doc/doxygen/Doxyfile
@@ -1,2427 +1,2427 @@
# Doxyfile 1.8.11
# This file describes the settings to be used by the documentation system
# doxygen (www.doxygen.org) for a project.
#
# All text after a double hash (##) is considered a comment and is placed in
# front of the TAG it is preceding.
#
# All text after a single hash (#) is considered a comment and will be ignored.
# The format is:
# TAG = value [value, ...]
# For lists, items can also be appended using:
# TAG += value [value, ...]
# Values that contain spaces should be placed between quotes (\" \").
#---------------------------------------------------------------------------
# Project related configuration options
#---------------------------------------------------------------------------
# This tag specifies the encoding used for all characters in the config file
# that follow. The default is UTF-8 which is also the encoding used for all text
# before the first occurrence of this tag. Doxygen uses libiconv (or the iconv
# built into libc) for the transcoding. See http://www.gnu.org/software/libiconv
# for the list of possible encodings.
# The default value is: UTF-8.
DOXYFILE_ENCODING = UTF-8
# The PROJECT_NAME tag is a single word (or a sequence of words surrounded by
# double-quotes, unless you are using Doxywizard) that should identify the
# project for which the documentation is generated. This name is used in the
# title of most generated pages and in a few other places.
# The default value is: My Project.
PROJECT_NAME = "HEJ 2"
# The PROJECT_NUMBER tag can be used to enter a project or revision number. This
# could be handy for archiving the generated documentation or if some version
# control system is used.
-PROJECT_NUMBER = "0.1"
+PROJECT_NUMBER = "2.0"
# Using the PROJECT_BRIEF tag one can provide an optional one line description
# for a project that appears at the top of each page and should give viewer a
# quick idea about the purpose of the project. Keep the description short.
PROJECT_BRIEF = "High energy resummation for hadron colliders"
# With the PROJECT_LOGO tag one can specify a logo or an icon that is included
# in the documentation. The maximum height of the logo should not exceed 55
# pixels and the maximum width should not exceed 200 pixels. Doxygen will copy
# the logo to the output directory.
PROJECT_LOGO =
# The OUTPUT_DIRECTORY tag is used to specify the (relative or absolute) path
# into which the generated documentation will be written. If a relative path is
# entered, it will be relative to the location where doxygen was started. If
# left blank the current directory will be used.
OUTPUT_DIRECTORY =
# If the CREATE_SUBDIRS tag is set to YES then doxygen will create 4096 sub-
# directories (in 2 levels) under the output directory of each output format and
# will distribute the generated files over these directories. Enabling this
# option can be useful when feeding doxygen a huge amount of source files, where
# putting all generated files in the same directory would otherwise causes
# performance problems for the file system.
# The default value is: NO.
CREATE_SUBDIRS = NO
# If the ALLOW_UNICODE_NAMES tag is set to YES, doxygen will allow non-ASCII
# characters to appear in the names of generated files. If set to NO, non-ASCII
# characters will be escaped, for example _xE3_x81_x84 will be used for Unicode
# U+3044.
# The default value is: NO.
ALLOW_UNICODE_NAMES = NO
# The OUTPUT_LANGUAGE tag is used to specify the language in which all
# documentation generated by doxygen is written. Doxygen will use this
# information to generate all constant output in the proper language.
# Possible values are: Afrikaans, Arabic, Armenian, Brazilian, Catalan, Chinese,
# Chinese-Traditional, Croatian, Czech, Danish, Dutch, English (United States),
# Esperanto, Farsi (Persian), Finnish, French, German, Greek, Hungarian,
# Indonesian, Italian, Japanese, Japanese-en (Japanese with English messages),
# Korean, Korean-en (Korean with English messages), Latvian, Lithuanian,
# Macedonian, Norwegian, Persian (Farsi), Polish, Portuguese, Romanian, Russian,
# Serbian, Serbian-Cyrillic, Slovak, Slovene, Spanish, Swedish, Turkish,
# Ukrainian and Vietnamese.
# The default value is: English.
OUTPUT_LANGUAGE = English
# If the BRIEF_MEMBER_DESC tag is set to YES, doxygen will include brief member
# descriptions after the members that are listed in the file and class
# documentation (similar to Javadoc). Set to NO to disable this.
# The default value is: YES.
BRIEF_MEMBER_DESC = YES
# If the REPEAT_BRIEF tag is set to YES, doxygen will prepend the brief
# description of a member or function before the detailed description
#
# Note: If both HIDE_UNDOC_MEMBERS and BRIEF_MEMBER_DESC are set to NO, the
# brief descriptions will be completely suppressed.
# The default value is: YES.
REPEAT_BRIEF = YES
# This tag implements a quasi-intelligent brief description abbreviator that is
# used to form the text in various listings. Each string in this list, if found
# as the leading text of the brief description, will be stripped from the text
# and the result, after processing the whole list, is used as the annotated
# text. Otherwise, the brief description is used as-is. If left blank, the
# following values are used ($name is automatically replaced with the name of
# the entity):The $name class, The $name widget, The $name file, is, provides,
# specifies, contains, represents, a, an and the.
ABBREVIATE_BRIEF =
# If the ALWAYS_DETAILED_SEC and REPEAT_BRIEF tags are both set to YES then
# doxygen will generate a detailed section even if there is only a brief
# description.
# The default value is: NO.
ALWAYS_DETAILED_SEC = NO
# If the INLINE_INHERITED_MEMB tag is set to YES, doxygen will show all
# inherited members of a class in the documentation of that class as if those
# members were ordinary class members. Constructors, destructors and assignment
# operators of the base classes will not be shown.
# The default value is: NO.
INLINE_INHERITED_MEMB = NO
# If the FULL_PATH_NAMES tag is set to YES, doxygen will prepend the full path
# before files name in the file list and in the header files. If set to NO the
# shortest path that makes the file name unique will be used
# The default value is: YES.
FULL_PATH_NAMES = YES
# The STRIP_FROM_PATH tag can be used to strip a user-defined part of the path.
# Stripping is only done if one of the specified strings matches the left-hand
# part of the path. The tag can be used to show relative paths in the file list.
# If left blank the directory from which doxygen is run is used as the path to
# strip.
#
# Note that you can specify absolute paths here, but also relative paths, which
# will be relative from the directory where doxygen is started.
# This tag requires that the tag FULL_PATH_NAMES is set to YES.
STRIP_FROM_PATH =
# The STRIP_FROM_INC_PATH tag can be used to strip a user-defined part of the
# path mentioned in the documentation of a class, which tells the reader which
# header file to include in order to use a class. If left blank only the name of
# the header file containing the class definition is used. Otherwise one should
# specify the list of include paths that are normally passed to the compiler
# using the -I flag.
STRIP_FROM_INC_PATH =
# If the SHORT_NAMES tag is set to YES, doxygen will generate much shorter (but
# less readable) file names. This can be useful is your file systems doesn't
# support long names like on DOS, Mac, or CD-ROM.
# The default value is: NO.
SHORT_NAMES = NO
# If the JAVADOC_AUTOBRIEF tag is set to YES then doxygen will interpret the
# first line (until the first dot) of a Javadoc-style comment as the brief
# description. If set to NO, the Javadoc-style will behave just like regular Qt-
# style comments (thus requiring an explicit @brief command for a brief
# description.)
# The default value is: NO.
JAVADOC_AUTOBRIEF = NO
# If the QT_AUTOBRIEF tag is set to YES then doxygen will interpret the first
# line (until the first dot) of a Qt-style comment as the brief description. If
# set to NO, the Qt-style will behave just like regular Qt-style comments (thus
# requiring an explicit \brief command for a brief description.)
# The default value is: NO.
QT_AUTOBRIEF = NO
# The MULTILINE_CPP_IS_BRIEF tag can be set to YES to make doxygen treat a
# multi-line C++ special comment block (i.e. a block of //! or /// comments) as
# a brief description. This used to be the default behavior. The new default is
# to treat a multi-line C++ comment block as a detailed description. Set this
# tag to YES if you prefer the old behavior instead.
#
# Note that setting this tag to YES also means that rational rose comments are
# not recognized any more.
# The default value is: NO.
MULTILINE_CPP_IS_BRIEF = NO
# If the INHERIT_DOCS tag is set to YES then an undocumented member inherits the
# documentation from any documented member that it re-implements.
# The default value is: YES.
INHERIT_DOCS = YES
# If the SEPARATE_MEMBER_PAGES tag is set to YES then doxygen will produce a new
# page for each member. If set to NO, the documentation of a member will be part
# of the file/class/namespace that contains it.
# The default value is: NO.
SEPARATE_MEMBER_PAGES = NO
# The TAB_SIZE tag can be used to set the number of spaces in a tab. Doxygen
# uses this value to replace tabs by spaces in code fragments.
# Minimum value: 1, maximum value: 16, default value: 4.
TAB_SIZE = 4
# This tag can be used to specify a number of aliases that act as commands in
# the documentation. An alias has the form:
# name=value
# For example adding
# "sideeffect=@par Side Effects:\n"
# will allow you to put the command \sideeffect (or @sideeffect) in the
# documentation, which will result in a user-defined paragraph with heading
# "Side Effects:". You can put \n's in the value part of an alias to insert
# newlines.
ALIASES += TODO="\todo"
# This tag can be used to specify a number of word-keyword mappings (TCL only).
# A mapping has the form "name=value". For example adding "class=itcl::class"
# will allow you to use the command class in the itcl::class meaning.
TCL_SUBST =
# Set the OPTIMIZE_OUTPUT_FOR_C tag to YES if your project consists of C sources
# only. Doxygen will then generate output that is more tailored for C. For
# instance, some of the names that are used will be different. The list of all
# members will be omitted, etc.
# The default value is: NO.
OPTIMIZE_OUTPUT_FOR_C = NO
# Set the OPTIMIZE_OUTPUT_JAVA tag to YES if your project consists of Java or
# Python sources only. Doxygen will then generate output that is more tailored
# for that language. For instance, namespaces will be presented as packages,
# qualified scopes will look different, etc.
# The default value is: NO.
OPTIMIZE_OUTPUT_JAVA = NO
# Set the OPTIMIZE_FOR_FORTRAN tag to YES if your project consists of Fortran
# sources. Doxygen will then generate output that is tailored for Fortran.
# The default value is: NO.
OPTIMIZE_FOR_FORTRAN = NO
# Set the OPTIMIZE_OUTPUT_VHDL tag to YES if your project consists of VHDL
# sources. Doxygen will then generate output that is tailored for VHDL.
# The default value is: NO.
OPTIMIZE_OUTPUT_VHDL = NO
# Doxygen selects the parser to use depending on the extension of the files it
# parses. With this tag you can assign which parser to use for a given
# extension. Doxygen has a built-in mapping, but you can override or extend it
# using this tag. The format is ext=language, where ext is a file extension, and
# language is one of the parsers supported by doxygen: IDL, Java, Javascript,
# C#, C, C++, D, PHP, Objective-C, Python, Fortran (fixed format Fortran:
# FortranFixed, free formatted Fortran: FortranFree, unknown formatted Fortran:
# Fortran. In the later case the parser tries to guess whether the code is fixed
# or free formatted code, this is the default for Fortran type files), VHDL. For
# instance to make doxygen treat .inc files as Fortran files (default is PHP),
# and .f files as C (default is Fortran), use: inc=Fortran f=C.
#
# Note: For files without extension you can use no_extension as a placeholder.
#
# Note that for custom extensions you also need to set FILE_PATTERNS otherwise
# the files are not read by doxygen.
EXTENSION_MAPPING =
# If the MARKDOWN_SUPPORT tag is enabled then doxygen pre-processes all comments
# according to the Markdown format, which allows for more readable
# documentation. See http://daringfireball.net/projects/markdown/ for details.
# The output of markdown processing is further processed by doxygen, so you can
# mix doxygen, HTML, and XML commands with Markdown formatting. Disable only in
# case of backward compatibilities issues.
# The default value is: YES.
MARKDOWN_SUPPORT = YES
# When enabled doxygen tries to link words that correspond to documented
# classes, or namespaces to their corresponding documentation. Such a link can
# be prevented in individual cases by putting a % sign in front of the word or
# globally by setting AUTOLINK_SUPPORT to NO.
# The default value is: YES.
AUTOLINK_SUPPORT = YES
# If you use STL classes (i.e. std::string, std::vector, etc.) but do not want
# to include (a tag file for) the STL sources as input, then you should set this
# tag to YES in order to let doxygen match functions declarations and
# definitions whose arguments contain STL classes (e.g. func(std::string);
# versus func(std::string) {}). This also make the inheritance and collaboration
# diagrams that involve STL classes more complete and accurate.
# The default value is: NO.
BUILTIN_STL_SUPPORT = NO
# If you use Microsoft's C++/CLI language, you should set this option to YES to
# enable parsing support.
# The default value is: NO.
CPP_CLI_SUPPORT = NO
# Set the SIP_SUPPORT tag to YES if your project consists of sip (see:
# http://www.riverbankcomputing.co.uk/software/sip/intro) sources only. Doxygen
# will parse them like normal C++ but will assume all classes use public instead
# of private inheritance when no explicit protection keyword is present.
# The default value is: NO.
SIP_SUPPORT = NO
# For Microsoft's IDL there are propget and propput attributes to indicate
# getter and setter methods for a property. Setting this option to YES will make
# doxygen to replace the get and set methods by a property in the documentation.
# This will only work if the methods are indeed getting or setting a simple
# type. If this is not the case, or you want to show the methods anyway, you
# should set this option to NO.
# The default value is: YES.
IDL_PROPERTY_SUPPORT = YES
# If member grouping is used in the documentation and the DISTRIBUTE_GROUP_DOC
# tag is set to YES then doxygen will reuse the documentation of the first
# member in the group (if any) for the other members of the group. By default
# all members of a group must be documented explicitly.
# The default value is: NO.
DISTRIBUTE_GROUP_DOC = NO
# If one adds a struct or class to a group and this option is enabled, then also
# any nested class or struct is added to the same group. By default this option
# is disabled and one has to add nested compounds explicitly via \ingroup.
# The default value is: NO.
GROUP_NESTED_COMPOUNDS = NO
# Set the SUBGROUPING tag to YES to allow class member groups of the same type
# (for instance a group of public functions) to be put as a subgroup of that
# type (e.g. under the Public Functions section). Set it to NO to prevent
# subgrouping. Alternatively, this can be done per class using the
# \nosubgrouping command.
# The default value is: YES.
SUBGROUPING = YES
# When the INLINE_GROUPED_CLASSES tag is set to YES, classes, structs and unions
# are shown inside the group in which they are included (e.g. using \ingroup)
# instead of on a separate page (for HTML and Man pages) or section (for LaTeX
# and RTF).
#
# Note that this feature does not work in combination with
# SEPARATE_MEMBER_PAGES.
# The default value is: NO.
INLINE_GROUPED_CLASSES = NO
# When the INLINE_SIMPLE_STRUCTS tag is set to YES, structs, classes, and unions
# with only public data fields or simple typedef fields will be shown inline in
# the documentation of the scope in which they are defined (i.e. file,
# namespace, or group documentation), provided this scope is documented. If set
# to NO, structs, classes, and unions are shown on a separate page (for HTML and
# Man pages) or section (for LaTeX and RTF).
# The default value is: NO.
INLINE_SIMPLE_STRUCTS = NO
# When TYPEDEF_HIDES_STRUCT tag is enabled, a typedef of a struct, union, or
# enum is documented as struct, union, or enum with the name of the typedef. So
# typedef struct TypeS {} TypeT, will appear in the documentation as a struct
# with name TypeT. When disabled the typedef will appear as a member of a file,
# namespace, or class. And the struct will be named TypeS. This can typically be
# useful for C code in case the coding convention dictates that all compound
# types are typedef'ed and only the typedef is referenced, never the tag name.
# The default value is: NO.
TYPEDEF_HIDES_STRUCT = NO
# The size of the symbol lookup cache can be set using LOOKUP_CACHE_SIZE. This
# cache is used to resolve symbols given their name and scope. Since this can be
# an expensive process and often the same symbol appears multiple times in the
# code, doxygen keeps a cache of pre-resolved symbols. If the cache is too small
# doxygen will become slower. If the cache is too large, memory is wasted. The
# cache size is given by this formula: 2^(16+LOOKUP_CACHE_SIZE). The valid range
# is 0..9, the default is 0, corresponding to a cache size of 2^16=65536
# symbols. At the end of a run doxygen will report the cache usage and suggest
# the optimal cache size from a speed point of view.
# Minimum value: 0, maximum value: 9, default value: 0.
LOOKUP_CACHE_SIZE = 0
#---------------------------------------------------------------------------
# Build related configuration options
#---------------------------------------------------------------------------
# If the EXTRACT_ALL tag is set to YES, doxygen will assume all entities in
# documentation are documented, even if no documentation was available. Private
# class members and static file members will be hidden unless the
# EXTRACT_PRIVATE respectively EXTRACT_STATIC tags are set to YES.
# Note: This will also disable the warnings about undocumented members that are
# normally produced when WARNINGS is set to YES.
# The default value is: NO.
EXTRACT_ALL = YES
# If the EXTRACT_PRIVATE tag is set to YES, all private members of a class will
# be included in the documentation.
# The default value is: NO.
EXTRACT_PRIVATE = NO
# If the EXTRACT_PACKAGE tag is set to YES, all members with package or internal
# scope will be included in the documentation.
# The default value is: NO.
EXTRACT_PACKAGE = NO
# If the EXTRACT_STATIC tag is set to YES, all static members of a file will be
# included in the documentation.
# The default value is: NO.
EXTRACT_STATIC = NO
# If the EXTRACT_LOCAL_CLASSES tag is set to YES, classes (and structs) defined
# locally in source files will be included in the documentation. If set to NO,
# only classes defined in header files are included. Does not have any effect
# for Java sources.
# The default value is: YES.
EXTRACT_LOCAL_CLASSES = YES
# This flag is only useful for Objective-C code. If set to YES, local methods,
# which are defined in the implementation section but not in the interface are
# included in the documentation. If set to NO, only methods in the interface are
# included.
# The default value is: NO.
EXTRACT_LOCAL_METHODS = NO
# If this flag is set to YES, the members of anonymous namespaces will be
# extracted and appear in the documentation as a namespace called
# 'anonymous_namespace{file}', where file will be replaced with the base name of
# the file that contains the anonymous namespace. By default anonymous namespace
# are hidden.
# The default value is: NO.
EXTRACT_ANON_NSPACES = NO
# If the HIDE_UNDOC_MEMBERS tag is set to YES, doxygen will hide all
# undocumented members inside documented classes or files. If set to NO these
# members will be included in the various overviews, but no documentation
# section is generated. This option has no effect if EXTRACT_ALL is enabled.
# The default value is: NO.
HIDE_UNDOC_MEMBERS = NO
# If the HIDE_UNDOC_CLASSES tag is set to YES, doxygen will hide all
# undocumented classes that are normally visible in the class hierarchy. If set
# to NO, these classes will be included in the various overviews. This option
# has no effect if EXTRACT_ALL is enabled.
# The default value is: NO.
HIDE_UNDOC_CLASSES = NO
# If the HIDE_FRIEND_COMPOUNDS tag is set to YES, doxygen will hide all friend
# (class|struct|union) declarations. If set to NO, these declarations will be
# included in the documentation.
# The default value is: NO.
HIDE_FRIEND_COMPOUNDS = NO
# If the HIDE_IN_BODY_DOCS tag is set to YES, doxygen will hide any
# documentation blocks found inside the body of a function. If set to NO, these
# blocks will be appended to the function's detailed documentation block.
# The default value is: NO.
HIDE_IN_BODY_DOCS = NO
# The INTERNAL_DOCS tag determines if documentation that is typed after a
# \internal command is included. If the tag is set to NO then the documentation
# will be excluded. Set it to YES to include the internal documentation.
# The default value is: NO.
INTERNAL_DOCS = NO
# If the CASE_SENSE_NAMES tag is set to NO then doxygen will only generate file
# names in lower-case letters. If set to YES, upper-case letters are also
# allowed. This is useful if you have classes or files whose names only differ
# in case and if your file system supports case sensitive file names. Windows
# and Mac users are advised to set this option to NO.
# The default value is: system dependent.
CASE_SENSE_NAMES = YES
# If the HIDE_SCOPE_NAMES tag is set to NO then doxygen will show members with
# their full class and namespace scopes in the documentation. If set to YES, the
# scope will be hidden.
# The default value is: NO.
HIDE_SCOPE_NAMES = NO
# If the HIDE_COMPOUND_REFERENCE tag is set to NO (default) then doxygen will
# append additional text to a page's title, such as Class Reference. If set to
# YES the compound reference will be hidden.
# The default value is: NO.
HIDE_COMPOUND_REFERENCE= NO
# If the SHOW_INCLUDE_FILES tag is set to YES then doxygen will put a list of
# the files that are included by a file in the documentation of that file.
# The default value is: YES.
SHOW_INCLUDE_FILES = YES
# If the SHOW_GROUPED_MEMB_INC tag is set to YES then Doxygen will add for each
# grouped member an include statement to the documentation, telling the reader
# which file to include in order to use the member.
# The default value is: NO.
SHOW_GROUPED_MEMB_INC = NO
# If the FORCE_LOCAL_INCLUDES tag is set to YES then doxygen will list include
# files with double quotes in the documentation rather than with sharp brackets.
# The default value is: NO.
FORCE_LOCAL_INCLUDES = NO
# If the INLINE_INFO tag is set to YES then a tag [inline] is inserted in the
# documentation for inline members.
# The default value is: YES.
INLINE_INFO = YES
# If the SORT_MEMBER_DOCS tag is set to YES then doxygen will sort the
# (detailed) documentation of file and class members alphabetically by member
# name. If set to NO, the members will appear in declaration order.
# The default value is: YES.
SORT_MEMBER_DOCS = YES
# If the SORT_BRIEF_DOCS tag is set to YES then doxygen will sort the brief
# descriptions of file, namespace and class members alphabetically by member
# name. If set to NO, the members will appear in declaration order. Note that
# this will also influence the order of the classes in the class list.
# The default value is: NO.
SORT_BRIEF_DOCS = NO
# If the SORT_MEMBERS_CTORS_1ST tag is set to YES then doxygen will sort the
# (brief and detailed) documentation of class members so that constructors and
# destructors are listed first. If set to NO the constructors will appear in the
# respective orders defined by SORT_BRIEF_DOCS and SORT_MEMBER_DOCS.
# Note: If SORT_BRIEF_DOCS is set to NO this option is ignored for sorting brief
# member documentation.
# Note: If SORT_MEMBER_DOCS is set to NO this option is ignored for sorting
# detailed member documentation.
# The default value is: NO.
SORT_MEMBERS_CTORS_1ST = NO
# If the SORT_GROUP_NAMES tag is set to YES then doxygen will sort the hierarchy
# of group names into alphabetical order. If set to NO the group names will
# appear in their defined order.
# The default value is: NO.
SORT_GROUP_NAMES = NO
# If the SORT_BY_SCOPE_NAME tag is set to YES, the class list will be sorted by
# fully-qualified names, including namespaces. If set to NO, the class list will
# be sorted only by class name, not including the namespace part.
# Note: This option is not very useful if HIDE_SCOPE_NAMES is set to YES.
# Note: This option applies only to the class list, not to the alphabetical
# list.
# The default value is: NO.
SORT_BY_SCOPE_NAME = NO
# If the STRICT_PROTO_MATCHING option is enabled and doxygen fails to do proper
# type resolution of all parameters of a function it will reject a match between
# the prototype and the implementation of a member function even if there is
# only one candidate or it is obvious which candidate to choose by doing a
# simple string match. By disabling STRICT_PROTO_MATCHING doxygen will still
# accept a match between prototype and implementation in such cases.
# The default value is: NO.
STRICT_PROTO_MATCHING = NO
# The GENERATE_TODOLIST tag can be used to enable (YES) or disable (NO) the todo
# list. This list is created by putting \todo commands in the documentation.
# The default value is: YES.
GENERATE_TODOLIST = YES
# The GENERATE_TESTLIST tag can be used to enable (YES) or disable (NO) the test
# list. This list is created by putting \test commands in the documentation.
# The default value is: YES.
GENERATE_TESTLIST = YES
# The GENERATE_BUGLIST tag can be used to enable (YES) or disable (NO) the bug
# list. This list is created by putting \bug commands in the documentation.
# The default value is: YES.
GENERATE_BUGLIST = YES
# The GENERATE_DEPRECATEDLIST tag can be used to enable (YES) or disable (NO)
# the deprecated list. This list is created by putting \deprecated commands in
# the documentation.
# The default value is: YES.
GENERATE_DEPRECATEDLIST= YES
# The ENABLED_SECTIONS tag can be used to enable conditional documentation
# sections, marked by \if <section_label> ... \endif and \cond <section_label>
# ... \endcond blocks.
ENABLED_SECTIONS =
# The MAX_INITIALIZER_LINES tag determines the maximum number of lines that the
# initial value of a variable or macro / define can have for it to appear in the
# documentation. If the initializer consists of more lines than specified here
# it will be hidden. Use a value of 0 to hide initializers completely. The
# appearance of the value of individual variables and macros / defines can be
# controlled using \showinitializer or \hideinitializer command in the
# documentation regardless of this setting.
# Minimum value: 0, maximum value: 10000, default value: 30.
MAX_INITIALIZER_LINES = 30
# Set the SHOW_USED_FILES tag to NO to disable the list of files generated at
# the bottom of the documentation of classes and structs. If set to YES, the
# list will mention the files that were used to generate the documentation.
# The default value is: YES.
SHOW_USED_FILES = YES
# Set the SHOW_FILES tag to NO to disable the generation of the Files page. This
# will remove the Files entry from the Quick Index and from the Folder Tree View
# (if specified).
# The default value is: YES.
SHOW_FILES = YES
# Set the SHOW_NAMESPACES tag to NO to disable the generation of the Namespaces
# page. This will remove the Namespaces entry from the Quick Index and from the
# Folder Tree View (if specified).
# The default value is: YES.
SHOW_NAMESPACES = YES
# The FILE_VERSION_FILTER tag can be used to specify a program or script that
# doxygen should invoke to get the current version for each file (typically from
# the version control system). Doxygen will invoke the program by executing (via
# popen()) the command command input-file, where command is the value of the
# FILE_VERSION_FILTER tag, and input-file is the name of an input file provided
# by doxygen. Whatever the program writes to standard output is used as the file
# version. For an example see the documentation.
FILE_VERSION_FILTER =
# The LAYOUT_FILE tag can be used to specify a layout file which will be parsed
# by doxygen. The layout file controls the global structure of the generated
# output files in an output format independent way. To create the layout file
# that represents doxygen's defaults, run doxygen with the -l option. You can
# optionally specify a file name after the option, if omitted DoxygenLayout.xml
# will be used as the name of the layout file.
#
# Note that if you run doxygen from a directory containing a file called
# DoxygenLayout.xml, doxygen will parse it automatically even if the LAYOUT_FILE
# tag is left empty.
LAYOUT_FILE =
# The CITE_BIB_FILES tag can be used to specify one or more bib files containing
# the reference definitions. This must be a list of .bib files. The .bib
# extension is automatically appended if omitted. This requires the bibtex tool
# to be installed. See also http://en.wikipedia.org/wiki/BibTeX for more info.
# For LaTeX the style of the bibliography can be controlled using
# LATEX_BIB_STYLE. To use this feature you need bibtex and perl available in the
# search path. See also \cite for info how to create references.
CITE_BIB_FILES = biblio.bib
#---------------------------------------------------------------------------
# Configuration options related to warning and progress messages
#---------------------------------------------------------------------------
# The QUIET tag can be used to turn on/off the messages that are generated to
# standard output by doxygen. If QUIET is set to YES this implies that the
# messages are off.
# The default value is: NO.
QUIET = NO
# The WARNINGS tag can be used to turn on/off the warning messages that are
# generated to standard error (stderr) by doxygen. If WARNINGS is set to YES
# this implies that the warnings are on.
#
# Tip: Turn warnings on while writing the documentation.
# The default value is: YES.
WARNINGS = YES
# If the WARN_IF_UNDOCUMENTED tag is set to YES then doxygen will generate
# warnings for undocumented members. If EXTRACT_ALL is set to YES then this flag
# will automatically be disabled.
# The default value is: YES.
WARN_IF_UNDOCUMENTED = YES
# If the WARN_IF_DOC_ERROR tag is set to YES, doxygen will generate warnings for
# potential errors in the documentation, such as not documenting some parameters
# in a documented function, or documenting parameters that don't exist or using
# markup commands wrongly.
# The default value is: YES.
WARN_IF_DOC_ERROR = YES
# This WARN_NO_PARAMDOC option can be enabled to get warnings for functions that
# are documented, but have no documentation for their parameters or return
# value. If set to NO, doxygen will only warn about wrong or incomplete
# parameter documentation, but not about the absence of documentation.
# The default value is: NO.
WARN_NO_PARAMDOC = NO
# If the WARN_AS_ERROR tag is set to YES then doxygen will immediately stop when
# a warning is encountered.
# The default value is: NO.
WARN_AS_ERROR = NO
# The WARN_FORMAT tag determines the format of the warning messages that doxygen
# can produce. The string should contain the $file, $line, and $text tags, which
# will be replaced by the file and line number from which the warning originated
# and the warning text. Optionally the format may contain $version, which will
# be replaced by the version of the file (if it could be obtained via
# FILE_VERSION_FILTER)
# The default value is: $file:$line: $text.
WARN_FORMAT = "$file:$line: $text"
# The WARN_LOGFILE tag can be used to specify a file to which warning and error
# messages should be written. If left blank the output is written to standard
# error (stderr).
WARN_LOGFILE =
#---------------------------------------------------------------------------
# Configuration options related to the input files
#---------------------------------------------------------------------------
# The INPUT tag is used to specify the files and/or directories that contain
# documented source files. You may enter file names like myfile.cpp or
# directories like /usr/src/myproject. Separate the files or directories with
# spaces. See also FILE_PATTERNS and EXTENSION_MAPPING
# Note: If this tag is empty the current directory is searched.
INPUT = mainpage.dox "../../include/HEJ"
# This tag can be used to specify the character encoding of the source files
# that doxygen parses. Internally doxygen uses the UTF-8 encoding. Doxygen uses
# libiconv (or the iconv built into libc) for the transcoding. See the libiconv
# documentation (see: http://www.gnu.org/software/libiconv) for the list of
# possible encodings.
# The default value is: UTF-8.
INPUT_ENCODING = UTF-8
# If the value of the INPUT tag contains directories, you can use the
# FILE_PATTERNS tag to specify one or more wildcard patterns (like *.cpp and
# *.h) to filter out the source-files in the directories.
#
# Note that for custom extensions or not directly supported extensions you also
# need to set EXTENSION_MAPPING for the extension otherwise the files are not
# read by doxygen.
#
# If left blank the following patterns are tested:*.c, *.cc, *.cxx, *.cpp,
# *.c++, *.java, *.ii, *.ixx, *.ipp, *.i++, *.inl, *.idl, *.ddl, *.odl, *.h,
# *.hh, *.hxx, *.hpp, *.h++, *.cs, *.d, *.php, *.php4, *.php5, *.phtml, *.inc,
# *.m, *.markdown, *.md, *.mm, *.dox, *.py, *.pyw, *.f90, *.f, *.for, *.tcl,
# *.vhd, *.vhdl, *.ucf, *.qsf, *.as and *.js.
FILE_PATTERNS =
# The RECURSIVE tag can be used to specify whether or not subdirectories should
# be searched for input files as well.
# The default value is: NO.
RECURSIVE = YES
# The EXCLUDE tag can be used to specify files and/or directories that should be
# excluded from the INPUT source files. This way you can easily exclude a
# subdirectory from a directory tree whose root is specified with the INPUT tag.
#
# Note that relative paths are relative to the directory from which doxygen is
# run.
EXCLUDE =
# The EXCLUDE_SYMLINKS tag can be used to select whether or not files or
# directories that are symbolic links (a Unix file system feature) are excluded
# from the input.
# The default value is: NO.
EXCLUDE_SYMLINKS = NO
# If the value of the INPUT tag contains directories, you can use the
# EXCLUDE_PATTERNS tag to specify one or more wildcard patterns to exclude
# certain files from those directories.
#
# Note that the wildcards are matched against the file with absolute path, so to
# exclude all test directories for example use the pattern */test/*
EXCLUDE_PATTERNS =
# The EXCLUDE_SYMBOLS tag can be used to specify one or more symbol names
# (namespaces, classes, functions, etc.) that should be excluded from the
# output. The symbol name can be a fully qualified name, a word, or if the
# wildcard * is used, a substring. Examples: ANamespace, AClass,
# AClass::ANamespace, ANamespace::*Test
#
# Note that the wildcards are matched against the file with absolute path, so to
# exclude all test directories use the pattern */test/*
EXCLUDE_SYMBOLS =
# The EXAMPLE_PATH tag can be used to specify one or more files or directories
# that contain example code fragments that are included (see the \include
# command).
EXAMPLE_PATH =
# If the value of the EXAMPLE_PATH tag contains directories, you can use the
# EXAMPLE_PATTERNS tag to specify one or more wildcard pattern (like *.cpp and
# *.h) to filter out the source-files in the directories. If left blank all
# files are included.
EXAMPLE_PATTERNS =
# If the EXAMPLE_RECURSIVE tag is set to YES then subdirectories will be
# searched for input files to be used with the \include or \dontinclude commands
# irrespective of the value of the RECURSIVE tag.
# The default value is: NO.
EXAMPLE_RECURSIVE = NO
# The IMAGE_PATH tag can be used to specify one or more files or directories
# that contain images that are to be included in the documentation (see the
# \image command).
IMAGE_PATH =
# The INPUT_FILTER tag can be used to specify a program that doxygen should
# invoke to filter for each input file. Doxygen will invoke the filter program
# by executing (via popen()) the command:
#
# <filter> <input-file>
#
# where <filter> is the value of the INPUT_FILTER tag, and <input-file> is the
# name of an input file. Doxygen will then use the output that the filter
# program writes to standard output. If FILTER_PATTERNS is specified, this tag
# will be ignored.
#
# Note that the filter must not add or remove lines; it is applied before the
# code is scanned, but not when the output code is generated. If lines are added
# or removed, the anchors will not be placed correctly.
#
# Note that for custom extensions or not directly supported extensions you also
# need to set EXTENSION_MAPPING for the extension otherwise the files are not
# properly processed by doxygen.
INPUT_FILTER =
# The FILTER_PATTERNS tag can be used to specify filters on a per file pattern
# basis. Doxygen will compare the file name with each pattern and apply the
# filter if there is a match. The filters are a list of the form: pattern=filter
# (like *.cpp=my_cpp_filter). See INPUT_FILTER for further information on how
# filters are used. If the FILTER_PATTERNS tag is empty or if none of the
# patterns match the file name, INPUT_FILTER is applied.
#
# Note that for custom extensions or not directly supported extensions you also
# need to set EXTENSION_MAPPING for the extension otherwise the files are not
# properly processed by doxygen.
FILTER_PATTERNS =
# If the FILTER_SOURCE_FILES tag is set to YES, the input filter (if set using
# INPUT_FILTER) will also be used to filter the input files that are used for
# producing the source files to browse (i.e. when SOURCE_BROWSER is set to YES).
# The default value is: NO.
FILTER_SOURCE_FILES = NO
# The FILTER_SOURCE_PATTERNS tag can be used to specify source filters per file
# pattern. A pattern will override the setting for FILTER_PATTERN (if any) and
# it is also possible to disable source filtering for a specific pattern using
# *.ext= (so without naming a filter).
# This tag requires that the tag FILTER_SOURCE_FILES is set to YES.
FILTER_SOURCE_PATTERNS =
# If the USE_MDFILE_AS_MAINPAGE tag refers to the name of a markdown file that
# is part of the input, its contents will be placed on the main page
# (index.html). This can be useful if you have a project on for instance GitHub
# and want to reuse the introduction page also for the doxygen output.
USE_MDFILE_AS_MAINPAGE =
#---------------------------------------------------------------------------
# Configuration options related to source browsing
#---------------------------------------------------------------------------
# If the SOURCE_BROWSER tag is set to YES then a list of source files will be
# generated. Documented entities will be cross-referenced with these sources.
#
# Note: To get rid of all source code in the generated output, make sure that
# also VERBATIM_HEADERS is set to NO.
# The default value is: NO.
SOURCE_BROWSER = NO
# Setting the INLINE_SOURCES tag to YES will include the body of functions,
# classes and enums directly into the documentation.
# The default value is: NO.
INLINE_SOURCES = NO
# Setting the STRIP_CODE_COMMENTS tag to YES will instruct doxygen to hide any
# special comment blocks from generated source code fragments. Normal C, C++ and
# Fortran comments will always remain visible.
# The default value is: YES.
STRIP_CODE_COMMENTS = YES
# If the REFERENCED_BY_RELATION tag is set to YES then for each documented
# function all documented functions referencing it will be listed.
# The default value is: NO.
REFERENCED_BY_RELATION = NO
# If the REFERENCES_RELATION tag is set to YES then for each documented function
# all documented entities called/used by that function will be listed.
# The default value is: NO.
REFERENCES_RELATION = NO
# If the REFERENCES_LINK_SOURCE tag is set to YES and SOURCE_BROWSER tag is set
# to YES then the hyperlinks from functions in REFERENCES_RELATION and
# REFERENCED_BY_RELATION lists will link to the source code. Otherwise they will
# link to the documentation.
# The default value is: YES.
REFERENCES_LINK_SOURCE = YES
# If SOURCE_TOOLTIPS is enabled (the default) then hovering a hyperlink in the
# source code will show a tooltip with additional information such as prototype,
# brief description and links to the definition and documentation. Since this
# will make the HTML file larger and loading of large files a bit slower, you
# can opt to disable this feature.
# The default value is: YES.
# This tag requires that the tag SOURCE_BROWSER is set to YES.
SOURCE_TOOLTIPS = YES
# If the USE_HTAGS tag is set to YES then the references to source code will
# point to the HTML generated by the htags(1) tool instead of doxygen built-in
# source browser. The htags tool is part of GNU's global source tagging system
# (see http://www.gnu.org/software/global/global.html). You will need version
# 4.8.6 or higher.
#
# To use it do the following:
# - Install the latest version of global
# - Enable SOURCE_BROWSER and USE_HTAGS in the config file
# - Make sure the INPUT points to the root of the source tree
# - Run doxygen as normal
#
# Doxygen will invoke htags (and that will in turn invoke gtags), so these
# tools must be available from the command line (i.e. in the search path).
#
# The result: instead of the source browser generated by doxygen, the links to
# source code will now point to the output of htags.
# The default value is: NO.
# This tag requires that the tag SOURCE_BROWSER is set to YES.
USE_HTAGS = NO
# If the VERBATIM_HEADERS tag is set the YES then doxygen will generate a
# verbatim copy of the header file for each class for which an include is
# specified. Set to NO to disable this.
# See also: Section \class.
# The default value is: YES.
VERBATIM_HEADERS = YES
# If the CLANG_ASSISTED_PARSING tag is set to YES then doxygen will use the
# clang parser (see: http://clang.llvm.org/) for more accurate parsing at the
# cost of reduced performance. This can be particularly helpful with template
# rich C++ code for which doxygen's built-in parser lacks the necessary type
# information.
# Note: The availability of this option depends on whether or not doxygen was
# generated with the -Duse-libclang=ON option for CMake.
# The default value is: NO.
CLANG_ASSISTED_PARSING = NO
# If clang assisted parsing is enabled you can provide the compiler with command
# line options that you would normally use when invoking the compiler. Note that
# the include paths will already be set by doxygen for the files and directories
# specified with INPUT and INCLUDE_PATH.
# This tag requires that the tag CLANG_ASSISTED_PARSING is set to YES.
CLANG_OPTIONS =
#---------------------------------------------------------------------------
# Configuration options related to the alphabetical class index
#---------------------------------------------------------------------------
# If the ALPHABETICAL_INDEX tag is set to YES, an alphabetical index of all
# compounds will be generated. Enable this if the project contains a lot of
# classes, structs, unions or interfaces.
# The default value is: YES.
ALPHABETICAL_INDEX = YES
# The COLS_IN_ALPHA_INDEX tag can be used to specify the number of columns in
# which the alphabetical index list will be split.
# Minimum value: 1, maximum value: 20, default value: 5.
# This tag requires that the tag ALPHABETICAL_INDEX is set to YES.
COLS_IN_ALPHA_INDEX = 5
# In case all classes in a project start with a common prefix, all classes will
# be put under the same header in the alphabetical index. The IGNORE_PREFIX tag
# can be used to specify a prefix (or a list of prefixes) that should be ignored
# while generating the index headers.
# This tag requires that the tag ALPHABETICAL_INDEX is set to YES.
IGNORE_PREFIX =
#---------------------------------------------------------------------------
# Configuration options related to the HTML output
#---------------------------------------------------------------------------
# If the GENERATE_HTML tag is set to YES, doxygen will generate HTML output
# The default value is: YES.
GENERATE_HTML = YES
# The HTML_OUTPUT tag is used to specify where the HTML docs will be put. If a
# relative path is entered the value of OUTPUT_DIRECTORY will be put in front of
# it.
# The default directory is: html.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_OUTPUT = html
# The HTML_FILE_EXTENSION tag can be used to specify the file extension for each
# generated HTML page (for example: .htm, .php, .asp).
# The default value is: .html.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_FILE_EXTENSION = .html
# The HTML_HEADER tag can be used to specify a user-defined HTML header file for
# each generated HTML page. If the tag is left blank doxygen will generate a
# standard header.
#
# To get valid HTML the header file that includes any scripts and style sheets
# that doxygen needs, which is dependent on the configuration options used (e.g.
# the setting GENERATE_TREEVIEW). It is highly recommended to start with a
# default header using
# doxygen -w html new_header.html new_footer.html new_stylesheet.css
# YourConfigFile
# and then modify the file new_header.html. See also section "Doxygen usage"
# for information on how to generate the default header that doxygen normally
# uses.
# Note: The header is subject to change so you typically have to regenerate the
# default header when upgrading to a newer version of doxygen. For a description
# of the possible markers and block names see the documentation.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_HEADER =
# The HTML_FOOTER tag can be used to specify a user-defined HTML footer for each
# generated HTML page. If the tag is left blank doxygen will generate a standard
# footer. See HTML_HEADER for more information on how to generate a default
# footer and what special commands can be used inside the footer. See also
# section "Doxygen usage" for information on how to generate the default footer
# that doxygen normally uses.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_FOOTER =
# The HTML_STYLESHEET tag can be used to specify a user-defined cascading style
# sheet that is used by each HTML page. It can be used to fine-tune the look of
# the HTML output. If left blank doxygen will generate a default style sheet.
# See also section "Doxygen usage" for information on how to generate the style
# sheet that doxygen normally uses.
# Note: It is recommended to use HTML_EXTRA_STYLESHEET instead of this tag, as
# it is more robust and this tag (HTML_STYLESHEET) will in the future become
# obsolete.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_STYLESHEET =
# The HTML_EXTRA_STYLESHEET tag can be used to specify additional user-defined
# cascading style sheets that are included after the standard style sheets
# created by doxygen. Using this option one can overrule certain style aspects.
# This is preferred over using HTML_STYLESHEET since it does not replace the
# standard style sheet and is therefore more robust against future updates.
# Doxygen will copy the style sheet files to the output directory.
# Note: The order of the extra style sheet files is of importance (e.g. the last
# style sheet in the list overrules the setting of the previous ones in the
# list). For an example see the documentation.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_EXTRA_STYLESHEET =
# The HTML_EXTRA_FILES tag can be used to specify one or more extra images or
# other source files which should be copied to the HTML output directory. Note
# that these files will be copied to the base HTML output directory. Use the
# $relpath^ marker in the HTML_HEADER and/or HTML_FOOTER files to load these
# files. In the HTML_STYLESHEET file, use the file name only. Also note that the
# files will be copied as-is; there are no commands or markers available.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_EXTRA_FILES =
# The HTML_COLORSTYLE_HUE tag controls the color of the HTML output. Doxygen
# will adjust the colors in the style sheet and background images according to
# this color. Hue is specified as an angle on a colorwheel, see
# http://en.wikipedia.org/wiki/Hue for more information. For instance the value
# 0 represents red, 60 is yellow, 120 is green, 180 is cyan, 240 is blue, 300
# purple, and 360 is red again.
# Minimum value: 0, maximum value: 359, default value: 220.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_COLORSTYLE_HUE = 220
# The HTML_COLORSTYLE_SAT tag controls the purity (or saturation) of the colors
# in the HTML output. For a value of 0 the output will use grayscales only. A
# value of 255 will produce the most vivid colors.
# Minimum value: 0, maximum value: 255, default value: 100.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_COLORSTYLE_SAT = 100
# The HTML_COLORSTYLE_GAMMA tag controls the gamma correction applied to the
# luminance component of the colors in the HTML output. Values below 100
# gradually make the output lighter, whereas values above 100 make the output
# darker. The value divided by 100 is the actual gamma applied, so 80 represents
# a gamma of 0.8, The value 220 represents a gamma of 2.2, and 100 does not
# change the gamma.
# Minimum value: 40, maximum value: 240, default value: 80.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_COLORSTYLE_GAMMA = 80
# If the HTML_TIMESTAMP tag is set to YES then the footer of each generated HTML
# page will contain the date and time when the page was generated. Setting this
# to YES can help to show when doxygen was last run and thus if the
# documentation is up to date.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_TIMESTAMP = NO
# If the HTML_DYNAMIC_SECTIONS tag is set to YES then the generated HTML
# documentation will contain sections that can be hidden and shown after the
# page has loaded.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_DYNAMIC_SECTIONS = NO
# With HTML_INDEX_NUM_ENTRIES one can control the preferred number of entries
# shown in the various tree structured indices initially; the user can expand
# and collapse entries dynamically later on. Doxygen will expand the tree to
# such a level that at most the specified number of entries are visible (unless
# a fully collapsed tree already exceeds this amount). So setting the number of
# entries 1 will produce a full collapsed tree by default. 0 is a special value
# representing an infinite number of entries and will result in a full expanded
# tree by default.
# Minimum value: 0, maximum value: 9999, default value: 100.
# This tag requires that the tag GENERATE_HTML is set to YES.
HTML_INDEX_NUM_ENTRIES = 100
# If the GENERATE_DOCSET tag is set to YES, additional index files will be
# generated that can be used as input for Apple's Xcode 3 integrated development
# environment (see: http://developer.apple.com/tools/xcode/), introduced with
# OSX 10.5 (Leopard). To create a documentation set, doxygen will generate a
# Makefile in the HTML output directory. Running make will produce the docset in
# that directory and running make install will install the docset in
# ~/Library/Developer/Shared/Documentation/DocSets so that Xcode will find it at
# startup. See http://developer.apple.com/tools/creatingdocsetswithdoxygen.html
# for more information.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
GENERATE_DOCSET = NO
# This tag determines the name of the docset feed. A documentation feed provides
# an umbrella under which multiple documentation sets from a single provider
# (such as a company or product suite) can be grouped.
# The default value is: Doxygen generated docs.
# This tag requires that the tag GENERATE_DOCSET is set to YES.
DOCSET_FEEDNAME = "Doxygen generated docs"
# This tag specifies a string that should uniquely identify the documentation
# set bundle. This should be a reverse domain-name style string, e.g.
# com.mycompany.MyDocSet. Doxygen will append .docset to the name.
# The default value is: org.doxygen.Project.
# This tag requires that the tag GENERATE_DOCSET is set to YES.
DOCSET_BUNDLE_ID = org.doxygen.Project
# The DOCSET_PUBLISHER_ID tag specifies a string that should uniquely identify
# the documentation publisher. This should be a reverse domain-name style
# string, e.g. com.mycompany.MyDocSet.documentation.
# The default value is: org.doxygen.Publisher.
# This tag requires that the tag GENERATE_DOCSET is set to YES.
DOCSET_PUBLISHER_ID = org.doxygen.Publisher
# The DOCSET_PUBLISHER_NAME tag identifies the documentation publisher.
# The default value is: Publisher.
# This tag requires that the tag GENERATE_DOCSET is set to YES.
DOCSET_PUBLISHER_NAME = Publisher
# If the GENERATE_HTMLHELP tag is set to YES then doxygen generates three
# additional HTML index files: index.hhp, index.hhc, and index.hhk. The
# index.hhp is a project file that can be read by Microsoft's HTML Help Workshop
# (see: http://www.microsoft.com/en-us/download/details.aspx?id=21138) on
# Windows.
#
# The HTML Help Workshop contains a compiler that can convert all HTML output
# generated by doxygen into a single compiled HTML file (.chm). Compiled HTML
# files are now used as the Windows 98 help format, and will replace the old
# Windows help format (.hlp) on all Windows platforms in the future. Compressed
# HTML files also contain an index, a table of contents, and you can search for
# words in the documentation. The HTML workshop also contains a viewer for
# compressed HTML files.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
GENERATE_HTMLHELP = NO
# The CHM_FILE tag can be used to specify the file name of the resulting .chm
# file. You can add a path in front of the file if the result should not be
# written to the html output directory.
# This tag requires that the tag GENERATE_HTMLHELP is set to YES.
CHM_FILE =
# The HHC_LOCATION tag can be used to specify the location (absolute path
# including file name) of the HTML help compiler (hhc.exe). If non-empty,
# doxygen will try to run the HTML help compiler on the generated index.hhp.
# The file has to be specified with full path.
# This tag requires that the tag GENERATE_HTMLHELP is set to YES.
HHC_LOCATION =
# The GENERATE_CHI flag controls if a separate .chi index file is generated
# (YES) or that it should be included in the master .chm file (NO).
# The default value is: NO.
# This tag requires that the tag GENERATE_HTMLHELP is set to YES.
GENERATE_CHI = NO
# The CHM_INDEX_ENCODING is used to encode HtmlHelp index (hhk), content (hhc)
# and project file content.
# This tag requires that the tag GENERATE_HTMLHELP is set to YES.
CHM_INDEX_ENCODING =
# The BINARY_TOC flag controls whether a binary table of contents is generated
# (YES) or a normal table of contents (NO) in the .chm file. Furthermore it
# enables the Previous and Next buttons.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTMLHELP is set to YES.
BINARY_TOC = NO
# The TOC_EXPAND flag can be set to YES to add extra items for group members to
# the table of contents of the HTML help documentation and to the tree view.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTMLHELP is set to YES.
TOC_EXPAND = NO
# If the GENERATE_QHP tag is set to YES and both QHP_NAMESPACE and
# QHP_VIRTUAL_FOLDER are set, an additional index file will be generated that
# can be used as input for Qt's qhelpgenerator to generate a Qt Compressed Help
# (.qch) of the generated HTML documentation.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
GENERATE_QHP = NO
# If the QHG_LOCATION tag is specified, the QCH_FILE tag can be used to specify
# the file name of the resulting .qch file. The path specified is relative to
# the HTML output folder.
# This tag requires that the tag GENERATE_QHP is set to YES.
QCH_FILE =
# The QHP_NAMESPACE tag specifies the namespace to use when generating Qt Help
# Project output. For more information please see Qt Help Project / Namespace
# (see: http://qt-project.org/doc/qt-4.8/qthelpproject.html#namespace).
# The default value is: org.doxygen.Project.
# This tag requires that the tag GENERATE_QHP is set to YES.
QHP_NAMESPACE = org.doxygen.Project
# The QHP_VIRTUAL_FOLDER tag specifies the namespace to use when generating Qt
# Help Project output. For more information please see Qt Help Project / Virtual
# Folders (see: http://qt-project.org/doc/qt-4.8/qthelpproject.html#virtual-
# folders).
# The default value is: doc.
# This tag requires that the tag GENERATE_QHP is set to YES.
QHP_VIRTUAL_FOLDER = doc
# If the QHP_CUST_FILTER_NAME tag is set, it specifies the name of a custom
# filter to add. For more information please see Qt Help Project / Custom
# Filters (see: http://qt-project.org/doc/qt-4.8/qthelpproject.html#custom-
# filters).
# This tag requires that the tag GENERATE_QHP is set to YES.
QHP_CUST_FILTER_NAME =
# The QHP_CUST_FILTER_ATTRS tag specifies the list of the attributes of the
# custom filter to add. For more information please see Qt Help Project / Custom
# Filters (see: http://qt-project.org/doc/qt-4.8/qthelpproject.html#custom-
# filters).
# This tag requires that the tag GENERATE_QHP is set to YES.
QHP_CUST_FILTER_ATTRS =
# The QHP_SECT_FILTER_ATTRS tag specifies the list of the attributes this
# project's filter section matches. Qt Help Project / Filter Attributes (see:
# http://qt-project.org/doc/qt-4.8/qthelpproject.html#filter-attributes).
# This tag requires that the tag GENERATE_QHP is set to YES.
QHP_SECT_FILTER_ATTRS =
# The QHG_LOCATION tag can be used to specify the location of Qt's
# qhelpgenerator. If non-empty doxygen will try to run qhelpgenerator on the
# generated .qhp file.
# This tag requires that the tag GENERATE_QHP is set to YES.
QHG_LOCATION =
# If the GENERATE_ECLIPSEHELP tag is set to YES, additional index files will be
# generated, together with the HTML files, they form an Eclipse help plugin. To
# install this plugin and make it available under the help contents menu in
# Eclipse, the contents of the directory containing the HTML and XML files needs
# to be copied into the plugins directory of eclipse. The name of the directory
# within the plugins directory should be the same as the ECLIPSE_DOC_ID value.
# After copying Eclipse needs to be restarted before the help appears.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
GENERATE_ECLIPSEHELP = NO
# A unique identifier for the Eclipse help plugin. When installing the plugin
# the directory name containing the HTML and XML files should also have this
# name. Each documentation set should have its own identifier.
# The default value is: org.doxygen.Project.
# This tag requires that the tag GENERATE_ECLIPSEHELP is set to YES.
ECLIPSE_DOC_ID = org.doxygen.Project
# If you want full control over the layout of the generated HTML pages it might
# be necessary to disable the index and replace it with your own. The
# DISABLE_INDEX tag can be used to turn on/off the condensed index (tabs) at top
# of each HTML page. A value of NO enables the index and the value YES disables
# it. Since the tabs in the index contain the same information as the navigation
# tree, you can set this option to YES if you also set GENERATE_TREEVIEW to YES.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
DISABLE_INDEX = NO
# The GENERATE_TREEVIEW tag is used to specify whether a tree-like index
# structure should be generated to display hierarchical information. If the tag
# value is set to YES, a side panel will be generated containing a tree-like
# index structure (just like the one that is generated for HTML Help). For this
# to work a browser that supports JavaScript, DHTML, CSS and frames is required
# (i.e. any modern browser). Windows users are probably better off using the
# HTML help feature. Via custom style sheets (see HTML_EXTRA_STYLESHEET) one can
# further fine-tune the look of the index. As an example, the default style
# sheet generated by doxygen has an example that shows how to put an image at
# the root of the tree instead of the PROJECT_NAME. Since the tree basically has
# the same information as the tab index, you could consider setting
# DISABLE_INDEX to YES when enabling this option.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
GENERATE_TREEVIEW = NO
# The ENUM_VALUES_PER_LINE tag can be used to set the number of enum values that
# doxygen will group on one line in the generated HTML documentation.
#
# Note that a value of 0 will completely suppress the enum values from appearing
# in the overview section.
# Minimum value: 0, maximum value: 20, default value: 4.
# This tag requires that the tag GENERATE_HTML is set to YES.
ENUM_VALUES_PER_LINE = 4
# If the treeview is enabled (see GENERATE_TREEVIEW) then this tag can be used
# to set the initial width (in pixels) of the frame in which the tree is shown.
# Minimum value: 0, maximum value: 1500, default value: 250.
# This tag requires that the tag GENERATE_HTML is set to YES.
TREEVIEW_WIDTH = 250
# If the EXT_LINKS_IN_WINDOW option is set to YES, doxygen will open links to
# external symbols imported via tag files in a separate window.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
EXT_LINKS_IN_WINDOW = NO
# Use this tag to change the font size of LaTeX formulas included as images in
# the HTML documentation. When you change the font size after a successful
# doxygen run you need to manually remove any form_*.png images from the HTML
# output directory to force them to be regenerated.
# Minimum value: 8, maximum value: 50, default value: 10.
# This tag requires that the tag GENERATE_HTML is set to YES.
FORMULA_FONTSIZE = 10
# Use the FORMULA_TRANPARENT tag to determine whether or not the images
# generated for formulas are transparent PNGs. Transparent PNGs are not
# supported properly for IE 6.0, but are supported on all modern browsers.
#
# Note that when changing this option you need to delete any form_*.png files in
# the HTML output directory before the changes have effect.
# The default value is: YES.
# This tag requires that the tag GENERATE_HTML is set to YES.
FORMULA_TRANSPARENT = YES
# Enable the USE_MATHJAX option to render LaTeX formulas using MathJax (see
# http://www.mathjax.org) which uses client side Javascript for the rendering
# instead of using pre-rendered bitmaps. Use this if you do not have LaTeX
# installed or if you want to formulas look prettier in the HTML output. When
# enabled you may also need to install MathJax separately and configure the path
# to it using the MATHJAX_RELPATH option.
# The default value is: NO.
# This tag requires that the tag GENERATE_HTML is set to YES.
USE_MATHJAX = NO
# When MathJax is enabled you can set the default output format to be used for
# the MathJax output. See the MathJax site (see:
# http://docs.mathjax.org/en/latest/output.html) for more details.
# Possible values are: HTML-CSS (which is slower, but has the best
# compatibility), NativeMML (i.e. MathML) and SVG.
# The default value is: HTML-CSS.
# This tag requires that the tag USE_MATHJAX is set to YES.
MATHJAX_FORMAT = HTML-CSS
# When MathJax is enabled you need to specify the location relative to the HTML
# output directory using the MATHJAX_RELPATH option. The destination directory
# should contain the MathJax.js script. For instance, if the mathjax directory
# is located at the same level as the HTML output directory, then
# MATHJAX_RELPATH should be ../mathjax. The default value points to the MathJax
# Content Delivery Network so you can quickly see the result without installing
# MathJax. However, it is strongly recommended to install a local copy of
# MathJax from http://www.mathjax.org before deployment.
# The default value is: http://cdn.mathjax.org/mathjax/latest.
# This tag requires that the tag USE_MATHJAX is set to YES.
MATHJAX_RELPATH = http://cdn.mathjax.org/mathjax/latest
# The MATHJAX_EXTENSIONS tag can be used to specify one or more MathJax
# extension names that should be enabled during MathJax rendering. For example
# MATHJAX_EXTENSIONS = TeX/AMSmath TeX/AMSsymbols
# This tag requires that the tag USE_MATHJAX is set to YES.
MATHJAX_EXTENSIONS =
# The MATHJAX_CODEFILE tag can be used to specify a file with javascript pieces
# of code that will be used on startup of the MathJax code. See the MathJax site
# (see: http://docs.mathjax.org/en/latest/output.html) for more details. For an
# example see the documentation.
# This tag requires that the tag USE_MATHJAX is set to YES.
MATHJAX_CODEFILE =
# When the SEARCHENGINE tag is enabled doxygen will generate a search box for
# the HTML output. The underlying search engine uses javascript and DHTML and
# should work on any modern browser. Note that when using HTML help
# (GENERATE_HTMLHELP), Qt help (GENERATE_QHP), or docsets (GENERATE_DOCSET)
# there is already a search function so this one should typically be disabled.
# For large projects the javascript based search engine can be slow, then
# enabling SERVER_BASED_SEARCH may provide a better solution. It is possible to
# search using the keyboard; to jump to the search box use <access key> + S
# (what the <access key> is depends on the OS and browser, but it is typically
# <CTRL>, <ALT>/<option>, or both). Inside the search box use the <cursor down
# key> to jump into the search results window, the results can be navigated
# using the <cursor keys>. Press <Enter> to select an item or <escape> to cancel
# the search. The filter options can be selected when the cursor is inside the
# search box by pressing <Shift>+<cursor down>. Also here use the <cursor keys>
# to select a filter and <Enter> or <escape> to activate or cancel the filter
# option.
# The default value is: YES.
# This tag requires that the tag GENERATE_HTML is set to YES.
SEARCHENGINE = YES
# When the SERVER_BASED_SEARCH tag is enabled the search engine will be
# implemented using a web server instead of a web client using Javascript. There
# are two flavors of web server based searching depending on the EXTERNAL_SEARCH
# setting. When disabled, doxygen will generate a PHP script for searching and
# an index file used by the script. When EXTERNAL_SEARCH is enabled the indexing
# and searching needs to be provided by external tools. See the section
# "External Indexing and Searching" for details.
# The default value is: NO.
# This tag requires that the tag SEARCHENGINE is set to YES.
SERVER_BASED_SEARCH = NO
# When EXTERNAL_SEARCH tag is enabled doxygen will no longer generate the PHP
# script for searching. Instead the search results are written to an XML file
# which needs to be processed by an external indexer. Doxygen will invoke an
# external search engine pointed to by the SEARCHENGINE_URL option to obtain the
# search results.
#
# Doxygen ships with an example indexer (doxyindexer) and search engine
# (doxysearch.cgi) which are based on the open source search engine library
# Xapian (see: http://xapian.org/).
#
# See the section "External Indexing and Searching" for details.
# The default value is: NO.
# This tag requires that the tag SEARCHENGINE is set to YES.
EXTERNAL_SEARCH = NO
# The SEARCHENGINE_URL should point to a search engine hosted by a web server
# which will return the search results when EXTERNAL_SEARCH is enabled.
#
# Doxygen ships with an example indexer (doxyindexer) and search engine
# (doxysearch.cgi) which are based on the open source search engine library
# Xapian (see: http://xapian.org/). See the section "External Indexing and
# Searching" for details.
# This tag requires that the tag SEARCHENGINE is set to YES.
SEARCHENGINE_URL =
# When SERVER_BASED_SEARCH and EXTERNAL_SEARCH are both enabled the unindexed
# search data is written to a file for indexing by an external tool. With the
# SEARCHDATA_FILE tag the name of this file can be specified.
# The default file is: searchdata.xml.
# This tag requires that the tag SEARCHENGINE is set to YES.
SEARCHDATA_FILE = searchdata.xml
# When SERVER_BASED_SEARCH and EXTERNAL_SEARCH are both enabled the
# EXTERNAL_SEARCH_ID tag can be used as an identifier for the project. This is
# useful in combination with EXTRA_SEARCH_MAPPINGS to search through multiple
# projects and redirect the results back to the right project.
# This tag requires that the tag SEARCHENGINE is set to YES.
EXTERNAL_SEARCH_ID =
# The EXTRA_SEARCH_MAPPINGS tag can be used to enable searching through doxygen
# projects other than the one defined by this configuration file, but that are
# all added to the same external search index. Each project needs to have a
# unique id set via EXTERNAL_SEARCH_ID. The search mapping then maps the id of
# to a relative location where the documentation can be found. The format is:
# EXTRA_SEARCH_MAPPINGS = tagname1=loc1 tagname2=loc2 ...
# This tag requires that the tag SEARCHENGINE is set to YES.
EXTRA_SEARCH_MAPPINGS =
#---------------------------------------------------------------------------
# Configuration options related to the LaTeX output
#---------------------------------------------------------------------------
# If the GENERATE_LATEX tag is set to YES, doxygen will generate LaTeX output.
# The default value is: YES.
GENERATE_LATEX = YES
# The LATEX_OUTPUT tag is used to specify where the LaTeX docs will be put. If a
# relative path is entered the value of OUTPUT_DIRECTORY will be put in front of
# it.
# The default directory is: latex.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_OUTPUT = latex
# The LATEX_CMD_NAME tag can be used to specify the LaTeX command name to be
# invoked.
#
# Note that when enabling USE_PDFLATEX this option is only used for generating
# bitmaps for formulas in the HTML output, but not in the Makefile that is
# written to the output directory.
# The default file is: latex.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_CMD_NAME = latex
# The MAKEINDEX_CMD_NAME tag can be used to specify the command name to generate
# index for LaTeX.
# The default file is: makeindex.
# This tag requires that the tag GENERATE_LATEX is set to YES.
MAKEINDEX_CMD_NAME = makeindex
# If the COMPACT_LATEX tag is set to YES, doxygen generates more compact LaTeX
# documents. This may be useful for small projects and may help to save some
# trees in general.
# The default value is: NO.
# This tag requires that the tag GENERATE_LATEX is set to YES.
COMPACT_LATEX = NO
# The PAPER_TYPE tag can be used to set the paper type that is used by the
# printer.
# Possible values are: a4 (210 x 297 mm), letter (8.5 x 11 inches), legal (8.5 x
# 14 inches) and executive (7.25 x 10.5 inches).
# The default value is: a4.
# This tag requires that the tag GENERATE_LATEX is set to YES.
PAPER_TYPE = a4
# The EXTRA_PACKAGES tag can be used to specify one or more LaTeX package names
# that should be included in the LaTeX output. The package can be specified just
# by its name or with the correct syntax as to be used with the LaTeX
# \usepackage command. To get the times font for instance you can specify :
# EXTRA_PACKAGES=times or EXTRA_PACKAGES={times}
# To use the option intlimits with the amsmath package you can specify:
# EXTRA_PACKAGES=[intlimits]{amsmath}
# If left blank no extra packages will be included.
# This tag requires that the tag GENERATE_LATEX is set to YES.
EXTRA_PACKAGES =
# The LATEX_HEADER tag can be used to specify a personal LaTeX header for the
# generated LaTeX document. The header should contain everything until the first
# chapter. If it is left blank doxygen will generate a standard header. See
# section "Doxygen usage" for information on how to let doxygen write the
# default header to a separate file.
#
# Note: Only use a user-defined header if you know what you are doing! The
# following commands have a special meaning inside the header: $title,
# $datetime, $date, $doxygenversion, $projectname, $projectnumber,
# $projectbrief, $projectlogo. Doxygen will replace $title with the empty
# string, for the replacement values of the other commands the user is referred
# to HTML_HEADER.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_HEADER =
# The LATEX_FOOTER tag can be used to specify a personal LaTeX footer for the
# generated LaTeX document. The footer should contain everything after the last
# chapter. If it is left blank doxygen will generate a standard footer. See
# LATEX_HEADER for more information on how to generate a default footer and what
# special commands can be used inside the footer.
#
# Note: Only use a user-defined footer if you know what you are doing!
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_FOOTER =
# The LATEX_EXTRA_STYLESHEET tag can be used to specify additional user-defined
# LaTeX style sheets that are included after the standard style sheets created
# by doxygen. Using this option one can overrule certain style aspects. Doxygen
# will copy the style sheet files to the output directory.
# Note: The order of the extra style sheet files is of importance (e.g. the last
# style sheet in the list overrules the setting of the previous ones in the
# list).
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_EXTRA_STYLESHEET =
# The LATEX_EXTRA_FILES tag can be used to specify one or more extra images or
# other source files which should be copied to the LATEX_OUTPUT output
# directory. Note that the files will be copied as-is; there are no commands or
# markers available.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_EXTRA_FILES =
# If the PDF_HYPERLINKS tag is set to YES, the LaTeX that is generated is
# prepared for conversion to PDF (using ps2pdf or pdflatex). The PDF file will
# contain links (just like the HTML output) instead of page references. This
# makes the output suitable for online browsing using a PDF viewer.
# The default value is: YES.
# This tag requires that the tag GENERATE_LATEX is set to YES.
PDF_HYPERLINKS = YES
# If the USE_PDFLATEX tag is set to YES, doxygen will use pdflatex to generate
# the PDF file directly from the LaTeX files. Set this option to YES, to get a
# higher quality PDF documentation.
# The default value is: YES.
# This tag requires that the tag GENERATE_LATEX is set to YES.
USE_PDFLATEX = YES
# If the LATEX_BATCHMODE tag is set to YES, doxygen will add the \batchmode
# command to the generated LaTeX files. This will instruct LaTeX to keep running
# if errors occur, instead of asking the user for help. This option is also used
# when generating formulas in HTML.
# The default value is: NO.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_BATCHMODE = NO
# If the LATEX_HIDE_INDICES tag is set to YES then doxygen will not include the
# index chapters (such as File Index, Compound Index, etc.) in the output.
# The default value is: NO.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_HIDE_INDICES = NO
# If the LATEX_SOURCE_CODE tag is set to YES then doxygen will include source
# code with syntax highlighting in the LaTeX output.
#
# Note that which sources are shown also depends on other settings such as
# SOURCE_BROWSER.
# The default value is: NO.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_SOURCE_CODE = NO
# The LATEX_BIB_STYLE tag can be used to specify the style to use for the
# bibliography, e.g. plainnat, or ieeetr. See
# http://en.wikipedia.org/wiki/BibTeX and \cite for more info.
# The default value is: plain.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_BIB_STYLE = plain
# If the LATEX_TIMESTAMP tag is set to YES then the footer of each generated
# page will contain the date and time when the page was generated. Setting this
# to NO can help when comparing the output of multiple runs.
# The default value is: NO.
# This tag requires that the tag GENERATE_LATEX is set to YES.
LATEX_TIMESTAMP = NO
#---------------------------------------------------------------------------
# Configuration options related to the RTF output
#---------------------------------------------------------------------------
# If the GENERATE_RTF tag is set to YES, doxygen will generate RTF output. The
# RTF output is optimized for Word 97 and may not look too pretty with other RTF
# readers/editors.
# The default value is: NO.
GENERATE_RTF = NO
# The RTF_OUTPUT tag is used to specify where the RTF docs will be put. If a
# relative path is entered the value of OUTPUT_DIRECTORY will be put in front of
# it.
# The default directory is: rtf.
# This tag requires that the tag GENERATE_RTF is set to YES.
RTF_OUTPUT = rtf
# If the COMPACT_RTF tag is set to YES, doxygen generates more compact RTF
# documents. This may be useful for small projects and may help to save some
# trees in general.
# The default value is: NO.
# This tag requires that the tag GENERATE_RTF is set to YES.
COMPACT_RTF = NO
# If the RTF_HYPERLINKS tag is set to YES, the RTF that is generated will
# contain hyperlink fields. The RTF file will contain links (just like the HTML
# output) instead of page references. This makes the output suitable for online
# browsing using Word or some other Word compatible readers that support those
# fields.
#
# Note: WordPad (write) and others do not support links.
# The default value is: NO.
# This tag requires that the tag GENERATE_RTF is set to YES.
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# Load stylesheet definitions from file. Syntax is similar to doxygen's config
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#
# See also section "Doxygen usage" for information on how to generate the
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# This tag requires that the tag GENERATE_RTF is set to YES.
RTF_STYLESHEET_FILE =
# Set optional variables used in the generation of an RTF document. Syntax is
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# using doxygen -e rtf extensionFile.
# This tag requires that the tag GENERATE_RTF is set to YES.
RTF_EXTENSIONS_FILE =
# If the RTF_SOURCE_CODE tag is set to YES then doxygen will include source code
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#
# Note that which sources are shown also depends on other settings such as
# SOURCE_BROWSER.
# The default value is: NO.
# This tag requires that the tag GENERATE_RTF is set to YES.
RTF_SOURCE_CODE = NO
#---------------------------------------------------------------------------
# Configuration options related to the man page output
#---------------------------------------------------------------------------
# If the GENERATE_MAN tag is set to YES, doxygen will generate man pages for
# classes and files.
# The default value is: NO.
GENERATE_MAN = NO
# The MAN_OUTPUT tag is used to specify where the man pages will be put. If a
# relative path is entered the value of OUTPUT_DIRECTORY will be put in front of
# it. A directory man3 will be created inside the directory specified by
# MAN_OUTPUT.
# The default directory is: man.
# This tag requires that the tag GENERATE_MAN is set to YES.
MAN_OUTPUT = man
# The MAN_EXTENSION tag determines the extension that is added to the generated
# man pages. In case the manual section does not start with a number, the number
# 3 is prepended. The dot (.) at the beginning of the MAN_EXTENSION tag is
# optional.
# The default value is: .3.
# This tag requires that the tag GENERATE_MAN is set to YES.
MAN_EXTENSION = .3
# The MAN_SUBDIR tag determines the name of the directory created within
# MAN_OUTPUT in which the man pages are placed. If defaults to man followed by
# MAN_EXTENSION with the initial . removed.
# This tag requires that the tag GENERATE_MAN is set to YES.
MAN_SUBDIR =
# If the MAN_LINKS tag is set to YES and doxygen generates man output, then it
# will generate one additional man file for each entity documented in the real
# man page(s). These additional files only source the real man page, but without
# them the man command would be unable to find the correct page.
# The default value is: NO.
# This tag requires that the tag GENERATE_MAN is set to YES.
MAN_LINKS = NO
#---------------------------------------------------------------------------
# Configuration options related to the XML output
#---------------------------------------------------------------------------
# If the GENERATE_XML tag is set to YES, doxygen will generate an XML file that
# captures the structure of the code including all documentation.
# The default value is: NO.
GENERATE_XML = NO
# The XML_OUTPUT tag is used to specify where the XML pages will be put. If a
# relative path is entered the value of OUTPUT_DIRECTORY will be put in front of
# it.
# The default directory is: xml.
# This tag requires that the tag GENERATE_XML is set to YES.
XML_OUTPUT = xml
# If the XML_PROGRAMLISTING tag is set to YES, doxygen will dump the program
# listings (including syntax highlighting and cross-referencing information) to
# the XML output. Note that enabling this will significantly increase the size
# of the XML output.
# The default value is: YES.
# This tag requires that the tag GENERATE_XML is set to YES.
XML_PROGRAMLISTING = YES
#---------------------------------------------------------------------------
# Configuration options related to the DOCBOOK output
#---------------------------------------------------------------------------
# If the GENERATE_DOCBOOK tag is set to YES, doxygen will generate Docbook files
# that can be used to generate PDF.
# The default value is: NO.
GENERATE_DOCBOOK = NO
# The DOCBOOK_OUTPUT tag is used to specify where the Docbook pages will be put.
# If a relative path is entered the value of OUTPUT_DIRECTORY will be put in
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# The default directory is: docbook.
# This tag requires that the tag GENERATE_DOCBOOK is set to YES.
DOCBOOK_OUTPUT = docbook
# If the DOCBOOK_PROGRAMLISTING tag is set to YES, doxygen will include the
# program listings (including syntax highlighting and cross-referencing
# information) to the DOCBOOK output. Note that enabling this will significantly
# increase the size of the DOCBOOK output.
# The default value is: NO.
# This tag requires that the tag GENERATE_DOCBOOK is set to YES.
DOCBOOK_PROGRAMLISTING = NO
#---------------------------------------------------------------------------
# Configuration options for the AutoGen Definitions output
#---------------------------------------------------------------------------
# If the GENERATE_AUTOGEN_DEF tag is set to YES, doxygen will generate an
# AutoGen Definitions (see http://autogen.sf.net) file that captures the
# structure of the code including all documentation. Note that this feature is
# still experimental and incomplete at the moment.
# The default value is: NO.
GENERATE_AUTOGEN_DEF = NO
#---------------------------------------------------------------------------
# Configuration options related to the Perl module output
#---------------------------------------------------------------------------
# If the GENERATE_PERLMOD tag is set to YES, doxygen will generate a Perl module
# file that captures the structure of the code including all documentation.
#
# Note that this feature is still experimental and incomplete at the moment.
# The default value is: NO.
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# If the PERLMOD_LATEX tag is set to YES, doxygen will generate the necessary
# Makefile rules, Perl scripts and LaTeX code to be able to generate PDF and DVI
# output from the Perl module output.
# The default value is: NO.
# This tag requires that the tag GENERATE_PERLMOD is set to YES.
PERLMOD_LATEX = NO
# If the PERLMOD_PRETTY tag is set to YES, the Perl module output will be nicely
# formatted so it can be parsed by a human reader. This is useful if you want to
# understand what is going on. On the other hand, if this tag is set to NO, the
# size of the Perl module output will be much smaller and Perl will parse it
# just the same.
# The default value is: YES.
# This tag requires that the tag GENERATE_PERLMOD is set to YES.
PERLMOD_PRETTY = YES
# The names of the make variables in the generated doxyrules.make file are
# prefixed with the string contained in PERLMOD_MAKEVAR_PREFIX. This is useful
# so different doxyrules.make files included by the same Makefile don't
# overwrite each other's variables.
# This tag requires that the tag GENERATE_PERLMOD is set to YES.
PERLMOD_MAKEVAR_PREFIX =
#---------------------------------------------------------------------------
# Configuration options related to the preprocessor
#---------------------------------------------------------------------------
# If the ENABLE_PREPROCESSING tag is set to YES, doxygen will evaluate all
# C-preprocessor directives found in the sources and include files.
# The default value is: YES.
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# If the MACRO_EXPANSION tag is set to YES, doxygen will expand all macro names
# in the source code. If set to NO, only conditional compilation will be
# performed. Macro expansion can be done in a controlled way by setting
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# The default value is: NO.
# This tag requires that the tag ENABLE_PREPROCESSING is set to YES.
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# If the EXPAND_ONLY_PREDEF and MACRO_EXPANSION tags are both set to YES then
# the macro expansion is limited to the macros specified with the PREDEFINED and
# EXPAND_AS_DEFINED tags.
# The default value is: NO.
# This tag requires that the tag ENABLE_PREPROCESSING is set to YES.
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# If the SEARCH_INCLUDES tag is set to YES, the include files in the
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# The default value is: YES.
# This tag requires that the tag ENABLE_PREPROCESSING is set to YES.
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# The INCLUDE_PATH tag can be used to specify one or more directories that
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# preprocessor.
# This tag requires that the tag SEARCH_INCLUDES is set to YES.
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# You can use the INCLUDE_FILE_PATTERNS tag to specify one or more wildcard
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# used.
# This tag requires that the tag ENABLE_PREPROCESSING is set to YES.
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# The PREDEFINED tag can be used to specify one or more macro names that are
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# gcc). The argument of the tag is a list of macros of the form: name or
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# recursively expanded use the := operator instead of the = operator.
# This tag requires that the tag ENABLE_PREPROCESSING is set to YES.
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# If the MACRO_EXPANSION and EXPAND_ONLY_PREDEF tags are set to YES then this
# tag can be used to specify a list of macro names that should be expanded. The
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# tag if you want to use a different macro definition that overrules the
# definition found in the source code.
# This tag requires that the tag ENABLE_PREPROCESSING is set to YES.
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# If the SKIP_FUNCTION_MACROS tag is set to YES then doxygen's preprocessor will
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# are typically used for boiler-plate code, and will confuse the parser if not
# removed.
# The default value is: YES.
# This tag requires that the tag ENABLE_PREPROCESSING is set to YES.
SKIP_FUNCTION_MACROS = YES
#---------------------------------------------------------------------------
# Configuration options related to external references
#---------------------------------------------------------------------------
# The TAGFILES tag can be used to specify one or more tag files. For each tag
# file the location of the external documentation should be added. The format of
# a tag file without this location is as follows:
# TAGFILES = file1 file2 ...
# Adding location for the tag files is done as follows:
# TAGFILES = file1=loc1 "file2 = loc2" ...
# where loc1 and loc2 can be relative or absolute paths or URLs. See the
# section "Linking to external documentation" for more information about the use
# of tag files.
# Note: Each tag file must have a unique name (where the name does NOT include
# the path). If a tag file is not located in the directory in which doxygen is
# run, you must also specify the path to the tagfile here.
TAGFILES =
# When a file name is specified after GENERATE_TAGFILE, doxygen will create a
# tag file that is based on the input files it reads. See section "Linking to
# external documentation" for more information about the usage of tag files.
GENERATE_TAGFILE =
# If the ALLEXTERNALS tag is set to YES, all external class will be listed in
# the class index. If set to NO, only the inherited external classes will be
# listed.
# The default value is: NO.
ALLEXTERNALS = NO
# If the EXTERNAL_GROUPS tag is set to YES, all external groups will be listed
# in the modules index. If set to NO, only the current project's groups will be
# listed.
# The default value is: YES.
EXTERNAL_GROUPS = YES
# If the EXTERNAL_PAGES tag is set to YES, all external pages will be listed in
# the related pages index. If set to NO, only the current project's pages will
# be listed.
# The default value is: YES.
EXTERNAL_PAGES = YES
# The PERL_PATH should be the absolute path and name of the perl script
# interpreter (i.e. the result of 'which perl').
# The default file (with absolute path) is: /usr/bin/perl.
PERL_PATH = /usr/bin/perl
#---------------------------------------------------------------------------
# Configuration options related to the dot tool
#---------------------------------------------------------------------------
# If the CLASS_DIAGRAMS tag is set to YES, doxygen will generate a class diagram
# (in HTML and LaTeX) for classes with base or super classes. Setting the tag to
# NO turns the diagrams off. Note that this option also works with HAVE_DOT
# disabled, but it is recommended to install and use dot, since it yields more
# powerful graphs.
# The default value is: YES.
CLASS_DIAGRAMS = YES
# You can define message sequence charts within doxygen comments using the \msc
# command. Doxygen will then run the mscgen tool (see:
# http://www.mcternan.me.uk/mscgen/)) to produce the chart and insert it in the
# documentation. The MSCGEN_PATH tag allows you to specify the directory where
# the mscgen tool resides. If left empty the tool is assumed to be found in the
# default search path.
MSCGEN_PATH =
# You can include diagrams made with dia in doxygen documentation. Doxygen will
# then run dia to produce the diagram and insert it in the documentation. The
# DIA_PATH tag allows you to specify the directory where the dia binary resides.
# If left empty dia is assumed to be found in the default search path.
DIA_PATH =
# If set to YES the inheritance and collaboration graphs will hide inheritance
# and usage relations if the target is undocumented or is not a class.
# The default value is: YES.
HIDE_UNDOC_RELATIONS = YES
# If you set the HAVE_DOT tag to YES then doxygen will assume the dot tool is
# available from the path. This tool is part of Graphviz (see:
# http://www.graphviz.org/), a graph visualization toolkit from AT&T and Lucent
# Bell Labs. The other options in this section have no effect if this option is
# set to NO
# The default value is: YES.
HAVE_DOT = YES
# The DOT_NUM_THREADS specifies the number of dot invocations doxygen is allowed
# to run in parallel. When set to 0 doxygen will base this on the number of
# processors available in the system. You can set it explicitly to a value
# larger than 0 to get control over the balance between CPU load and processing
# speed.
# Minimum value: 0, maximum value: 32, default value: 0.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_NUM_THREADS = 0
# When you want a differently looking font in the dot files that doxygen
# generates you can specify the font name using DOT_FONTNAME. You need to make
# sure dot is able to find the font, which can be done by putting it in a
# standard location or by setting the DOTFONTPATH environment variable or by
# setting DOT_FONTPATH to the directory containing the font.
# The default value is: Helvetica.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_FONTNAME = Helvetica
# The DOT_FONTSIZE tag can be used to set the size (in points) of the font of
# dot graphs.
# Minimum value: 4, maximum value: 24, default value: 10.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_FONTSIZE = 10
# By default doxygen will tell dot to use the default font as specified with
# DOT_FONTNAME. If you specify a different font using DOT_FONTNAME you can set
# the path where dot can find it using this tag.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_FONTPATH =
# If the CLASS_GRAPH tag is set to YES then doxygen will generate a graph for
# each documented class showing the direct and indirect inheritance relations.
# Setting this tag to YES will force the CLASS_DIAGRAMS tag to NO.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
CLASS_GRAPH = YES
# If the COLLABORATION_GRAPH tag is set to YES then doxygen will generate a
# graph for each documented class showing the direct and indirect implementation
# dependencies (inheritance, containment, and class references variables) of the
# class with other documented classes.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
COLLABORATION_GRAPH = YES
# If the GROUP_GRAPHS tag is set to YES then doxygen will generate a graph for
# groups, showing the direct groups dependencies.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
GROUP_GRAPHS = YES
# If the UML_LOOK tag is set to YES, doxygen will generate inheritance and
# collaboration diagrams in a style similar to the OMG's Unified Modeling
# Language.
# The default value is: NO.
# This tag requires that the tag HAVE_DOT is set to YES.
UML_LOOK = NO
# If the UML_LOOK tag is enabled, the fields and methods are shown inside the
# class node. If there are many fields or methods and many nodes the graph may
# become too big to be useful. The UML_LIMIT_NUM_FIELDS threshold limits the
# number of items for each type to make the size more manageable. Set this to 0
# for no limit. Note that the threshold may be exceeded by 50% before the limit
# is enforced. So when you set the threshold to 10, up to 15 fields may appear,
# but if the number exceeds 15, the total amount of fields shown is limited to
# 10.
# Minimum value: 0, maximum value: 100, default value: 10.
# This tag requires that the tag HAVE_DOT is set to YES.
UML_LIMIT_NUM_FIELDS = 10
# If the TEMPLATE_RELATIONS tag is set to YES then the inheritance and
# collaboration graphs will show the relations between templates and their
# instances.
# The default value is: NO.
# This tag requires that the tag HAVE_DOT is set to YES.
TEMPLATE_RELATIONS = NO
# If the INCLUDE_GRAPH, ENABLE_PREPROCESSING and SEARCH_INCLUDES tags are set to
# YES then doxygen will generate a graph for each documented file showing the
# direct and indirect include dependencies of the file with other documented
# files.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
INCLUDE_GRAPH = YES
# If the INCLUDED_BY_GRAPH, ENABLE_PREPROCESSING and SEARCH_INCLUDES tags are
# set to YES then doxygen will generate a graph for each documented file showing
# the direct and indirect include dependencies of the file with other documented
# files.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
INCLUDED_BY_GRAPH = YES
# If the CALL_GRAPH tag is set to YES then doxygen will generate a call
# dependency graph for every global function or class method.
#
# Note that enabling this option will significantly increase the time of a run.
# So in most cases it will be better to enable call graphs for selected
# functions only using the \callgraph command. Disabling a call graph can be
# accomplished by means of the command \hidecallgraph.
# The default value is: NO.
# This tag requires that the tag HAVE_DOT is set to YES.
CALL_GRAPH = NO
# If the CALLER_GRAPH tag is set to YES then doxygen will generate a caller
# dependency graph for every global function or class method.
#
# Note that enabling this option will significantly increase the time of a run.
# So in most cases it will be better to enable caller graphs for selected
# functions only using the \callergraph command. Disabling a caller graph can be
# accomplished by means of the command \hidecallergraph.
# The default value is: NO.
# This tag requires that the tag HAVE_DOT is set to YES.
CALLER_GRAPH = NO
# If the GRAPHICAL_HIERARCHY tag is set to YES then doxygen will graphical
# hierarchy of all classes instead of a textual one.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
GRAPHICAL_HIERARCHY = YES
# If the DIRECTORY_GRAPH tag is set to YES then doxygen will show the
# dependencies a directory has on other directories in a graphical way. The
# dependency relations are determined by the #include relations between the
# files in the directories.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
DIRECTORY_GRAPH = YES
# The DOT_IMAGE_FORMAT tag can be used to set the image format of the images
# generated by dot. For an explanation of the image formats see the section
# output formats in the documentation of the dot tool (Graphviz (see:
# http://www.graphviz.org/)).
# Note: If you choose svg you need to set HTML_FILE_EXTENSION to xhtml in order
# to make the SVG files visible in IE 9+ (other browsers do not have this
# requirement).
# Possible values are: png, png:cairo, png:cairo:cairo, png:cairo:gd, png:gd,
# png:gd:gd, jpg, jpg:cairo, jpg:cairo:gd, jpg:gd, jpg:gd:gd, gif, gif:cairo,
# gif:cairo:gd, gif:gd, gif:gd:gd, svg, png:gd, png:gd:gd, png:cairo,
# png:cairo:gd, png:cairo:cairo, png:cairo:gdiplus, png:gdiplus and
# png:gdiplus:gdiplus.
# The default value is: png.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_IMAGE_FORMAT = png
# If DOT_IMAGE_FORMAT is set to svg, then this option can be set to YES to
# enable generation of interactive SVG images that allow zooming and panning.
#
# Note that this requires a modern browser other than Internet Explorer. Tested
# and working are Firefox, Chrome, Safari, and Opera.
# Note: For IE 9+ you need to set HTML_FILE_EXTENSION to xhtml in order to make
# the SVG files visible. Older versions of IE do not have SVG support.
# The default value is: NO.
# This tag requires that the tag HAVE_DOT is set to YES.
INTERACTIVE_SVG = NO
# The DOT_PATH tag can be used to specify the path where the dot tool can be
# found. If left blank, it is assumed the dot tool can be found in the path.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_PATH =
# The DOTFILE_DIRS tag can be used to specify one or more directories that
# contain dot files that are included in the documentation (see the \dotfile
# command).
# This tag requires that the tag HAVE_DOT is set to YES.
DOTFILE_DIRS =
# The MSCFILE_DIRS tag can be used to specify one or more directories that
# contain msc files that are included in the documentation (see the \mscfile
# command).
MSCFILE_DIRS =
# The DIAFILE_DIRS tag can be used to specify one or more directories that
# contain dia files that are included in the documentation (see the \diafile
# command).
DIAFILE_DIRS =
# When using plantuml, the PLANTUML_JAR_PATH tag should be used to specify the
# path where java can find the plantuml.jar file. If left blank, it is assumed
# PlantUML is not used or called during a preprocessing step. Doxygen will
# generate a warning when it encounters a \startuml command in this case and
# will not generate output for the diagram.
PLANTUML_JAR_PATH =
# When using plantuml, the specified paths are searched for files specified by
# the !include statement in a plantuml block.
PLANTUML_INCLUDE_PATH =
# The DOT_GRAPH_MAX_NODES tag can be used to set the maximum number of nodes
# that will be shown in the graph. If the number of nodes in a graph becomes
# larger than this value, doxygen will truncate the graph, which is visualized
# by representing a node as a red box. Note that doxygen if the number of direct
# children of the root node in a graph is already larger than
# DOT_GRAPH_MAX_NODES then the graph will not be shown at all. Also note that
# the size of a graph can be further restricted by MAX_DOT_GRAPH_DEPTH.
# Minimum value: 0, maximum value: 10000, default value: 50.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_GRAPH_MAX_NODES = 50
# The MAX_DOT_GRAPH_DEPTH tag can be used to set the maximum depth of the graphs
# generated by dot. A depth value of 3 means that only nodes reachable from the
# root by following a path via at most 3 edges will be shown. Nodes that lay
# further from the root node will be omitted. Note that setting this option to 1
# or 2 may greatly reduce the computation time needed for large code bases. Also
# note that the size of a graph can be further restricted by
# DOT_GRAPH_MAX_NODES. Using a depth of 0 means no depth restriction.
# Minimum value: 0, maximum value: 1000, default value: 0.
# This tag requires that the tag HAVE_DOT is set to YES.
MAX_DOT_GRAPH_DEPTH = 0
# Set the DOT_TRANSPARENT tag to YES to generate images with a transparent
# background. This is disabled by default, because dot on Windows does not seem
# to support this out of the box.
#
# Warning: Depending on the platform used, enabling this option may lead to
# badly anti-aliased labels on the edges of a graph (i.e. they become hard to
# read).
# The default value is: NO.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_TRANSPARENT = NO
# Set the DOT_MULTI_TARGETS tag to YES to allow dot to generate multiple output
# files in one run (i.e. multiple -o and -T options on the command line). This
# makes dot run faster, but since only newer versions of dot (>1.8.10) support
# this, this feature is disabled by default.
# The default value is: NO.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_MULTI_TARGETS = NO
# If the GENERATE_LEGEND tag is set to YES doxygen will generate a legend page
# explaining the meaning of the various boxes and arrows in the dot generated
# graphs.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
GENERATE_LEGEND = YES
# If the DOT_CLEANUP tag is set to YES, doxygen will remove the intermediate dot
# files that are used to generate the various graphs.
# The default value is: YES.
# This tag requires that the tag HAVE_DOT is set to YES.
DOT_CLEANUP = YES
diff --git a/doc/doxygen/mainpage.dox b/doc/doxygen/mainpage.dox
index 8e754d3..60cbb24 100644
--- a/doc/doxygen/mainpage.dox
+++ b/doc/doxygen/mainpage.dox
@@ -1,44 +1,225 @@
namespace HEJ { // so that doxygen links names in this namespace
/**
* @mainpage
*
* @section intro Introduction
*
* HEJ 2 is a library for all-order resummation of high-energy
* logarithms. It includes a program to add resummation to fixed-order
* events. User documentation for the program can be found <a
- * href="TODO">TODO: here</a>. This documentation is instead aimed at users
- * of the library itself.
+ * href="https://hej.web.cern.ch/HEJ/doc/2.0/user/">here</a>. This
+ * documentation is instead aimed at users of the library itself.
*
* @section overview Overview
*
* The main functionality is contained in the HEJ namespace. Particles
* are defined via the Particle struct, which consists of the particle
* four-momentum and its identifier according to the <a
* href="http://pdg.lbl.gov/2017/reviews/rpp2017-rev-monte-carlo-numbering.pdf">
* PDG Monte Carlo numbering scheme </a>. Given a number of incoming and
* outgoing particles, the square of the resummation matrix element can
* be calculated with the help of the MatrixElement class.
*
* The EventReweighter class adds resummation to existing fixed-order
* events. Both fixed-order and resummation events are objects of the
* Event class, which are created from UnclusteredEvent objects with the
* help of a <a
* href="http://fastjet.fr/repo/doxygen-3.3.1/classfastjet_1_1JetDefinition.html">jet
* definition according to the fastjet</a> library. UnclusteredEvent
* objects can be assembled manually or converted from input events in
* the LesHouches standard, read from file with a LHEF::Reader.
*
* Events can be saved with one of the EventWriter classes. Currently,
* there is support for the Les Houches event file format with the
* LesHouchesWriter class. If HEJ 2 was installed with HepMC 2 or 3
* support, the respective format is available through the HepMCWriter
* class.
*
* Further classes of interest are the interfaces to the Mixmax and
* Ranlux64 random number generators, the PDF class to interact with <a
* href="https://lhapdf.hepforge.org/"> LHAPDF </a> and the ScaleGenerator
* and ScaleConfig classes to calculate renormalisation and factorisation
* scales for a given Event.
+ *
+ * @section example Example
+ *
+ * As an example, we show a toy program that computes the square of a
+ * matrix element in the HEJ approximation for a single event. First, we
+ * include the necessary header files:
+ * @code{.cpp}
+ * #include "HEJ/Event.hh"
+ * #include "HEJ/MatrixElement.hh"
+ * @endcode
+ * We then specify the incoming and outgoing particles. A particle
+ * has a type and four-momentum \f$(p_x, p_y, p_z, E)\f$. For instance, an
+ * incoming gluon could be defined as
+ * @code{.cpp}
+ * fastjet::PseudoJet momentum{0, 0, 308., 308.};
+ * HEJ::Particle gluon_in{HEJ::ParticleID::gluon, momentum};
+ * @endcode
+ * We collect all incoming and outgoing particles in a partonic event. Here
+ * is an example for a partonic \f$gu \to gghu\f$ event:
+ * @code{.cpp}
+ * HEJ::UnclusteredEvent partonic_event;
+ *
+ * // incoming particles
+ * partonic_event.incoming[0] = {
+ * HEJ::ParticleID::gluon,
+ * { 0., 0., 308., 308.}
+ * };
+ * partonic_event.incoming[1] = {
+ * HEJ::ParticleID::up,
+ * { 0., 0.,-164., 164.}
+ * };
+ * // outgoing particles
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::higgs,
+ * { 98., 82., 14., 180.}
+ * });
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::up,
+ * { 68.,-54., 36., 94.}
+ * });
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::gluon,
+ * {-72., 9., 48., 87.}
+ * });
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::gluon,
+ * {-94.,-37., 46., 111.}
+ * });
+ * @endcode
+ * Alternatively, we could read the event from a Les Houches event file,
+ * possibly compressed with gzip. For this, the additional header
+ * files @c HEJ/stream.hh and @c LHEF/LHEF.h have to be
+ * included.
+ * @code{.cpp}
+ * HEJ::istream in{"events.lhe.gz"};
+ * LHEF::Reader reader{in};
+ * reader.readEvent();
+ * HEJ::UnclusteredEvent partonic_event{reader.hepeup};
+ * @endcode
+ *
+ * In this specific example we will later choose a constant value for the
+ * strong coupling, so that the HEJ matrix element does not depend on the
+ * renormalisation scale. However, in a more general scenario, we will want
+ * to set a central scale:
+ * @code{.cpp}
+ * partonic_event.central.mur = 50.;
+ * @endcode
+ * It is possible to add more scales in order to perform scale variation:
+ * @code{.cpp}
+ * partonic_event.variations.resize(2);
+ * partonic_event.variations[0].mur = 25.;
+ * partonic_event.variations[1].mur = 100.;
+ * @endcode
+ *
+ * In the next step, we leverage FastJet to construct an event with
+ * clustered jets. Here, we use antikt jets with R=0.4 and transverse
+ * momenta of at least 30 GeV.
+ * @code{.cpp}
+ * const fastjet::JetDefinition jet_def{
+ * fastjet::JetAlgorithm::antikt_algorithm, 0.4
+ * };
+ * const double min_jet_pt = 30.;
+ * HEJ::Event event{partonic_event, jet_def, min_jet_pt};
+ * @endcode
+ * In order to calculate the Matrix element, we now have to fix the physics
+ * parameters. For the sake of simplicity, we assume an effective coupling
+ * of the Higgs boson to gluons in the limit of an infinite top-quark mass
+ * and a fixed value of $\alpha_s = 0.118$ for the strong coupling.
+ * @code{.cpp}
+ * const auto alpha_s = [](double /* mu_r */) { return 0.118; };
+ * HEJ::MatrixElementConfig ME_config;
+ * // whether to include corrections from the
+ * // evolution of \alpha_s in virtual corrections
+ * ME_config.log_correction = false;
+ * HEJ::MatrixElement ME{alpha_s, ME_config};
+ * @endcode
+ * If QCDLoop is installed, we can also take into account the full loop
+ * effects with finite top and bottom quark masses:
+ * @code{.cpp}
+ * HEJ::MatrixElementConfig ME_config;
+ * ME_config.Higgs_coupling.use_impact_factors = false;
+ * ME_config.Higgs_coupling.mt = 163;
+ * ME_config.Higgs_coupling.include_bottom = true;
+ * ME_config.Higgs_coupling.mb = 2.8;
+ * @endcode
+ * Finally, we can compute and print the square of the matrix element with
+ * @code{.cpp}
+ * std::cout << "HEJ ME: " << ME(event).central << '\n';
+ * @endcode
+ * In the case of scale variation, the weight associated with the scale
+ * @c event.variations[i].mur is @c ME(event).variations[i].
+ *
+ * Collecting the above pieces, we have the following program:
+ * @code{.cpp}
+ * #include "HEJ/Event.hh"
+ * #include "HEJ/MatrixElement.hh"
+ *
+ * int main(){
+ * HEJ::UnclusteredEvent partonic_event;
+ * // incoming particles
+ * partonic_event.incoming[0] = {
+ * HEJ::ParticleID::gluon,
+ * { 0., 0., 308., 308.}
+ * };
+ * partonic_event.incoming[1] = {
+ * HEJ::ParticleID::up,
+ * { 0., 0.,-164., 164.}
+ * };
+ * // outgoing particles
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::higgs,
+ * { 98., 82., 14., 180.}
+ * });
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::up,
+ * { 68.,-54., 36., 94.}
+ * });
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::gluon,
+ * {-72., 9., 48., 87.}
+ * });
+ * partonic_event.outgoing.push_back({
+ * HEJ::ParticleID::gluon,
+ * {-94.,-37., 46., 111.}
+ * });
+ *
+ * const fastjet::JetDefinition jet_def{
+ * fastjet::JetAlgorithm::antikt_algorithm, 0.4
+ * };
+ * const double min_jet_pt = 30.;
+ * HEJ::Event event{partonic_event, jet_def, min_jet_pt};
+ *
+ * const auto alpha_s = [](double /* mu_r */) { return 0.118; };
+ * HEJ::MatrixElementConfig ME_config;
+ * // whether to include corrections from the
+ * // evolution of \alpha_s in virtual corrections
+ * ME_config.log_correction = false;
+ * HEJ::MatrixElement ME{alpha_s, ME_config};
+ *
+ * std::cout
+ * << "HEJ ME: " << ME(event).central
+ * << " = tree * virtual = " << ME.tree(event).central
+ * << " * " << ME.virtual_corrections(event).central
+ * << '\n';
+ * }
+ * @endcode
+ * After saving the above code to a file @c matrix_element.cc, it
+ * can be compiled into an executable @c matrix_element with a
+ * suitable compiler. For example, with @c g++ this can be done
+ * with the command
+ * @code{.sh}
+ * g++ -o matrix_element matrix_element.cc -lHEJ -lfastjet
+ * @endcode
+ * If HEJ or any of the required libraries was installed to a
+ * non-standard location, it may be necessary to explicitly specify the
+ * paths to the required header and library files. This can be done with
+ * the @c HEJ-config executable and similar programs for the
+ * other dependencies:
+ * @code{.sh}
+ * g++ $(fastjet-config --cxxflags) $(HEJ-config --cxxflags) -o matrix_element matrix_element.cc $(HEJ-config --libs) $(fastjet-config --libs)
+ * @endcode
*/
}
diff --git a/doc/sphinx/HEJ.rst b/doc/sphinx/HEJ.rst
index d73349b..83df36f 100644
--- a/doc/sphinx/HEJ.rst
+++ b/doc/sphinx/HEJ.rst
@@ -1,281 +1,289 @@
.. _`Running HEJ 2`:
Running HEJ 2
=============
Quick start
-----------
In order to run HEJ 2, you need a configuration file and a file
containing fixed-order events. A sample configuration is given by the
:file:`config.yml` file distributed together with HEJ 2. Events
in the Les Houches Event File format can be generated with standard
Monte Carlo generators like `MadGraph5_aMC@NLO
<https://launchpad.net/mg5amcnlo>`_ or `Sherpa
<https://sherpa.hepforge.org/trac/wiki>`_. HEJ 2 assumes that the
cross section is given by the sum of the event weights. Depending on the
fixed-order generator it may be necessary to adjust the weights in the
Les Houches Event File accordingly.
The processes supported by HEJ 2 are
- Pure multijet production
- Production of a Higgs boson with jets
..
- *TODO* Production of a W boson with jets
- *TODO* Production of a Z boson or photon with jets
where at least two jets are required in each case. For the time being,
only leading-order events are supported.
After generating an event file :file:`events.lhe` adjust the parameters
under the `fixed order jets`_ setting in :file:`config.yml` to the
settings in the fixed-order generation. Resummation can then be added by
running::
HEJ config.yml events.lhe
Using the default settings, this will produce an output event file
:file:`HEJ.lhe` with events including high-energy resummation.
+When using the `Docker image <https://hub.docker.com/r/hejdock/hej>`_,
+HEJ can be run with
+
+.. code-block:: bash
+
+ docker run -v $PWD:$PWD -w $PWD hejdock/hej HEJ config.yml events.lhe
+
.. _`HEJ 2 settings`:
Settings
--------
HEJ 2 configuration files follow the `YAML <http://yaml.org/>`_
format. The following configuration parameters are supported:
.. _`trials`:
**trials**
High-energy resummation is performed by generating a number of
- resummation phase space configurations corresponding to the input
+ resummation phase space configurations corresponding to an input
fixed-order event. This parameter specifies how many such
configurations HEJ 2 should try to generate for each input
event. Typical values vary between 10 and 100.
.. _`min extparton pt`:
**min extparton pt**
Specifies the minimum transverse momentum in GeV of the most forward
and the most backward parton. This setting is needed to regulate an
otherwise uncancelled divergence. Its value should be slightly below
the minimum transverse momentum of jets specified by `resummation
jets: min pt`_. See also the `max ext soft pt fraction`_ setting.
.. _`max ext soft pt fraction`:
**max ext soft pt fraction**
Specifies the maximum fraction that soft radiation can contribute to
the transverse momentum of each the most forward and the most backward
jet. Values between around 0.05 and 0.1 are recommended. See also the
`min extparton pt`_ setting.
.. _`fixed order jets`:
**fixed order jets**
This tag collects a number of settings specifying the jet definition
in the event input. The settings should correspond to the ones used in
the fixed-order Monte Carlo that generated the input events.
.. _`fixed order jets: min pt`:
**min pt**
Minimum transverse momentum in GeV of fixed-order jets.
.. _`fixed order jets: algorithm`:
**algorithm**
The algorithm used to define jets. Allowed settings are
:code:`kt`, :code:`cambridge`, :code:`antikt`,
:code:`cambridge for passive`. See the `FastJet
<http://fastjet.fr/>`_ documentation for a description of these
algorithms.
.. _`fixed order jets: R`:
**R**
The R parameter used in the jet algorithm, roughly corresponding
to the jet radius in the plane spanned by the rapidity and the
azimuthal angle.
.. _`resummation jets`:
**resummation jets**
This tag collects a number of settings specifying the jet definition
in the observed, i.e. resummed events. These settings are optional, by
default the same values as for the `fixed order jets`_ are assumed.
.. _`resummation jets: min pt`:
**min pt**
Minimum transverse momentum in GeV of resummation jets. This
should be between 25% and 50% larger than the minimum transverse
momentum of fixed order jets set by `fixed order jets: min pt`_.
.. _`resummation jets: algorithm`:
**algorithm**
The algorithm used to define jets. The HEJ 2 approach to
resummation relies on properties of :code:`antikt` jets, so this
value is strongly recommended. For a list of possible other
values, see the `fixed order jets: algorithm`_ setting.
.. _`resummation jets: R`:
**R**
The R parameter used in the jet algorithm.
.. _`FKL`:
**FKL**
- Specifies how to treat FKL events. The possible values are
- :code:`reweight` to enable resummation, :code:`keep` to keep the
- events as they are up to a possible change of renormalisation and
- factorisation scale, and :code:`discard` to discard these events.
+ Specifies how to treat events respecting FKL rapidity ordering. These
+ configurations are dominant in the high-energy limit. The possible
+ values are :code:`reweight` to enable resummation, :code:`keep` to
+ keep the events as they are up to a possible change of
+ renormalisation and factorisation scale, and :code:`discard` to
+ discard these events.
.. _`unordered`:
**unordered**
Specifies how to treat events with one emission that does not respect
- FKL ordering. The possible values are the same as for the `FKL`_
- setting, but :code:`reweight` may not be supported for all process
- types.
-
+ FKL ordering. In the high-energy limit, such configurations are
+ logarithmically suppressed compared to FKL configurations. The
+ possible values are the same as for the `FKL`_ setting, but
+ :code:`reweight` is currently only supported for Higgs boson plus
+ jets production.
.. _`non-HEJ`:
**non-HEJ**
Specifies how to treat events where no resummation is possible. The
allowed values are :code:`keep` to keep the events as they are up to
a possible change of renormalisation and factorisation scale and
:code:`discard` to discard these events.
.. _`scales`:
**scales**
Specifies the renormalisation and factorisation scales for the output
events. This can either be a single entry or a list :code:`[scale1,
scale2, ...]`. For the case of a list the first entry defines the
central scale. Possible values are fixed numbers to set the scale in
GeV or the following:
- :code:`H_T`: The sum of the scalar transverse momenta of all
final-state particles
- :code:`max jet pperp`: The maximum transverse momentum of all jets
- :code:`jet invariant mass`: Sum of the invariant masses of all jets
- :code:`m_j1j2`: Invariant mass between the two hardest jets.
Scales can be multiplied or divided by an overall factor,
e.g. :code:`H_T/2`.
It is also possible to import scales from an external library, see
:ref:`Custom scales`
.. _`scale factors`:
**scale factors**
A list of numeric factors by which each of the `scales`_ should be
multiplied. Renormalisation and factorisation scales are varied
independently. For example, a list with entries :code:`[0.5, 2]`
would give the four scale choices (0.5μ\ :sub:`r`, 0.5μ\ :sub:`f`);
(0.5μ\ :sub:`r`, 2μ\ :sub:`f`); (2μ\ :sub:`r`, 0.5μ\ :sub:`f`); (2μ\
:sub:`r`, 2μ\ :sub:`f`) in this order. The ordering corresponds to
the order of the final event weights.
.. _`max scale ratio`:
**max scale ratio**
Specifies the maximum factor by which renormalisation and
factorisation scales may difer. For a value of :code:`2` and the
example given for the `scale factors`_ the scale choices
(0.5μ\ :sub:`r`, 2μ\ :sub:`f`) and (2μ\ :sub:`r`, 0.5μ\ :sub:`f`)
will be discarded.
.. _`log correction`:
**log correction**
Whether to include corrections due to the evolution of the strong
coupling constant in the virtual corrections. Allowed values are
:code:`true` and :code:`false`.
-.. TODO: unweight
-
.. _`event output`:
**event output**
Specifies the name of a single event output file or a list of such
files. The file format is either specified explicitly or derived from
the suffix. For example, :code:`events.lhe` or, equivalently
:code:`Les Houches: events.lhe` generates an output event file
:code:`events.lhe` in the Les Houches format. The supported formats
are
- :code:`file.lhe` or :code:`Les Houches: file`: The Les Houches
event file format.
- :code:`file.hepmc` or :code:`HepMC: file`: The HepMC format.
.. _`random generator`:
**random generator**
Sets parameters for random number generation.
.. _`random generator: name`:
**name**
Which random number generator to use. Currently, :code:`mixmax`
- and :code:`ranlux64` are implemented. Mixmax is recommended. See
+ and :code:`ranlux64` are supported. Mixmax is recommended. See
the `CLHEP documentation
<http://proj-clhep.web.cern.ch/proj-clhep/index.html#docu>`_ for
details on the generators.
.. _`random generator: seed`:
**seed**
The seed for random generation. This should be a single number for
- mixmax and the name of a state file for ranlux64.
+ :code:`mixmax` and the name of a state file for :code:`ranlux64`.
.. _`analysis`:
**analysis**
Name and Setting for the event analyses; either a custom
- analysis plugin or rivet. For the first the :code:`plugin` sub-entry
+ analysis plugin or Rivet. For the first the :code:`plugin` sub-entry
should be set to the analysis file path. All further entries are passed on
- to the analysis. To use rivet a list of rivet-analysis have to be
+ to the analysis. To use Rivet a list of Rivet analyses have to be
given in :code:`rivet` and prefix for the yoda file has to be set
through :code:`output`. See :ref:`Writing custom analyses` for details.
.. _`Higgs coupling`:
**Higgs coupling**
This collects a number of settings concerning the effective coupling
of the Higgs boson to gluons. This is only relevant for the
production process of a Higgs boson with jets and only supported if
- HEJ 2 was compiled with `QCDloop
+ HEJ 2 was compiled with `QCDLoop
<https://github.com/scarrazza/qcdloop>`_ support.
.. _`Higgs coupling: use impact factors`:
**use impact factors**
Whether to use impact factors for the coupling to the most forward
and most backward partons. Impact factors imply the infinite
top-quark mass limit.
.. _`Higgs coupling: mt`:
**mt**
The value of the top-quark mass in GeV. If this is not specified,
the limit of an infinite mass is taken.
.. _`Higgs coupling: include bottom`:
**include bottom**
Whether to include the Higgs coupling to bottom quarks.
.. _`Higgs coupling: mb`:
**mb**
The value of the bottom-quark mass in GeV. Only used for the Higgs
coupling, external bottom-quarks are always assumed to be massless.
diff --git a/doc/sphinx/HEJFOG.rst b/doc/sphinx/HEJFOG.rst
index 02c1e89..1a5c8d8 100644
--- a/doc/sphinx/HEJFOG.rst
+++ b/doc/sphinx/HEJFOG.rst
@@ -1,291 +1,299 @@
The HEJ Fixed Order Generator
=============================
For high jet multiplicities event generation with standard fixed-order
generators becomes increasingly cumbersome. For example, the
leading-order production of a Higgs Boson with five or more jets is
computationally prohibitively expensive.
To this end, HEJ 2 provides the ``HEJFOG`` fixed-order generator
that allows to generate events with high jet multiplicities. To
facilitate the computation the limit of Multi-Regge Kinematics with
large invariant masses between all outgoing particles is assumed in the
matrix elements. The typical use of the ``HEJFOG`` is to supplement
low-multiplicity events from standard generators with high-multiplicity
events before using the HEJ 2 program to add high-energy
resummation.
Installation
------------
The ``HEJFOG`` comes bundled together with HEJ 2 and the
installation is very similar. After downloading HEJ 2 and
installing the prerequisites as described in :ref:`Installation` the
``HEJFOG`` can be installed with::
- cmake /path/to/FixedOrderGen -DCMAKE_INSTALL_PREFIX=target/directory -DCMAKE_BUILD_TYPE=Release
+ cmake /path/to/FixedOrderGen -DCMAKE_INSTALL_PREFIX=target/directory
make install
where :file:`/path/to/FixedOrderGen` refers to the :file:`FixedOrderGen`
subdirectory in the HEJ 2 directory. If HEJ 2 was
installed to a non-standard location, it may be necessary to specify the
directory containing :file:`HEJ-config.cmake`. If the base installation
directory is :file:`/path/to/HEJ`, :file:`HEJ-config.cmake` should be
found in :file:`/path/to/HEJ/lib/cmake/HEJ` and the commands for
installing the ``HEJFOG`` would read::
- cmake /path/to/FixedOrderGen -DHEJ_DIR=/path/to/HEJ/lib/cmake/HEJ -DCMAKE_INSTALL_PREFIX=target/directory -DCMAKE_BUILD_TYPE=Release
+ cmake /path/to/FixedOrderGen -DHEJ_DIR=/path/to/HEJ/lib/cmake/HEJ -DCMAKE_INSTALL_PREFIX=target/directory
make install
The installation can be tested with::
make test
-provided that the NNPDF 3.0 PDF set is installed.
+provided that the CT10nlo PDF set is installed.
Running the fixed-order generator
---------------------------------
After installing the ``HEJFOG`` you can modify the provided
configuration file :file:`configFO.yml` and run the generator with::
HEJFOG configFO.yml
The resulting event file, by default named :file:`HEJFO.lhe`, can then be
fed into HEJ 2 like any event file generated from a standard
fixed-order generator, see :ref:`Running HEJ 2`.
Settings
--------
Similar to HEJ 2, the ``HEJFOG`` uses a `YAML
<http://yaml.org/>`_ configuration file. The settings are
.. _`process`:
**process**
The scattering process for which events are being generated. The
format is
:code:`in1 in2 => out1 out2 ...`
The incoming particles, :code:`in1`, :code:`in2` can be
- quarks: :code:`u`, :code:`d`, :code:`u_bar`, and so on
- gluons: :code:`g`
- protons :code:`p` or antiprotons :code:`p_bar`
At most one of the outgoing particles can be a boson, the rest has to be
partonic. At the moment only the Higgs boson :code:`h` is supported. All
other outgoing particles are jets. Multiple jets can be grouped together, so
:code:`p p => h j j` is the same as :code:`p p => h 2j`. There have to be at
least two jets. Further decays of the boson can be added through the
:ref:`particle properties<particle properties: particle: decays>`.
.. _`events`:
**events**
Specifies the number of events to generate.
.. _`jets`:
**jets**
Defines the properties of the generated jets.
.. _`jets: min pt`:
**min pt**
Minimum jet transverse momentum in GeV.
.. _`jets: peak pt`:
**peak pt**
Optional setting to specify the dominant jet transverse momentum
in GeV. If the generated events are used as input for HEJ
resummation, this should be set to the minimum transverse momentum
of the resummation jets. The effect is that only a small fraction
of jets will be generated with a transverse momentum below the
value of this setting.
.. _`jets: algorithm`:
**algorithm**
The algorithm used to define jets. Allowed settings are
:code:`kt`, :code:`cambridge`, :code:`antikt`,
:code:`cambridge for passive`. See the `FastJet
<http://fastjet.fr/>`_ documentation for a description of these
algorithms.
.. _`jets: R`:
**R**
The R parameter used in the jet algorithm.
.. _`jets: max rapidity`:
**max rapidity**
Maximum absolute value of the jet rapidity.
.. _`beam`:
**beam**
Defines various properties of the collider beam.
.. _`beam: energy`:
**energy**
The beam energy in GeV. For example, the 13
TeV LHC corresponds to a value of 6500.
.. _`beam: particles`:
**particles**
A list :code:`[p1, p2]` of two beam particles. The only supported
entries are protons :code:`p` and antiprotons :code:`p_bar`.
.. _`pdf`:
**pdf**
The `LHAPDF number <https://lhapdf.hepforge.org/pdfsets>`_ of the PDF set.
For example, 230000 corresponds to an NNPDF 2.3 NLO PDF set.
.. _`subleading fraction`:
**subleading fraction**
- This setting is related to the fraction of events, that are not a FKL
- configuration. All possible subleading process are listed in
- :ref:`subleading channels<subleading channels>`. Typically, this value
- should be between 0.01 and 0.1.
+ This setting is related to the fraction of events, that are not a
+ FKL configuration. All possible subleading process are listed in
+ :ref:`subleading channels<subleading channels>`. Typically, this
+ value should be between 0.01 and 0.1. Note that while this
+ parameter influences the chance of generating subleading
+ configurations, it generally does not correspond to the actual
+ fraction of subleading events.
.. _`subleading channels`:
**subleading channels**
- Optional parameters to select a specific subleading process, multiple
+
+Optional parameters to select a specific subleading process, multiple
channels can be selected at once. If multiple subleading configurations
are possible one will be selected at random for each event, thus each
final state will include at most one subleading process, e.g. either
:code:`unordered` or :code:`qqx`. The following values are allowed:
- :code:`all`: All channels allowed, default if nothing else set
- :code:`none`: No subleading contribution, only FKL allowed
Equivalent to :code:`subleading fraction: 0`
- :code:`unordered`: Unordered emission allowed
Unordered emission are any rapidity ordering, where exactly one gluon is
emitted outside the rapidity ordering required in FKL events. More
precisely, if at least one of the incoming particles is a quark or
antiquark and there are more than two jets in the final state,
:code:`subleading fraction` states the probability that the flavours
of the outgoing particles are assigned in such a way that an unordered
configuration arises. Unordered emissions are currently not implemented
for pure jet production.
- :code:`qqx`: Production of quark-antiquark pair
If allowed processes with at least three jets might include a
quark-antiquark pair, i.e. one quark (in rapidity) next to one antiquark.
The pair can be at any position in the FKL chain. Similar to above
:code:`subleading fraction` gives the probability of turning two gluons
into the quark-antiquark pair. Quark-antiquark pairs are currently only
implemented for W boson production.
.. _`unweight`:
**unweight**
This setting defines the parameters for the partial unweighting of
events. You can disable unweighting by removing this entry from the
configuration file.
.. _`unweight: sample size`:
**sample size**
The number of weighted events used to calibrate the unweighting.
A good default is to set this to the number of target
`events`_. If the number of `events`_ is large this can
lead to significant memory consumption and a lower value should be
chosen. Contrarily, for large multiplicities the unweighting
efficiency becomes worse and the sample size should be increased.
.. _`unweight: max deviation`:
**max deviation**
Controls the range of events to which unweighting is applied. A
larger value means that a larger fraction of events are unweighted.
Typical values are between -1 and 1.
.. _`particle properties`:
**particle properties**
Specifies various properties of the different particles (Higgs, W or Z).
This is only relevant if the chosen `process`_ is the production of the
corresponding particles with jets. E.g. for the `process`_
:code:`p p => h 2j` the :code:`mass`, :code:`width` and (optionally)
:code:`decays` of the :code:`Higgs` boson are required, while all other
particle properties will be ignored.
.. _`particle properties: particle`:
- **Higgs, Wp, Wm or Z**
- Name of the boson. Can be any of the once above.
+ **Higgs, W+, W- or Z**
+ The particle (Higgs, |W+|, |W-|, Z) for which the following
+ properties are defined.
+
+ .. |W+| replace:: W\ :sup:`+`
+ .. |W-| replace:: W\ :sup:`-`
.. _`particle properties: particle: mass`:
**mass**
The mass of the particle in GeV.
.. _`particle properties: particle: width`:
**width**
The total decay width of the particle in GeV.
.. _`particle properties: particle: decays`:
**decays**
Optional setting specifying the decays of the particle. Only the decay
into two particles is implemented. Each decay has the form
:code:`{into: [p1,p2], branching ratio: r}`
where :code:`p1` and :code:`p2` are the particle names of the
decay product (e.g. :code:`photon`) and :code:`r` is the branching
ratio.
Decays of a Higgs boson are treated as the production and subsequent
decay of an on-shell Higgs boson, so decays into e.g. Z bosons are not
supported.
.. _`scales`:
**scales**
Specifies the renormalisation and factorisation scales for the output
events. For details, see the corresponding entry in the HEJ 2
:ref:`HEJ 2 settings`. Note that this should usually be a
single value, as the weights resulting from additional scale choices
- will simply be ignored by HEJ 2.
+ will simply be ignored when adding high-energy resummation with HEJ 2.
.. _`event output`:
**event output**
Specifies the name of a single event output file or a list of such
files. See the corresponding entry in the HEJ 2
:ref:`HEJ 2 settings` for details.
.. _`RanLux init`:
.. _`random generator`:
**random generator**
Sets parameters for random number generation. See the HEJ 2
:ref:`HEJ 2 settings` for details.
.. _`analysis`:
**analysis**
Specifies the name and settings for a custom analysis library. This
can be useful to specify cuts at the fixed-order level. See the
corresponding entry in the HEJ 2 :ref:`HEJ 2 settings`
for details.
.. _`Higgs coupling`:
**Higgs coupling**
This collects a number of settings concerning the effective coupling
of the Higgs boson to gluons. See the corresponding entry in the
HEJ 2 :ref:`HEJ 2 settings` for details.
diff --git a/doc/sphinx/Makefile b/doc/sphinx/Makefile
index 21721f0..702f121 100644
--- a/doc/sphinx/Makefile
+++ b/doc/sphinx/Makefile
@@ -1,20 +1,20 @@
# Minimal makefile for Sphinx documentation
#
# You can set these variables from the command line.
SPHINXOPTS =
-SPHINXBUILD = python -msphinx
+SPHINXBUILD = python3 -msphinx
SPHINXPROJ = HEJ2
SOURCEDIR = .
BUILDDIR = _build
# Put it first so that "make" without argument is like "make help".
help:
@$(SPHINXBUILD) -M help "$(SOURCEDIR)" "$(BUILDDIR)" $(SPHINXOPTS) $(O)
.PHONY: help Makefile
# Catch-all target: route all unknown targets to Sphinx using the new
# "make mode" option. $(O) is meant as a shortcut for $(SPHINXOPTS).
%: Makefile
@$(SPHINXBUILD) -M $@ "$(SOURCEDIR)" "$(BUILDDIR)" $(SPHINXOPTS) $(O)
diff --git a/doc/sphinx/analyses.rst b/doc/sphinx/analyses.rst
index 3bb59e8..39ec4bc 100644
--- a/doc/sphinx/analyses.rst
+++ b/doc/sphinx/analyses.rst
@@ -1,179 +1,179 @@
.. _`Writing custom analyses`:
Writing custom analyses
=======================
HEJ 2 and the HEJ fixed-order generator can generate HepMC files, so you
-can always run a `rivet <https://rivet.hepforge.org/>`_ analysis on
-these. However if you compiled HEJ 2 with rivet you can use the native
-rivet interface. For example
+can always run a `Rivet <https://rivet.hepforge.org/>`_ analysis on
+these. However if you compiled HEJ 2 with Rivet you can use the native
+Rivet interface. For example
.. code-block:: YAML
analysis:
rivet: [MC_XS, MC_JETS]
output: HEJ
would call the generic
`MC_XS <https://rivet.hepforge.org/analyses/MC_XS.html>`_ and
`MC_JETS <https://rivet.hepforge.org/analyses/MC_JETS.html>`_ analysis
and write the result into :code:`HEJ[.Scalename].yoda`.
-HEJ 2 will then run rivet over all different scales seperatly and
+HEJ 2 will then run Rivet over all different scales seperatly and
write out each into a different yoda file. Alternatively instead
-of using rivet, you can provide a custom analysis inside a C++ library.
+of using Rivet, you can provide a custom analysis inside a C++ library.
An analysis is a class that derives from the abstract :code:`Analysis`
base class provided by HEJ 2. It has to implement three public
functions:
* The :code:`pass_cuts` member function return true if and only if the
given event (first argument) passes the analysis cuts
* The :code:`fill` member function adds an event to the analysis, which
for example can be used to fill histograms. HEJ 2 will only
pass events for which :code:`pass_cuts` has returned true.
* The :code:`finalise` member function is called after all events have
been processed. It can be used, for example, to print out or save the
analysis results.
The :code:`pass_cuts` and :code:`fill` functions take two arguments: the
resummation event generated by HEJ 2 and the original fixed-order
input event. Usually, the second argument can be ignored. It can be
used, for example, for implementing cuts that depend on the ratio of the
weights between the fixed-order and the resummation event.
In addition to the two member functions, there has to be a global
make_analysis function that takes the analysis parameters in the form of
a YAML :code:`Node` and returns a :code:`std::unique_ptr` to the
Analysis.
The following code creates the simplest conceivable analysis.
::
#include <memory> // for std::unique_ptr
#include "HEJ/Analysis.hh"
class MyAnalysis: public HEJ::Analysis {
public:
MyAnalysis(YAML::Node const & /* config */) {}
void fill(
HEJ::Event const & /* event */,
HEJ::Event const & /* FO_event */
) override {
}
bool pass_cuts(
HEJ::Event const & /* event */,
HEJ::Event const & /* FO_event */
) override {
return true;
}
void finalise() override {
}
};
extern "C"
std::unique_ptr<HEJ::Analysis> make_analysis(
YAML::Node const & config
){
return std::make_unique<MyAnalysis>(config);
}
You can save this code to a file, for example :code:`myanalysis.cc`, and
compile it into a shared library. Using the :code:`g++` compiler, the
library can be built with
.. code-block:: sh
g++ $(HEJ-config --cxxflags) -fPIC -shared -Wl,-soname,libmyanalysis.so -o libmyanalysis.so myanalysis.cc
With :code:`g++` it is also good practice to add
:code:`__attribute__((visibility("default")))` after :code:`extern "C"`
in the above code snippet and then compile with the additional flag
:code:`-fvisibility=hidden` to prevent name clashes.
You can use the analysis in HEJ 2 or the HEJ fixed-order
generator by adding
.. code-block:: YAML
analysis:
plugin: /path/to/libmyanalysis.so
to the .yml configuration file.
As a more interesting example, here is the code for an analysis that
sums up the total cross section and prints the result to both standard
output and a file specified in the .yml config with
.. code-block:: YAML
analysis:
plugin: analysis/build/directory/src/libmy_analysis.so
output: outfile
To access the configuration at run time, HEJ 2 uses the yaml-cpp
library; for more details see the `yaml-cpp tutorial
<https://github.com/jbeder/yaml-cpp/wiki/Tutorial>`_. The analysis code
itself is
::
#include <memory>
#include <iostream>
#include <fstream>
#include <string>
#include <cmath>
#include "HEJ/Analysis.hh"
#include "HEJ/Event.hh"
#include "yaml-cpp/yaml.h"
class MyAnalysis: public HEJ::Analysis {
public:
MyAnalysis(YAML::Node const & config):
xsection_{0.}, xsection_error_{0.},
outfile_{config["output"].as<std::string>()}
{}
void fill(
HEJ::Event const & event,
HEJ::Event const & /* FO_event */
) override {
const double wt = event.central().weight;
xsection_ += wt;
xsection_error_ += wt*wt;
}
bool pass_cuts(
HEJ::Event const & /* event */,
HEJ::Event const & /* FO_event */
) override {
return true;
}
void finalise() override {
std::cout << "cross section: " << xsection_ << " +- "
<< std::sqrt(xsection_error_) << "\n";
std::ofstream fout{outfile_};
fout << "cross section: " << xsection_ << " +- "
<< std::sqrt(xsection_error_) << "\n";
}
private:
double xsection_, xsection_error_;
std::string outfile_;
};
extern "C"
std::unique_ptr<HEJ::Analysis> make_analysis(
YAML::Node const & config
){
return std::make_unique<MyAnalysis>(config);
}
diff --git a/doc/sphinx/conf.py b/doc/sphinx/conf.py
index d2a330b..2b87061 100644
--- a/doc/sphinx/conf.py
+++ b/doc/sphinx/conf.py
@@ -1,171 +1,175 @@
# -*- coding: utf-8 -*-
#
# HEJ 2 documentation build configuration file, created by
# sphinx-quickstart on Fri Sep 15 16:13:57 2017.
#
# This file is execfile()d with the current directory set to its
# containing dir.
#
# Note that not all possible configuration values are present in this
# autogenerated file.
#
# All configuration values have a default; values that are commented out
# serve to show the default.
# If extensions (or modules to document with autodoc) are in another directory,
# add these directories to sys.path here. If the directory is relative to the
# documentation root, use os.path.abspath to make it absolute, like shown here.
#
# import os
# import sys
# sys.path.insert(0, os.path.abspath('.'))
# -- General configuration ------------------------------------------------
# If your documentation needs a minimal Sphinx version, state it here.
#
# needs_sphinx = '1.0'
# Add any Sphinx extension module names here, as strings. They can be
# extensions coming with Sphinx (named 'sphinx.ext.*') or your custom
# ones.
extensions = ['sphinx.ext.mathjax',
'sphinx.ext.githubpages']
# Add any paths that contain templates here, relative to this directory.
templates_path = ['_templates']
# The suffix(es) of source filenames.
# You can specify multiple suffix as a list of string:
#
# source_suffix = ['.rst', '.md']
source_suffix = '.rst'
# The master toctree document.
master_doc = 'index'
# General information about the project.
project = u'HEJ 2'
-copyright = u'2017, Jeppe Andersen, Tuomas Hapola, Andreas Maier, Jennifer Smillie'
-author = u'Jeppe Andersen, Tuomas Hapola, Andreas Maier, Jennifer Smillie'
+copyright = u'2017, Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie'
+author = u'Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie'
# The version info for the project you're documenting, acts as replacement for
# |version| and |release|, also used in various other places throughout the
# built documents.
#
# The short X.Y version.
-version = u'0.0.1'
+version = u'2.0'
# The full version, including alpha/beta/rc tags.
-release = u'0.0.1'
+release = u'2.0.3'
# The language for content autogenerated by Sphinx. Refer to documentation
# for a list of supported languages.
#
# This is also used if you do content translation via gettext catalogs.
# Usually you set "language" from the command line for these cases.
language = None
# List of patterns, relative to source directory, that match files and
# directories to ignore when looking for source files.
# This patterns also effect to html_static_path and html_extra_path
exclude_patterns = ['_build', 'Thumbs.db', '.DS_Store']
highlight_language = 'C++'
# The name of the Pygments (syntax highlighting) style to use.
pygments_style = 'sphinx'
# If true, `todo` and `todoList` produce output, else they produce nothing.
todo_include_todos = False
# -- Options for HTML output ----------------------------------------------
# The theme to use for HTML and HTML Help pages. See the documentation for
# a list of builtin themes.
-#
html_theme = 'alabaster'
# Theme options are theme-specific and customize the look and feel of a theme
# further. For a list of options available for each theme, see the
# documentation.
-#
-# html_theme_options = {}
+html_theme_options = {
+ 'body_text': '#000000',
+ 'narrow_sidebar_fg': '#000000',
+ 'sidebar_header': '#000000',
+ 'sidebar_link': '#000000',
+ 'sidebar_text': '#000000'
+}
# Add any paths that contain custom static files (such as style sheets) here,
# relative to this directory. They are copied after the builtin static files,
# so a file named "default.css" will overwrite the builtin "default.css".
-html_static_path = ['_static']
+# html_static_path = ['_static']
# Custom sidebar templates, must be a dictionary that maps document names
# to template names.
#
# This is required for the alabaster theme
# refs: http://alabaster.readthedocs.io/en/latest/installation.html#sidebars
html_sidebars = {
'**': [
'about.html',
'navigation.html',
'relations.html', # needs 'show_related': True theme option to display
'searchbox.html',
'donate.html',
]
}
# -- Options for HTMLHelp output ------------------------------------------
# Output file base name for HTML help builder.
htmlhelp_basename = 'HEJ2doc'
# -- Options for LaTeX output ---------------------------------------------
latex_elements = {
# The paper size ('letterpaper' or 'a4paper').
#
# 'papersize': 'letterpaper',
# The font size ('10pt', '11pt' or '12pt').
#
# 'pointsize': '10pt',
# Additional stuff for the LaTeX preamble.
#
# 'preamble': '',
# Latex figure (float) alignment
#
# 'figure_align': 'htbp',
}
# Grouping the document tree into LaTeX files. List of tuples
# (source start file, target name, title,
# author, documentclass [howto, manual, or own class]).
latex_documents = [
(master_doc, 'HEJ2.tex', u'HEJ 2 Documentation',
- u'Jeppe Andersen, Tuomas Hapola, Andreas Maier, Jennifer Smillie', 'manual'),
+ u'Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie', 'manual'),
]
# -- Options for manual page output ---------------------------------------
# One entry per manual page. List of tuples
# (source start file, name, description, authors, manual section).
man_pages = [
(master_doc, 'hej2', u'HEJ 2 Documentation',
[author], 1)
]
# -- Options for Texinfo output -------------------------------------------
# Grouping the document tree into Texinfo files. List of tuples
# (source start file, target name, title, author,
# dir menu entry, description, category)
texinfo_documents = [
(master_doc, 'HEJ2', u'HEJ 2 Documentation',
author, 'HEJ2', 'One line description of project.',
'Miscellaneous'),
]
diff --git a/doc/sphinx/installation.rst b/doc/sphinx/installation.rst
index a9ead44..2d2b755 100644
--- a/doc/sphinx/installation.rst
+++ b/doc/sphinx/installation.rst
@@ -1,63 +1,78 @@
.. _Installation:
Installation
============
Download
--------
-HEJ 2 is developed using the `git version control system
-<https://git-scm.com/>`_. To get a copy of HEJ 2, install git and
-run::
+A tar archive of the HEJ 2 source code can be downloaded and
+decompressed with the command::
- git clone https://gitlab.dur.scotgrid.ac.uk/hej/hej
+ curl https://hej.web.cern.ch/HEJ/downloads/HEJ_2.0.tar.gz | tar -xz
+
+To obtain the latest stable HEJ version, `HEJ_2.0.tar.gz` should be
+replaced by `HEJ.tar.gz`.
+
+Alternatively, the HEJ source code can be obtained by installing the
+`git version control system <https://git-scm.com/>`_. and running::
+
+ git clone https://phab.hepforge.org/source/hej.git
+
+We also provide a `Docker image <https://hub.docker.com/r/hejdock/hej>`_
+containing a HEJ 2 installation on. This image can be pulled with::
+
+ docker pull hejdock/hej
+
+When using the Docker image the remaining installation steps can be
+skipped.
Prerequisites
-------------
Before installing HEJ 2, you need the following programs and
libraries:
-- `cmake <https://cmake.org/>`_ version 3.1
+- `CMake <https://cmake.org/>`_ version 3.1
- A compiler supporting the C++14 standard, for example `gcc <https://gcc.gnu.org/>`_ 5 or later
- `FastJet <http://fastjet.fr/>`_
- `CLHEP <https://gitlab.cern.ch/CLHEP/CLHEP>`_
- `LHAPDF <https://lhapdf.hepforge.org/>`_
- The `IOStreams` and `uBLAS` `boost <https://www.boost.org>`_ libraries
- `yaml-cpp <https://github.com/jbeder/yaml-cpp>`_
If you want to include finite top mass corrections in Higgs boson + jets
-production, you additionally need version 2 of the `QCDloop
+production, you additionally need version 2 of the `QCDLoop
<https://github.com/scarrazza/qcdloop>`_ library. HEJ 2 supports
versions 2 and 3 of `HepMC <https://hepmc.web.cern.ch/hepmc/>`_ if it is
installed, but does not require it.
Compilation
-----------
To compile and install HEJ 2 run::
- cmake source/directory -DCMAKE_INSTALL_PREFIX=target/directory -DCMAKE_BUILD_TYPE=Release
+ cmake source/directory -DCMAKE_INSTALL_PREFIX=target/directory
make install
:file:`source/directory` is the directory containing the file
:file:`CMakeLists.txt`. If you omit
:code:`-DCMAKE_INSTALL_PREFIX=target/directory` HEJ 2 will be
installed to some default location.
In case some of the aforementioned prerequisites are not found by
:code:`cmake` you can give a hint by adding an additional argument
:code:`-Dlibname_ROOT_DIR=/directory/with/library`, where
:code:`libname` should be replaced by the name of the library in
question.
Testing
-------
To test your installation, download the NNPDF 2.3 PDF set with::
lhapdf install NNPDF23_nlo_as_0119
and run::
make test
diff --git a/include/HEJ/Analysis.hh b/include/HEJ/Analysis.hh
index 02c86ff..003667d 100644
--- a/include/HEJ/Analysis.hh
+++ b/include/HEJ/Analysis.hh
@@ -1,50 +1,47 @@
/** \file
* \brief Header file for the Analysis interface
*
* This header contains declarations that faciliate creating custom analyses
* to be used with HEJ 2.
* \todo link to user documentation
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <vector>
-#include <string>
-
-namespace YAML{
- class Node;
-}
-
//! Main HEJ 2 Namespace
namespace HEJ{
class Event;
//! Analysis base class
/**
* This is the interface that all analyses should implement,
* i.e. all custom analyses have to be derived from this struct.
*/
struct Analysis{
//! Fill event into analysis (e.g. to histograms)
/**
* @param res_event The event in resummation phase space
* @param FO_event The original fixed-order event
*/
virtual void fill(Event const & res_event, Event const & FO_event) = 0;
//! Decide whether an event passes the cuts
/**
* @param res_event The event in resummation phase space
* @param FO_event The original fixed-order event
* @returns Whether the event passes all cuts
*/
virtual bool pass_cuts(Event const & res_event, Event const & FO_event) = 0;
//! Finalise analysis
/**
* This function is called after all events have been processed and
* can be used for example to print out or save the results.
*/
virtual void finalise() = 0;
virtual ~Analysis() = default;
};
}
diff --git a/include/HEJ/CombinedEventWriter.hh b/include/HEJ/CombinedEventWriter.hh
index c21a5fc..160da19 100644
--- a/include/HEJ/CombinedEventWriter.hh
+++ b/include/HEJ/CombinedEventWriter.hh
@@ -1,41 +1,45 @@
/** \file
* \brief Declares the CombinedEventWriter class
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <memory>
#include <vector>
#include "HEJ/EventWriter.hh"
-#include "HEJ/make_writer.hh"
+#include "HEJ/output_formats.hh"
namespace LHEF{
struct HEPRUP;
}
namespace HEJ{
//! Write event output to zero or more output files.
class CombinedEventWriter: public EventWriter{
public:
//!Constructor
/**
* @param outfiles Specifies files output should be written to.
* Each entry in the vector contains a file name
* and output format.
* @param heprup General process information
*/
CombinedEventWriter(
std::vector<OutputFile> const & outfiles,
LHEF::HEPRUP const & heprup
);
//! Write one event to all output files
void write(Event const &) override;
private:
std::vector<std::unique_ptr<EventWriter>> writers_;
};
}
diff --git a/include/HEJ/Constants.hh b/include/HEJ/Constants.hh
index 72e384c..4e2c052 100644
--- a/include/HEJ/Constants.hh
+++ b/include/HEJ/Constants.hh
@@ -1,29 +1,33 @@
/** \file
* \brief Header file defining all global constants used for HEJ
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
namespace HEJ{
/// @name QCD parameters
//@{
constexpr double N_C = 3.; //!< number of Colours
constexpr double C_A = N_C; //!< \f$C_A\f$
constexpr double C_F = (N_C*N_C - 1.)/(2.*N_C); //!< \f$C_F\f$
constexpr double t_f = 0.5; //!< \f$t_f\f$
constexpr double n_f = 5.; //!< number light flavours
constexpr double beta0 = 11./3.*C_A - 4./3.*t_f*n_f; //!< \f$\beta_0\f$
//@}
/// @name QFT parameters
//@{
constexpr double vev = 246.2196508; //!< Higgs vacuum expectation value in GeV
constexpr double gw = 0.653233;
constexpr double MW = 80.419; // The W mass in GeV/c^2
constexpr double GammaW = 2.0476; // the W width in GeV/c^2
//@}
/// @name Generation Parameters
//@{
constexpr double CLAMBDA = 0.2; //!< Scale for virtual correction, \f$\lambda\f$ cf. eq. (20) in \cite Andersen:2011hs
constexpr double CMINPT = CLAMBDA; //!< minimal \f$p_t\f$ of all partons
//@}
}
diff --git a/include/HEJ/EmptyAnalysis.hh b/include/HEJ/EmptyAnalysis.hh
index 8572d11..f0d1933 100644
--- a/include/HEJ/EmptyAnalysis.hh
+++ b/include/HEJ/EmptyAnalysis.hh
@@ -1,44 +1,48 @@
/** \file
* \brief Declaration of the trivial (empty) analysis
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <memory>
#include "HEJ/Analysis.hh"
//! YAML Namespace
namespace YAML{
class Node;
}
namespace HEJ{
/** An analysis that does nothing
*
* This analysis is used by default if no user analysis is specified.
* The member functions don't do anything and events passed to the
* analysis are simply ignored.
*/
struct EmptyAnalysis: Analysis{
static std::unique_ptr<Analysis> create(YAML::Node const & parameters);
//! Fill event into analysis (e.g. to histograms)
/**
* This function does nothing
*/
virtual void fill(Event const &, Event const &) override;
//! Whether a resummation event passes all cuts
/**
* There are no cuts, so all events pass
*/
virtual bool pass_cuts(Event const &, Event const &) override;
//! Finalise analysis
/**
* This function does nothing
*/
virtual void finalise() override;
virtual ~EmptyAnalysis() override = default;
};
}
diff --git a/include/HEJ/Event.hh b/include/HEJ/Event.hh
index 51f9f50..6b59620 100644
--- a/include/HEJ/Event.hh
+++ b/include/HEJ/Event.hh
@@ -1,186 +1,199 @@
/** \file
* \brief Declares the Event class and helpers
*
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <string>
+#include <array>
#include <memory>
+#include <string>
#include <unordered_map>
+#include <vector>
-#include "HEJ/utility.hh"
#include "HEJ/event_types.hh"
-#include "LHEF/LHEF.h"
-#include "fastjet/JetDefinition.hh"
+#include "HEJ/Particle.hh"
+
#include "fastjet/ClusterSequence.hh"
+namespace LHEF{
+ class HEPEUP;
+ class HEPRUP;
+}
+
+namespace fastjet{
+ class JetDefinition;
+}
+
namespace HEJ{
struct ParameterDescription;
//! Event parameters
struct EventParameters{
double mur; /**< Value of the Renormalisation Scale */
double muf; /**< Value of the Factorisation Scale */
double weight; /**< Event Weight */
//! Optional description
std::shared_ptr<ParameterDescription> description = nullptr;
};
//! Description of event parameters
struct ParameterDescription {
//! Name of central scale choice (e.g. "H_T/2")
std::string scale_name;
//! Actual renormalisation scale divided by central scale
double mur_factor;
//! Actual factorisation scale divided by central scale
double muf_factor;
ParameterDescription() = default;
ParameterDescription(
std::string scale_name, double mur_factor, double muf_factor
):
scale_name{scale_name}, mur_factor{mur_factor}, muf_factor{muf_factor}
{};
};
//! An event before jet clustering
struct UnclusteredEvent{
//! Default Constructor
UnclusteredEvent() = default;
//! Constructor from LesHouches event information
UnclusteredEvent(LHEF::HEPEUP const & hepeup);
std::array<Particle, 2> incoming; /**< Incoming Particles */
std::vector<Particle> outgoing; /**< Outgoing Particles */
//! Particle decays in the format {outgoing index, decay products}
std::unordered_map<size_t, std::vector<Particle>> decays;
//! Central parameter (e.g. scale) choice
EventParameters central;
std::vector<EventParameters> variations; /**< For parameter variation */
};
/** An event with clustered jets
*
* This is the main HEJ 2 event class.
* It contains kinematic information including jet clustering,
* parameter (e.g. scale) settings and the event weight.
*/
class Event{
public:
//! Default Event Constructor
Event() = default;
//! Event Constructor adding jet clustering to an unclustered event
Event(
UnclusteredEvent ev,
fastjet::JetDefinition const & jet_def, double min_jet_pt
);
//! The jets formed by the outgoing partons
std::vector<fastjet::PseudoJet> jets() const;
//! The corresponding event before jet clustering
UnclusteredEvent const & unclustered() const {
return ev_;
}
//! Central parameter choice
EventParameters const & central() const{
return ev_.central;
}
//! Central parameter choice
EventParameters & central(){
return ev_.central;
}
//! Incoming particles
std::array<Particle, 2> const & incoming() const{
return ev_.incoming;
}
//! Outgoing particles
std::vector<Particle> const & outgoing() const{
return ev_.outgoing;
}
//! Particle decays
/**
* The key in the returned map corresponds to the index in the
* vector returned by outgoing()
*/
std::unordered_map<size_t, std::vector<Particle>> const & decays() const{
return ev_.decays;
}
//! Parameter (scale) variations
std::vector<EventParameters> const & variations() const{
return ev_.variations;
}
//! Parameter (scale) variations
std::vector<EventParameters> & variations(){
return ev_.variations;
}
//! Parameter (scale) variation
/**
* @param i Index of the requested variation
*/
EventParameters const & variations(size_t i) const{
return ev_.variations[i];
}
//! Parameter (scale) variation
/**
* @param i Index of the requested variation
*/
EventParameters & variations(size_t i){
return ev_.variations[i];
}
//! Indices of the jets the outgoing partons belong to
/**
* @param jets Jets to be tested
* @returns A vector containing, for each outgoing parton,
* the index in the vector of jets the considered parton
* belongs to. If the parton is not inside any of the
* passed jets, the corresponding index is set to -1.
*/
std::vector<int> particle_jet_indices(
std::vector<fastjet::PseudoJet> const & jets
) const{
return cs_.particle_jet_indices(jets);
}
//! Jet definition used for clustering
fastjet::JetDefinition const & jet_def() const{
return cs_.jet_def();
}
//! Minimum jet transverse momentum
double min_jet_pt() const{
return min_jet_pt_;
}
//! Event type
event_type::EventType type() const{
return type_;
}
private:
UnclusteredEvent ev_;
fastjet::ClusterSequence cs_;
double min_jet_pt_;
event_type::EventType type_;
};
//! Square of the partonic centre-of-mass energy \f$\hat{s}\f$
double shat(Event const & ev);
//! Convert an event to a LHEF::HEPEUP
LHEF::HEPEUP to_HEPEUP(Event const & event, LHEF::HEPRUP *);
}
diff --git a/include/HEJ/EventReweighter.hh b/include/HEJ/EventReweighter.hh
index 8e33d2d..b6b1c2d 100644
--- a/include/HEJ/EventReweighter.hh
+++ b/include/HEJ/EventReweighter.hh
@@ -1,181 +1,190 @@
/** \file
* \brief Declares the EventReweighter class
*
* EventReweighter is the main class used within HEJ 2. It reweights the
* resummation events.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include "fastjet/PseudoJet.hh"
-#include "fastjet/ClusterSequence.hh"
-
-#include "LHEF/LHEF.h"
+#include <array>
+#include <functional>
+#include <utility>
+#include <vector>
#include "HEJ/config.hh"
-#include "HEJ/PDF.hh"
-#include "HEJ/utility.hh"
-#include "HEJ/Event.hh"
#include "HEJ/event_types.hh"
-#include "HEJ/PhaseSpacePoint.hh"
#include "HEJ/MatrixElement.hh"
+#include "HEJ/PDF.hh"
+#include "HEJ/PDG_codes.hh"
#include "HEJ/RNG.hh"
+#include "HEJ/ScaleFunction.hh"
+
+namespace LHEF {
+ class HEPRUP;
+}
namespace HEJ{
+ class Event;
+ class Weights;
//! Beam parameters
/**
* Currently, only symmetric beams are supported,
* so there is a single beam energy.
*/
struct Beam{
double E; /**< Beam energy */
std::array<ParticleID, 2> type; /**< Beam particles */
};
//! Main class for reweighting events in HEJ.
class EventReweighter{
using EventType = event_type::EventType;
public:
EventReweighter(
Beam beam, /**< Beam Energy */
int pdf_id, /**< PDF ID */
ScaleGenerator scale_gen, /**< Scale settings */
EventReweighterConfig conf, /**< Configuration parameters */
HEJ::RNG & ran /**< Random number generator */
);
EventReweighter(
LHEF::HEPRUP const & heprup, /**< LHEF event header */
ScaleGenerator scale_gen, /**< Scale settings */
EventReweighterConfig conf, /**< Configuration parameters */
HEJ::RNG & ran /**< Random number generator */
);
//! Get the used pdf
PDF const & pdf() const;
//! Generate resummation events for a given fixed-order event
/**
* @param ev Fixed-order event corresponding
* to the resummation events
* @param num_events Number of trial resummation configurations.
* @returns A vector of resummation events.
*
* The result vector depends on the type of the input event and the
* treatment of different types as specified in the constructor:
*
* \ref reweight The result vector contains between
* 0 and num_events resummation events.
*
* \ref keep If the input event passes the resummation jet cuts
* the result vector contains one event. Otherwise it is empty.
*
* \ref discard The result vector is empty
*/
std::vector<Event> reweight(
Event const & ev,
int num_events
);
private:
template<typename... T>
PDF const & pdf(T&& ...);
/** \internal
* \brief main generation/reweighting function:
* generate phase space points and divide out Born factors
*/
std::vector<Event> gen_res_events(
Event const & ev, int num_events
);
std::vector<Event> rescale(
Event const & Born_ev, std::vector<Event> events
) const;
/** \internal
* \brief Do the Jets pass the resummation Cuts?
*
* @param ev Event in Question
* @returns 0 or 1 depending on if ev passes Jet Cuts
*/
bool jets_pass_resummation_cuts(Event const & ev) const;
/** \internal
* \brief pdf_factors Function
*
* @param ev Event in Question
* @returns EventFactor due to PDFs
*
* Calculates the Central value and the variation due
* to the PDF choice made.
*/
Weights pdf_factors(Event const & ev) const;
/** \internal
* \brief matrix_elements Function
*
* @param ev Event in question
* @returns EventFactor due to MatrixElements
*
* Calculates the Central value and the variation due
* to the Matrix Element.
*/
Weights matrix_elements(Event const & ev) const;
/** \internal
* \brief Scale-dependent part of fixed-order matrix element
*
* @param ev Event in question
* @returns EventFactor scale variation due to FO-ME.
*
* This is only called to compute the scale variation for events where
* we don't do resummation (e.g. non-FKL).
* Since at tree level the scale dependence is just due to alpha_s,
* it is enough to return the alpha_s(mur) factors in the matrix element.
* The rest drops out in the ratio of (output event ME)/(input event ME),
* so we never have to compute it.
*/
Weights fixed_order_scale_ME(Event const & ev) const;
/** \internal
* \brief Computes the tree level matrix element
*
* @param ev Event in Question
* @returns HEJ approximation to Tree level Matrix Element
*
* This computes the HEJ approximation to the tree level FO
* Matrix element which is used within the LO weighting process.
*/
double tree_matrix_element(Event const & ev) const;
//! \internal General parameters
EventReweighterConfig param_;
//! \internal Beam energy
double E_beam_;
//! \internal PDF
PDF pdf_;
//! \internal Object to calculate the square of the matrix element
MatrixElement MEt2_;
//! \internal Object to calculate event renormalisation and factorisation scales
ScaleGenerator scale_gen_;
/** \internal random number generator
*
* \note We use a reference_wrapper so that EventReweighter objects can
* still be copied (which would be impossible with a reference).
*/
std::reference_wrapper<HEJ::RNG> ran_;
};
template<typename... T>
PDF const & EventReweighter::pdf(T&&... t){
return pdf_ = PDF{std::forward<T>(t)...};
}
}
diff --git a/include/HEJ/EventWriter.hh b/include/HEJ/EventWriter.hh
index cd1714b..997a510 100644
--- a/include/HEJ/EventWriter.hh
+++ b/include/HEJ/EventWriter.hh
@@ -1,20 +1,21 @@
/** \file
* \brief Header file for the EventWriter interface.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <string>
-#include <exception>
-
namespace HEJ{
class Event;
//! Pure abstract base class for event writers
struct EventWriter{
//! Write an event
virtual void write(Event const &) = 0;
virtual ~EventWriter() = default;
};
}
diff --git a/include/HEJ/HepMCInterface.hh b/include/HEJ/HepMCInterface.hh
index 9db003f..b920dbf 100644
--- a/include/HEJ/HepMCInterface.hh
+++ b/include/HEJ/HepMCInterface.hh
@@ -1,71 +1,73 @@
/** \file
* \brief Header file for the HepMCInterface
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <cstddef>
-
-#include "LHEF/LHEF.h"
+#include <sys/types.h>
+#include <vector>
namespace HepMC{
- class GenEvent;
class GenCrossSection;
- class GenRunInfo;
+ class GenEvent;
}
namespace HEJ{
class Event;
class EventParameters;
//! This class converts the Events into HepMC::GenEvents
/**
* \details The output is depended on the HepMC version HEJ is compiled with,
* both HepMC 2 and HepMC 3 are supported. If HEJ 2 is compiled
* without HepMC calling this interface will throw an error.
*
* This interface will also keep track of the cross section of all the events that
* being fed into it.
*/
class HepMCInterface{
public:
HepMCInterface();
/**
* \brief main function to convert an event into HepMC::GenEvent
*
* \param event Event to convert
* \param weight_index optional selection of specific weight
* (negative value gives central weight)
*/
HepMC::GenEvent operator()(Event const & event, ssize_t weight_index = -1);
/**
* \brief initialise the event kinematics (everything but the weights)
*
* \param event Event to convert
* \param weight_index optional selection of specific weight
* (negative value gives central weight)
*/
HepMC::GenEvent init_kinematics(Event const & event);
/**
* \brief Sets the central value from \p event to \p out_ev
*
* \param out_ev HepMC::GenEvent to write to
* \param event Event to convert
* \param weight_index optional selection of specific weight
* (negative value gives "central")
*/
void set_central(HepMC::GenEvent & out_ev, Event const & event,
ssize_t weight_index = -1);
/**
* \brief Add the event \p variations to \p out_ev
*/
void add_variation(HepMC::GenEvent & out_ev,
std::vector<EventParameters> const & variations);
private:
size_t event_count_;
double tot_weight_;
double tot_weight2_;
HepMC::GenCrossSection cross_section() const;
};
}
diff --git a/include/HEJ/HepMCWriter.hh b/include/HEJ/HepMCWriter.hh
index be6d962..f696713 100644
--- a/include/HEJ/HepMCWriter.hh
+++ b/include/HEJ/HepMCWriter.hh
@@ -1,48 +1,55 @@
/** \file
* \brief Contains the EventWriter for HepMC Output.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
+#include <memory>
#include <string>
#include "HEJ/EventWriter.hh"
-#include "LHEF/LHEF.h"
+namespace LHEF {
+ class HEPRUP;
+}
namespace HEJ{
class Event;
//! This is an event writer specifically for HepMC output.
/**
* \internal Implementation note:
* This uses the pimpl ("pointer to implementation") idiom.
* HepMC support is optional and the implementation depends on the
* HepMC version. Without pimpl, we would have to specify the HepMC version
* via the preprocessor whenever this header is included. We don't want to
* burden users of the HEJ library (for example the HEJ fixed-order generator)
* with those details
*/
class HepMCWriter: public EventWriter{
public:
//! Constructor
/**
* @param file name of the output file
* @param heprup general process information
*/
HepMCWriter(std::string const & file, LHEF::HEPRUP heprup);
~HepMCWriter() override = default;
//! Write an event to the output file
void write(Event const & ev) override;
private:
struct HepMCWriterImpl;
struct HepMCWriterImplDeleter {
void operator()(HepMCWriterImpl* p);
};
std::unique_ptr<HepMCWriterImpl, HepMCWriterImplDeleter> impl_;
};
}
diff --git a/include/HEJ/HiggsCouplingSettings.hh b/include/HEJ/HiggsCouplingSettings.hh
index 206598a..9518ee4 100644
--- a/include/HEJ/HiggsCouplingSettings.hh
+++ b/include/HEJ/HiggsCouplingSettings.hh
@@ -1,20 +1,24 @@
/** \file
* \brief Defines the settings for Higgs boson coupling to gluons
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <limits>
namespace HEJ{
//! Settings for Higgs boson coupling to gluons
struct HiggsCouplingSettings{
//! Top quark mass
double mt = std::numeric_limits<double>::infinity();
//! Bottom quark mass
double mb = 4.7;
//! Whether to use impact factors
bool use_impact_factors = true;
//! Whether to include bottom quark effects
bool include_bottom = false;
};
}
diff --git a/include/HEJ/JetSplitter.hh b/include/HEJ/JetSplitter.hh
index b361dde..d8e0b9d 100644
--- a/include/HEJ/JetSplitter.hh
+++ b/include/HEJ/JetSplitter.hh
@@ -1,57 +1,69 @@
/**
* \file
* \brief Declaration of the JetSplitter class
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include "HEJ/utility.hh"
+#include <functional>
+#include <vector>
+
+#include "fastjet/JetDefinition.hh"
+
#include "HEJ/RNG.hh"
+namespace fastjet {
+ class PseudoJet;
+}
+
namespace HEJ {
//! Class to split jets into their constituents
class JetSplitter {
public:
struct SplitResult {
std::vector<fastjet::PseudoJet> constituents;
double weight;
};
//! Constructor
/**
* @param jet_def Jet definition
* @param min_pt Minimum jet transverse momentum
* @param ran Random number generator
*/
JetSplitter(
fastjet::JetDefinition jet_def, double min_pt,
HEJ::RNG & ran
):
R_{jet_def.R()},
min_jet_pt_{min_pt},
jet_def_{jet_def},
ran_{ran}
{}
//! Split a get into constituents
/**
* @param j2split Jet to be split
* @param ncons Number of constituents
* @returns The constituent momenta
* together with the associated weight
*/
SplitResult split(fastjet::PseudoJet const & j2split, int ncons) const;
//! Maximum distance of constituents to jet axis
static constexpr double R_factor = 5./3.;
private:
SplitResult Split2(fastjet::PseudoJet const & j2split) const;
double sample_distance_2p(double & wt) const;
double R_;
double min_jet_pt_;
fastjet::JetDefinition jet_def_;
std::reference_wrapper<HEJ::RNG> ran_;
};
}
diff --git a/include/HEJ/LesHouchesWriter.hh b/include/HEJ/LesHouchesWriter.hh
index b793540..7d23e79 100644
--- a/include/HEJ/LesHouchesWriter.hh
+++ b/include/HEJ/LesHouchesWriter.hh
@@ -1,55 +1,61 @@
/** \file
* \brief Contains the writer for LesHouches output
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <fstream>
-
-#include "HEJ/EventWriter.hh"
+#include <memory>
+#include <string>
#include "LHEF/LHEF.h"
+#include "HEJ/EventWriter.hh"
+
namespace HEJ{
class Event;
//! Class for writing events to a file in the Les Houches Event File format
class LesHouchesWriter : public EventWriter{
public:
//! Constructor
/**
* @param file Name of output file
* @param heprup General process information
*/
LesHouchesWriter(std::string const & file, LHEF::HEPRUP heprup);
LesHouchesWriter(LesHouchesWriter const & other) = delete;
LesHouchesWriter & operator=(LesHouchesWriter const & other) = delete;
/** @TODO in principle, this class should be movable
* but that somehow(?) breaks the write member function
*/
LesHouchesWriter(LesHouchesWriter && other) = delete;
LesHouchesWriter & operator=(LesHouchesWriter && other) = delete;
~LesHouchesWriter() override;
//! Write an event to the file specified in the constructor
void write(Event const & ev) override;
private:
void write_init(){
writer_->init();
}
void rewrite_init();
LHEF::HEPRUP & heprup(){
return writer_->heprup;
}
LHEF::HEPEUP & hepeup(){
return writer_->hepeup;
}
std::fstream out_;
std::unique_ptr<LHEF::Writer> writer_;
};
}
diff --git a/include/HEJ/MatrixElement.hh b/include/HEJ/MatrixElement.hh
index 150d7d5..8368072 100644
--- a/include/HEJ/MatrixElement.hh
+++ b/include/HEJ/MatrixElement.hh
@@ -1,173 +1,192 @@
/** \file
* \brief Contains the MatrixElement Class
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <functional>
+#include <vector>
-#include "HEJ/config.hh"
-#include "HEJ/utility.hh"
-#include "HEJ/HiggsCouplingSettings.hh"
-#include "HEJ/Weights.hh"
+#include "fastjet/PseudoJet.hh"
-#include "CLHEP/Vector/LorentzVector.h"
+#include "HEJ/PDG_codes.hh"
+#include "HEJ/Weights.hh"
+#include "HEJ/config.hh"
+namespace CLHEP {
+ class HepLorentzVector;
+}
namespace HEJ{
class Event;
+ class Particle;
//! Class to calculate the squares of matrix elements
class MatrixElement{
public:
/** \brief MatrixElement Constructor
* @param alpha_s Function taking the renormalisation scale
* and returning the strong coupling constant
* @param conf General matrix element settings
*/
MatrixElement(
std::function<double (double)> alpha_s,
MatrixElementConfig conf
);
/**
* \brief squares of regulated HEJ matrix elements
* @param event The event for which to calculate matrix elements
- * @param check_momenta Special treatment for partons inside extremal jets
* @returns The squares of HEJ matrix elements including virtual corrections
*
- * cf. eq. (22) in \cite Andersen:2011hs
+ * This function returns one value for the central parameter choice
+ * and one additional value for each entry in \ref Event.variations().
+ * See eq. (22) in \cite Andersen:2011hs for the definition of the squared
+ * matrix element.
*
* \internal Relation to standard HEJ Met2: MatrixElement = Met2*shat^2/(pdfta*pdftb)
*/
- Weights operator()(
- Event const & event,
- bool check_momenta
- ) const;
+ Weights operator()(Event const & event) const;
//! Squares of HEJ tree-level matrix elements
/**
* @param event The event for which to calculate matrix elements
- * @param check_momenta Special treatment for partons inside extremal jets
* @returns The squares of HEJ matrix elements without virtual corrections
*
* cf. eq. (22) in \cite Andersen:2011hs
*/
- Weights tree(
- Event const & event,
- bool check_momenta
- ) const;
+ Weights tree(Event const & event) const;
/**
* \brief Virtual corrections to matrix element squares
- * @param event The event for which to calculate matrix elements
+ * @param event The event for which to calculate matrix elements
* @returns The virtual corrections to the squares of the matrix elements
*
* The all order virtual corrections to LL in the MRK limit is
* given by replacing 1/t in the scattering amplitude according to the
* lipatov ansatz.
*
* cf. second-to-last line of eq. (22) in \cite Andersen:2011hs
* note that indices are off by one, i.e. out[0].p corresponds to p_1
*/
- Weights virtual_corrections(
- Event const & event
- ) const;
-
- private:
+ Weights virtual_corrections(Event const & event) const;
+ /**
+ * \brief Scale-dependent part of tree-level matrix element squares
+ * @param event The event for which to calculate matrix elements
+ * @returns The scale-dependent part of the squares of the
+ * tree-level matrix elements
+ *
+ * The tree-level matrix elements factorises into a renormalisation-scale
+ * dependent part, given by the strong coupling to some power, and a
+ * scale-independent remainder. This function only returns the former parts
+ * for the central scale choice and all \ref Event.variations().
+ *
+ * @see tree, tree_kin
+ */
Weights tree_param(
Event const & event
) const;
- double tree_kin(
- Event const & event,
- bool check_momenta
- ) const;
+ /**
+ * \brief Kinematic part of tree-level matrix element squares
+ * @param event The event for which to calculate matrix elements
+ * @returns The kinematic part of the squares of the
+ * tree-level matrix elements
+ *
+ * The tree-level matrix elements factorises into a renormalisation-scale
+ * dependent part, given by the strong coupling to some power, and a
+ * scale-independent remainder. This function only returns the latter part.
+ * Since it does not depend on the parameter variations, only a single value
+ * is returned.
+ *
+ * @see tree, tree_param
+ */
+ double tree_kin(Event const & event) const;
+
+ private:
double tree_param(
Event const & event,
double mur
) const;
double virtual_corrections_W(
Event const & event,
double mur,
Particle const & WBoson
) const;
double virtual_corrections(
Event const & event,
double mur
) const;
//! \internal cf. last line of eq. (22) in \cite Andersen:2011hs
double omega0(
double alpha_s, double mur,
fastjet::PseudoJet const & q_j, double lambda
) const;
double tree_kin_jets(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const;
double tree_kin_W(
Event const & ev,
- bool WPlus,
- bool check_momenta
+ bool WPlus
) const;
double tree_kin_Higgs(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const;
double tree_kin_Higgs_first(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const;
double tree_kin_Higgs_last(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const;
/**
* \internal
* \brief Higgs inbetween extremal partons.
*
* Note that in the case of unordered emission, the Higgs is *always*
* treated as if in between the extremal (FKL) partons, even if its
* rapidity is outside the extremal parton rapidities
*/
double tree_kin_Higgs_between(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const;
double tree_param_partons(
double alpha_s, double mur,
std::vector<Particle> const & partons
) const;
std::vector<int> in_extremal_jet_indices(
std::vector<fastjet::PseudoJet> const & partons
) const;
std::vector<Particle> tag_extremal_jet_partons(
- Event const & ev, bool check_momenta
+ Event const & ev
) const;
double MH2_forwardH(
CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
pid::ParticleID type2,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector pH,
double t1, double t2
) const;
std::function<double (double)> alpha_s_;
MatrixElementConfig param_;
};
}
diff --git a/include/HEJ/Mixmax.hh b/include/HEJ/Mixmax.hh
index 625ed4a..5f9677e 100644
--- a/include/HEJ/Mixmax.hh
+++ b/include/HEJ/Mixmax.hh
@@ -1,31 +1,35 @@
/** \file
* \brief The Mixmax random number generator
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <CLHEP/Random/Randomize.h>
#include <CLHEP/Random/MixMaxRng.h>
#include "HEJ/RNG.hh"
namespace HEJ {
//! MIXMAX random number generator
/**
* For details on MIXMAX, see \cite Savvidy:2014ana
*/
class Mixmax : public DefaultRNG {
public:
Mixmax() = default;
Mixmax(long seed): ran_{seed} {};
//! Generate pseudorandom number between 0 and 1
double flat() override {
return ran_.flat();
};
private:
CLHEP::MixMaxRng ran_;
};
}
diff --git a/include/HEJ/PDF.hh b/include/HEJ/PDF.hh
index 2772770..c5dddbf 100644
--- a/include/HEJ/PDF.hh
+++ b/include/HEJ/PDF.hh
@@ -1,73 +1,77 @@
/** \file
*
* \brief Contains all the necessary classes and functions for interaction with PDFs.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <array>
+#include <memory>
#include "LHAPDF/LHAPDF.h"
-#include "HEJ/utility.hh"
+
#include "HEJ/PDG_codes.hh"
namespace HEJ{
-
//! Class for interaction with a PDF set
class PDF {
public:
/**
* \brief PDF Constructor
* @param id Particle ID according to PDG
* @param beam1 Particle ID of particle in beam 1
* @param beam2 Particle ID of particle in beam 2
*/
PDF(int id, ParticleID beam1, ParticleID beam2);
/**
* \brief Calculate the pdf value x*f(x, q)
* @param beam_idx Beam number (0 or 1)
* @param x Momentum fraction
* @param q Energy scale
* @param id PDG particle id
* @returns x*f(x, q)
*
* Returns 0 if x or q are outside the range covered by the PDF set
*/
double pdfpt(size_t beam_idx, double x, double q, ParticleID id) const;
/**
* \brief Value of the strong coupling \f$\alpha_s(q)\f$ at the given scale
* @param q Renormalisation scale
* @returns Value of the strong coupling constant
*/
double Halphas(double q) const;
//! Check if the energy scale is within the range covered by the PDF set
/**
* @param q Energy Scale
* @returns true if q is within the covered range, false otherwise
*/
bool inRangeQ(double q) const;
//! Check if the momentum fraction is within the range covered by the PDF set
/**
* @param x Momentum Fraction
* @returns true if x is within the covered range, false otherwise
*/
bool inRangeX(double x) const;
#if defined LHAPDF_MAJOR_VERSION && LHAPDF_MAJOR_VERSION == 6
//! PDF id of the current set
int id() const;
#endif
private:
#if defined LHAPDF_MAJOR_VERSION && LHAPDF_MAJOR_VERSION == 6
std::unique_ptr<LHAPDF::PDF> pdf;
#endif
std::array<int, 2> beamtype;
};
}
diff --git a/include/HEJ/PDG_codes.hh b/include/HEJ/PDG_codes.hh
index f055c74..17c44a9 100644
--- a/include/HEJ/PDG_codes.hh
+++ b/include/HEJ/PDG_codes.hh
@@ -1,139 +1,143 @@
/** \file PDG_codes.hh
* \brief Contains the Particle IDs of all relevant SM particles.
*
* Large enumeration included which has multiple entries for potential
* alternative names of different particles. There are also functions
* which can be used to determine if a particle is a parton or if
* it is a non-gluon boson.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <string>
namespace HEJ {
//! particle ids according to PDG
namespace pid {
//! The possible particle identities. We use PDG IDs as standard.
enum ParticleID{
d = 1, /*!< Down Quark */
down = d, /*!< Down Quark */
u = 2, /*!< Up Quark */
up = u, /*!< Up Quark */
s = 3, /*!< Strange Quark */
strange = s, /*!< Strange Quark */
c = 4, /*!< Charm Quark */
charm = c, /*!< Charm Quark */
b = 5, /*!< Bottom Quark */
bottom = b, /*!< Bottom Quark */
t = 6, /*!< Top Quark */
top = t, /*!< Top Quark */
e = 11, /*!< Electron */
electron = e, /*!< Electron */
nu_e = 12, /*!< Electron Neutrino */
electron_neutrino = nu_e, /*!< Electron neutrino */
mu = 13, /*!< Muon */
muon = mu, /*!< Muon */
nu_mu = 14, /*!< Muon Neutrino */
muon_neutrino = nu_mu, /*!< Muon Neutrino */
tau = 15, /*!< Tau */
nu_tau = 16, /*!< Tau Neutrino */
tau_neutrino = nu_tau, /*!< Tau Neutrino */
d_bar = -d, /*!< Anti-Down Quark */
u_bar = -u, /*!< Anti-Up quark */
s_bar = -s, /*!< Anti-Strange Quark */
c_bar = -c, /*!< Anti-Charm Quark */
b_bar = -b, /*!< Anti-Bottom Quark */
t_bar = -t, /*!< Anti-Top Quark */
e_bar = -e, /*!< Positron */
positron = e_bar, /*!< Positron */
nu_e_bar = -nu_e, /*!< Anti-Electron Neutrino */
mu_bar = -mu, /*!< Anti-Muon */
nu_mu_bar = -nu_mu, /*!< Anti-Muon Neutrino */
tau_bar = -tau, /*!< Anti-Tau */
nu_tau_bar = -nu_tau, /*!< Anti-Tau Neutrino */
gluon = 21, /*!< Gluon */
g = gluon, /*!< Gluon */
photon = 22, /*!< Photon */
gamma = photon, /*!< Photon */
Z = 23, /*!< Z Boson */
Wp = 24, /*!< W- Boson */
Wm = -Wp, /*!< W+ Boson */
h = 25, /*!< Higgs Boson */
Higgs = h, /*!< Higgs Boson */
higgs = h, /*!< Higgs Boson */
p = 2212, /*!< Proton */
proton = p, /*!< Proton */
p_bar = -p, /*!< Anti-Proton */
};
}
using ParticleID = pid::ParticleID;
//! Convert a particle name to the corresponding PDG particle ID
ParticleID to_ParticleID(std::string const & name);
/**
* \brief Function to determine if particle is a parton
* @param p PDG ID of particle
* @returns true if the particle is a parton, false otherwise
*/
inline
constexpr bool is_parton(ParticleID p){
return p == pid::gluon || std::abs(p) <= pid::top;
}
/**
* \brief function to determine if the particle is a photon, W, Z, or Higgs boson
* @param id PDG ID of particle
* @returns true if the partice is a A,W,Z, or H, false otherwise
*/
inline
constexpr bool is_AWZH_boson(ParticleID id){
return id == pid::Wm || (id >= pid::photon && id <= pid::Higgs);
}
/**
* \brief Function to determine if particle is a quark
* @param id PDG ID of particle
* @returns true if the particle is a qaurk, false otherwise
*/
inline
constexpr bool is_quark(ParticleID id){
return (id >= pid::down && id <= pid::top);
}
/**
* \brief Function to determine if particle is a antiquark
* @param id PDG ID of particle
* @returns true if the particle is an antiquark, false otherwise
*/
inline
constexpr bool is_antiquark(ParticleID id){
return (id <= pid::d_bar && id >= pid::t_bar);
}
/**
* \brief Function to determine if particle is a any-quark
* @param id PDG ID of particle
* @returns true if the particle is a quark or antiquark, false otherwise
*/
inline
constexpr bool is_anyquark(ParticleID id){
return (id && id >= pid::t_bar && id <= pid::t);
}
/**
* \brief function to determine if the particle is a photon, W or Z
* @param id PDG ID of particle
* @returns true if the partice is a A,W,Z, or H, false otherwise
*/
inline
constexpr bool is_AWZ_boson(ParticleID id){
return id == pid::Wm || (id >= pid::photon && id <= pid::Wp);
}
}
diff --git a/include/HEJ/utility.hh b/include/HEJ/Particle.hh
similarity index 53%
copy from include/HEJ/utility.hh
copy to include/HEJ/Particle.hh
index 96a1961..cde958e 100644
--- a/include/HEJ/utility.hh
+++ b/include/HEJ/Particle.hh
@@ -1,238 +1,141 @@
/**
- * \file
- * \brief Contains various utilities
+ * \file Particle.hh
+ * \brief Contains the particle struct
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <algorithm>
-#include <cassert>
-
-#include <boost/core/demangle.hpp>
-
-// FastJet Includes
#include "fastjet/PseudoJet.hh"
-#include "fastjet/ClusterSequence.hh"
#include "HEJ/PDG_codes.hh"
-namespace HEJ{
+namespace HEJ {
+
//! Class representing a particle
struct Particle {
//! particle type
ParticleID type;
//! particle momentum
fastjet::PseudoJet p;
//! get rapidity
double rapidity() const{
return p.rapidity();
}
//! get transverse momentum
double perp() const{
return p.perp();
}
//! get momentum in x direction
double px() const{
return p.px();
}
//! get momentum in y direction
double py() const{
return p.py();
}
//! get momentum in z direction
double pz() const{
return p.pz();
}
//! get energy
double E() const{
return p.E();
}
//! get mass
double m() const{
return p.m();
}
};
//! Functor to compare rapidities
/**
* This can be used whenever a rapidity comparison function is needed,
* for example in many standard library functions.
*
* @see pz_less
*/
struct rapidity_less{
template<class FourVector>
bool operator()(FourVector const & p1, FourVector const & p2){
return p1.rapidity() < p2.rapidity();
}
};
//! Functor to compare momenta in z direction
/**
* This can be used whenever a pz comparison function is needed,
* for example in many standard library functions.
*
* @see rapidity_less
*/
struct pz_less{
template<class FourVector>
bool operator()(FourVector const & p1, FourVector const & p2){
return p1.pz() < p2.pz();
}
};
//! Convert a vector of Particles to a vector of particle momenta
inline
std::vector<fastjet::PseudoJet> to_PseudoJet(
std::vector<Particle> const & v
){
std::vector<fastjet::PseudoJet> result;
for(auto && sp: v) result.emplace_back(sp.p);
return result;
}
//! Check if a particle is a parton, i.e. quark, antiquark, or gluon
inline
bool is_parton(Particle const & p){
return is_parton(p.type);
}
//! Check if a particle is a quark
inline
bool is_quark(Particle const & p){
return is_quark(p.type);
}
//! Check if a particle is an anti-quark
inline
bool is_antiquark(Particle const & p){
return is_antiquark(p.type);
}
//! Check if a particle is a quark or any-quark
inline
bool is_anyquark(Particle const & p){
return is_anyquark(p.type);
}
//! Check if a particle is a photon, W or Z boson
inline bool is_AWZ_boson(Particle const & particle){
return is_AWZ_boson(particle.type);
}
//! Check if a particle is a photon, W, Z, or Higgs boson
inline bool is_AWZH_boson(Particle const & particle){
return is_AWZH_boson(particle.type);
}
//! Extract all partons from a vector of particles
inline
std::vector<Particle> filter_partons(
std::vector<Particle> const & v
){
std::vector<Particle> result;
result.reserve(v.size());
std::copy_if(
begin(v), end(v), std::back_inserter(result),
[](Particle const & p){ return is_parton(p); }
);
return result;
}
-
- //! Create a std::unique_ptr to a T object
- /**
- * For non-array types this works like std::make_unique,
- * which is not available under C++11
- */
- template<class T, class... Args>
- std::unique_ptr<T> make_unique(Args&&... a){
- return std::unique_ptr<T>{new T{std::forward<Args>(a)...}};
- }
-
- //! Create an array containing the passed arguments
- template<typename T, typename... U>
- constexpr
- std::array<T, 1 + sizeof...(U)> make_array(T t, U&&... rest){
- return {{t, std::forward<U>(rest)...}};
- }
-
-
- inline
- std::string join(
- std::string const & /* delim */
- ){
- return "";
- }
-
- inline
- std::string join(
- std::string const & /* delim */, std::string const & str
- ){
- return str;
- }
-
- //! Join strings with a delimiter
- /**
- * @param delim Delimiter to be put between consecutive strings
- * @param first First string
- * @param second Second string
- * @param rest Remaining strings
- */
- template<typename... Strings>
- std::string join(
- std::string const & delim,
- std::string const & first, std::string const & second,
- Strings&&... rest
- ){
- return join(delim, first + delim + second, std::forward<Strings>(rest)...);
- }
-
- //! Return the name of the argument's type
- template<typename T>
- std::string type_string(T&&){
- return boost::core::demangle(typeid(T).name());
- }
-
- //! Eliminate compiler warnings for unused variables
- template<typename... T>
- constexpr void ignore(T&&...) {}
-
- //! Check whether two doubles are closer than ep > 0 to each other
- inline
- bool nearby_ep(double a, double b, double ep){
- assert(ep > 0);
- return std::abs(a-b) < ep;
- }
-
- //! Check whether all components of two PseudoJets are closer than ep to each other
- inline
- bool nearby_ep(
- fastjet::PseudoJet const & pa, fastjet::PseudoJet const & pb,
- double ep
- ){
- assert(ep > 0);
- for(size_t i = 0; i < 4; ++i){
- if(!nearby_ep(pa[i], pb[i], ep)) return false;
- }
- return true;
- }
-
- inline
- bool nearby(
- fastjet::PseudoJet const & pa, fastjet::PseudoJet const & pb, double const norm = 1.
- ){
- return nearby_ep(pa, pb, 1e-7*norm);
- }
-
- //! Check whether two rapidities are close
- inline
- bool nearby_rap(
- double rapa, double rapb, double rap
- ){
- assert(rap > 0);
- if(!nearby_ep(rapa, rapb, rap)) return false;
- return true;
- }
}
diff --git a/include/HEJ/PhaseSpacePoint.hh b/include/HEJ/PhaseSpacePoint.hh
index 2ced4da..6bfce05 100644
--- a/include/HEJ/PhaseSpacePoint.hh
+++ b/include/HEJ/PhaseSpacePoint.hh
@@ -1,149 +1,155 @@
/** \file
* \brief Contains the PhaseSpacePoint Class
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
+#include <array>
+#include <functional>
+#include <unordered_map>
#include <vector>
-#include "HEJ/utility.hh"
#include "HEJ/config.hh"
-#include "HEJ/Event.hh"
-#include "HEJ/JetSplitter.hh"
+#include "HEJ/Particle.hh"
#include "HEJ/RNG.hh"
namespace HEJ{
+ class Event;
//! A point in resummation phase space
class PhaseSpacePoint{
public:
//! Default PhaseSpacePoint Constructor
PhaseSpacePoint() = default;
//! PhaseSpacePoint Constructor
/**
* @param ev Clustered Jet Event
* @param conf Configuration parameters
* @param ran Random number generator
*/
PhaseSpacePoint(
Event const & ev,
PhaseSpacePointConfig conf,
HEJ::RNG & ran
);
//! Get phase space point weight
double weight() const{
return weight_;
}
//! Access incoming particles
std::array<Particle, 2> const & incoming() const{
return incoming_;
}
//! Access outgoing particles
std::vector<Particle> const & outgoing() const{
return outgoing_;
}
//! Particle decays
/**
* The key in the returned map corresponds to the index in the
* vector returned by outgoing()
*/
std::unordered_map<size_t, std::vector<Particle>> const & decays() const{
return decays_;
}
static constexpr int ng_max = 1000; //< maximum number of extra gluons
private:
std::vector<fastjet::PseudoJet> cluster_jets(
std::vector<fastjet::PseudoJet> const & partons
) const;
bool pass_resummation_cuts(
std::vector<fastjet::PseudoJet> const & jets
) const;
bool pass_extremal_cuts(
fastjet::PseudoJet const & ext_parton,
fastjet::PseudoJet const & jet
) const;
int sample_ng(std::vector<fastjet::PseudoJet> const & Born_jets);
int sample_ng_jets(int ng, std::vector<fastjet::PseudoJet> const & Born_jets);
double probability_in_jet(
std::vector<fastjet::PseudoJet> const & Born_jets
) const;
std::vector<fastjet::PseudoJet> gen_non_jet(
int ng_non_jet,
double ptmin, double ptmax
);
void rescale_rapidities(
std::vector<fastjet::PseudoJet> & partons,
double ymin, double ymax
);
std::vector<fastjet::PseudoJet> reshuffle(
std::vector<fastjet::PseudoJet> const & Born_jets,
fastjet::PseudoJet const & q
);
bool jets_ok(
std::vector<fastjet::PseudoJet> const & Born_jets,
std::vector<fastjet::PseudoJet> const & partons
) const;
void reconstruct_incoming(std::array<Particle, 2> const & Born_incoming);
double phase_space_normalisation(
int num_Born_jets,
int num_res_partons
) const;
std::vector<fastjet::PseudoJet> split(
std::vector<fastjet::PseudoJet> const & jets, int ng_jets
);
std::vector<int> distribute_jet_partons(
int ng_jets, std::vector<fastjet::PseudoJet> const & jets
);
std::vector<fastjet::PseudoJet> split(
std::vector<fastjet::PseudoJet> const & jets,
std::vector<int> const & np_in_jet
);
bool split_preserved_jets(
std::vector<fastjet::PseudoJet> const & jets,
std::vector<fastjet::PseudoJet> const & jet_partons
) const;
template<class Particle>
Particle const & most_backward_FKL(
std::vector<Particle> const & partons
) const;
template<class Particle>
Particle const & most_forward_FKL(
std::vector<Particle> const & partons
) const;
template<class Particle>
Particle & most_backward_FKL(std::vector<Particle> & partons) const;
template<class Particle>
Particle & most_forward_FKL(std::vector<Particle> & partons) const;
bool extremal_ok(
std::vector<fastjet::PseudoJet> const & partons
) const;
void label_qqx(Event const & event);
void copy_AWZH_boson_from(Event const & event);
bool momentum_conserved() const;
bool unob_, unof_, qqxb_, qqxf_, qqxmid_;
double weight_;
PhaseSpacePointConfig param_;
std::array<Particle, 2> incoming_;
std::vector<Particle> outgoing_;
//! \internal Particle decays in the format {outgoing index, decay products}
std::unordered_map<size_t, std::vector<Particle>> decays_;
std::reference_wrapper<HEJ::RNG> ran_;
};
}
diff --git a/include/HEJ/ProgressBar.hh b/include/HEJ/ProgressBar.hh
index 402c91f..5f7f32d 100644
--- a/include/HEJ/ProgressBar.hh
+++ b/include/HEJ/ProgressBar.hh
@@ -1,89 +1,93 @@
/** \file
* \brief Contains the ProgressBar class
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <ostream>
#include <functional>
#include <stdexcept>
namespace HEJ {
//! Class representing (and printing) a progress bar
template<typename T>
class ProgressBar {
public:
//! Constructor
/**
* @param out Output stream
* @param max Maximum value of the progress parameter
*
* This will print a fixed-width progress bar, which is initially at 0%.
*/
ProgressBar(std::ostream & out, T max) :
out_{out}, max_{max}
{
if(max <= 0) {
throw std::invalid_argument{
"Maximum in progress bar has to be positive"
};
}
print_bar();
}
//! Increment progress
/**
* @param count Value to add to the current progress parameter
*
* After updating the progess parameter, the progress bar is updated
* to a percentage that corresponds to the ratio of the current and
* maximum progress parameters.
*/
ProgressBar & increment(T count) {
counter_ += count;
update_progress();
return *this;
}
//! Increase progress by one unit
/**
* After updating the progess parameter, the progress bar is updated
* to a percentage that corresponds to the ratio of the current and
* maximum progress parameters.
*/
ProgressBar & operator++() {
++counter_;
update_progress();
return *this;
}
private:
void update_progress() {
counter_ = std::min(counter_, max_);
const int ndots = (100*counter_)/max_;
const int new_dots = ndots - ndots_;
if(new_dots > 0) {
for(int dot = 0; dot < new_dots; ++dot) out_.get() << '.';
out_.get().flush();
ndots_ = ndots;
}
}
void print_bar() const {
out_.get() << "0% ";
for(int i = 10; i <= 100; i+= 10){
out_.get() << " " + std::to_string(i) + "%";
}
out_.get() << "\n|";
for(int i = 10; i <= 100; i+= 10){
out_.get() << "---------|";
}
out_.get() << '\n';
}
std::reference_wrapper<std::ostream> out_;
T counter_ = 0;
T ndots_ = 0;
T max_;
};
}
diff --git a/include/HEJ/RNG.hh b/include/HEJ/RNG.hh
index f479d8a..9cd36f6 100644
--- a/include/HEJ/RNG.hh
+++ b/include/HEJ/RNG.hh
@@ -1,41 +1,45 @@
/** \file
* \brief Interface for pseudorandom number generators
*
* We select our random number generator at runtime according to the
* configuration file. This interface guarantees that we can use all
* generators in the same way.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <limits>
namespace HEJ {
//! Interface for random number generator
struct RNG {
//! Generate random number in (0,1]
virtual double flat() = 0;
//! Minimum number that can be generated
virtual unsigned min() const = 0;
//! Maximum number that can be generated
virtual unsigned max() const = 0;
//! Generate random number in [min(), max()]
virtual unsigned operator()() = 0;
virtual ~RNG() = default;
};
//! Helper struct with default implementations
struct DefaultRNG : virtual RNG {
unsigned min() const override {
return 0u;
}
unsigned max() const override {
return std::numeric_limits<unsigned>::max() - 1;
}
unsigned operator()() override {
return flat()*std::numeric_limits<unsigned int>::max();
}
};
}
diff --git a/include/HEJ/Ranlux64.hh b/include/HEJ/Ranlux64.hh
index fc0e8fb..c11c3c7 100644
--- a/include/HEJ/Ranlux64.hh
+++ b/include/HEJ/Ranlux64.hh
@@ -1,29 +1,34 @@
/** \file
* \brief Contains a class for the ranlux64 random number generator
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <CLHEP/Random/Randomize.h>
-#include <CLHEP/Random/RanluxEngine.h>
+#include <string>
+
+#include <CLHEP/Random/Ranlux64Engine.h>
#include "HEJ/RNG.hh"
namespace HEJ {
//! Ranlux64 random number generator
/**
* For details on ranlux64, see \cite Luscher:1993dy, \cite James:1993np
*/
class Ranlux64 : public DefaultRNG {
public:
Ranlux64();
Ranlux64(std::string const & seed_file);
//! Generate pseudorandom number between 0 and 1
double flat() override;
private:
CLHEP::Ranlux64Engine ran_;
};
}
diff --git a/include/HEJ/RivetAnalysis.hh b/include/HEJ/RivetAnalysis.hh
index 8ccad0c..e36b88d 100644
--- a/include/HEJ/RivetAnalysis.hh
+++ b/include/HEJ/RivetAnalysis.hh
@@ -1,69 +1,69 @@
/** \file
* \brief HEJ 2 interface to rivet analyses
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <memory>
#include <string>
#include <vector>
#include "HEJ/Analysis.hh"
#include "HEJ/HepMCInterface.hh"
-namespace HEJ {
- class Event;
-}
-
namespace Rivet {
class AnalysisHandler;
}
namespace YAML {
class Node;
}
namespace HEJ {
/**
* @brief Class representing a Rivet analysis
*
* This class inherits from Analysis and can therefore be used
* like any other HEJ 2 analysis.
*/
class RivetAnalysis: public HEJ::Analysis {
public:
static std::unique_ptr<Analysis> create(YAML::Node const & config);
//! Constructor
/**
* @param config Configuration parameters
*
* config["analysis"] should be the name of a single Rivet analysis or
* a list of Rivet analyses. config["output"] is the prefix for
* the .yoda output files.
*/
RivetAnalysis(YAML::Node const & config);
//! Pass an event to the underlying Rivet analysis
void fill(HEJ::Event const & event, HEJ::Event const &) override;
bool pass_cuts(HEJ::Event const &, HEJ::Event const &) override
{return true;} //< no additional cuts are applied
void finalise() override;
private:
std::vector<std::string> analyses_names_;
const std::string output_name_;
/// struct to organise the infos per rivet run/scale setting
struct rivet_info {
std::unique_ptr<Rivet::AnalysisHandler> handler;
std::string name;
HEJ::HepMCInterface hepmc;
};
std::vector<rivet_info> rivet_runs_;
/**
* \internal
* @brief Calculates the scale variation from the first event for the output file
*/
void init(HEJ::Event const & event);
bool first_event_;
};
}
diff --git a/include/HEJ/ScaleFunction.hh b/include/HEJ/ScaleFunction.hh
index c2cc22f..42c2c99 100644
--- a/include/HEJ/ScaleFunction.hh
+++ b/include/HEJ/ScaleFunction.hh
@@ -1,155 +1,174 @@
/** \file
* \brief Functions to calculate the (renormalisation and factorisation) scales for an event
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <functional>
-#include <vector>
-#include <string>
#include <memory>
+#include <string>
+#include <utility>
+#include <vector>
namespace HEJ{
class Event;
//! Class to calculate the scale associated with an event
class ScaleFunction {
public:
//! Constructor
/**
* @param name Name of the scale choice (e.g. H_T)
* @param fun Function used to calculate the scale
*/
ScaleFunction(std::string name, std::function<double(Event const &)> fun):
name_{std::move(name)},
fun_{std::move(fun)}
{}
//! Name of the scale choice
std::string const & name() const {
return name_;
}
//! Calculate the scale associated with an event
double operator()(Event const & ev) const {
return fun_(ev);
}
private:
friend ScaleFunction operator*(double factor, ScaleFunction base_scale);
friend ScaleFunction operator/(ScaleFunction base_scale, double denom);
+ friend ScaleFunction operator*(ScaleFunction func1, ScaleFunction func2);
+ friend ScaleFunction operator/(ScaleFunction func1, ScaleFunction func2);
std::string name_;
std::function<double(Event const &)> fun_;
};
//! Multiply a scale choice by a constant factor
/**
* For example, multiplying 0.5 and a scale function for H_T
* will result in a scale function for H_T/2.
*/
ScaleFunction operator*(double factor, ScaleFunction base_scale);
+ //! Multiply a scale choice by a second one
+ /**
+ * For example, multiplying H_T and m_j1j2
+ * will result in a scale function for H_T*m_j1j2.
+ */
+ ScaleFunction operator*(ScaleFunction factor, ScaleFunction base_scale);
//! Divide a scale choice by a constant factor
/**
* For example, dividing a scale function for H_T by 2
* will result in a scale function for H_T/2.
*/
ScaleFunction operator/(ScaleFunction base_scale, double denom);
+ //! Divide a scale choice by a second one
+ /**
+ * For example, dividing a scale function for H_T by m_j1j2
+ * will result in a scale function for H_T/m_j1j2.
+ */
+ ScaleFunction operator/(ScaleFunction base_scale, ScaleFunction denom);
//! Calculate \f$H_T\f$ for the input event
/**
* \f$H_T\f$ is the sum of the (scalar) transverse momenta of all
* final-state particles
*/
double H_T(Event const &);
//! The maximum of all (scalar) jet transverse momentum
double max_jet_pt(Event const &);
//! The invariant mass of the sum of all jet momenta
double jet_invariant_mass(Event const &);
//! Invariant mass of the two hardest jets
double m_j1j2(Event const &);
//! Functor that returns a fixed scale regardless of the input event
class FixedScale {
public:
explicit FixedScale(double mu): mu_{mu} {}
double operator()(Event const &) const {
return mu_;
}
private:
double mu_;
};
class ParameterDescription;
//! Generate combinations of renormalisation and factorisation scales
class ScaleGenerator{
public:
ScaleGenerator() = default;
/** \brief Constructor
* @param scale_functions_begin Iterator to first base scale
* @param scale_functions_end Iterator past last base scale
* @param scale_factors_begin Iterator to first scale factor
* @param scale_factors_end Iterator past last scale factor
* @param max_scale_ratio Maximum ratio between renormalisation
* and factorisation scale
*/
template<class ScaleFunIterator, class FactorIterator>
ScaleGenerator(
ScaleFunIterator scale_functions_begin,
ScaleFunIterator scale_functions_end,
FactorIterator scale_factors_begin,
FactorIterator scale_factors_end,
double max_scale_ratio
):
scales_(scale_functions_begin, scale_functions_end),
scale_factors_(scale_factors_begin, scale_factors_end),
max_scale_ratio_{max_scale_ratio}
{
gen_descriptions();
}
/** \brief Constructor
* @param scales Base scales
* @param scale_factors Factors to multiply the base scales
* @param max_scale_ratio Maximum ratio between renormalisation
* and factorisation scale
*/
ScaleGenerator(
std::vector<ScaleFunction> scales,
std::vector<double> scale_factors,
double max_scale_ratio
):
scales_(std::move(scales)),
scale_factors_(std::move(scale_factors)),
max_scale_ratio_{max_scale_ratio}
{
gen_descriptions();
}
/** \brief Adjust event parameters, adding scale variation
*
* The central renormalisation and factorisation scale of the returned
* event is given be the first base scale passed to the constructor.
* The scale variation (stored in event.variation()) is constructed as
* follows: For each base scale according to the arguments of the
* constructor we add one variation where both renormalisation and
* factorisation scale are set according to the current base scale.
* Then, all combinations where the base renormalisation and factorisation
* scales are multiplied by one of the scale factors are added.
* The case were both scales are multiplied by one is skipped.
* Scale combinations where the ratio is larger than the maximum scale ratio
* set in the constructor are likewise discarded.
*/
Event operator()(Event event) const;
private:
void gen_descriptions();
std::vector<ScaleFunction> scales_;
std::vector<double> scale_factors_;
std::vector<std::shared_ptr<ParameterDescription>> descriptions_;
double max_scale_ratio_;
};
}
diff --git a/include/HEJ/Weights.hh b/include/HEJ/Weights.hh
index fc92237..fd34e92 100644
--- a/include/HEJ/Weights.hh
+++ b/include/HEJ/Weights.hh
@@ -1,45 +1,49 @@
/** \file
* \brief Container for event weights
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <vector>
namespace HEJ{
//! Collection of weights assigned to a single event
/**
* A number of member functions of the MatrixElement class return Weights
* objects containing the squares of the matrix elements for the various
* scale choices.
*/
struct Weights {
double central;
std::vector<double> variations;
Weights& operator*=(Weights const & other);
Weights& operator*=(double factor);
Weights& operator/=(Weights const & other);
Weights& operator/=(double factor);
};
inline
Weights operator*(Weights a, Weights const & b) {
return a*=b;
}
inline
Weights operator*(Weights a, double b) {
return a*=b;
}
inline
Weights operator*(double b, Weights a) {
return a*=b;
}
inline
Weights operator/(Weights a, Weights const & b) {
return a/=b;
}
inline
Weights operator/(Weights a, double b) {
return a/=b;
}
}
diff --git a/include/HEJ/YAMLreader.hh b/include/HEJ/YAMLreader.hh
index 03a5597..fd9b36a 100644
--- a/include/HEJ/YAMLreader.hh
+++ b/include/HEJ/YAMLreader.hh
@@ -1,241 +1,254 @@
/** \file
* \brief The file which handles the configuration file parameters
*
* The configuration files parameters are read and then stored
* within this objects.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
+#include <string>
+#include <utility>
+#include <vector>
+
#include "yaml-cpp/yaml.h"
+#include "fastjet/JetDefinition.hh"
+
#include "HEJ/config.hh"
#include "HEJ/exceptions.hh"
+#include "HEJ/optional.hh"
+#include "HEJ/PDG_codes.hh"
#include "HEJ/utility.hh"
namespace HEJ{
+ class OutputFile;
//! Load configuration from file
/**
* @param config_file Name of the YAML configuration file
* @returns The HEJ 2 configuration
*/
Config load_config(std::string const & config_file);
//! Set option using the corresponding YAML entry
/**
* @param setting Option variable to be set
* @param yaml Root of the YAML configuration
* @param names Name of the entry
*
* If the entry does not exist or has the wrong type or format
* an exception is thrown.
*
* For example
* @code
* set_from_yaml(foobar, yaml, "foo", "bar")
* @endcode
* is equivalent to
* @code
* foobar = yaml["foo"]["bar"].as<decltype(foobar)>()
* @endcode
* with improved diagnostics on errors.
*
* @see set_from_yaml_if_defined
*/
template<typename T, typename... YamlNames>
void set_from_yaml(
T & setting,
YAML::Node const & yaml, YamlNames const & ... names
);
//! Set option using the corresponding YAML entry, if present
/**
* @param setting Option variable to be set
* @param yaml Root of the YAML configuration
* @param names Name of the entry
*
* This function works similar to set_from_yaml, but does not
* throw any exception if the requested YAML entry does not exist.
*
* @see set_from_yaml
*/
template<typename T, typename... YamlNames>
void set_from_yaml_if_defined(
T & setting,
YAML::Node const & yaml, YamlNames const & ... names
);
//! Extract jet parameters from YAML configuration
JetParameters get_jet_parameters(
YAML::Node const & node, std::string const & entry
);
//! Extract Higgs coupling settings from YAML configuration
HiggsCouplingSettings get_Higgs_coupling(
YAML::Node const & node, std::string const & entry
);
//! Extract scale setting parameters from YAML configuration
ScaleConfig to_ScaleConfig(YAML::Node const & yaml);
//! Extract random number generator settings from YAML configuration
RNGConfig to_RNGConfig(YAML::Node const & node, std::string const & entry);
//! Check whether all options in configuration are supported
/**
* @param conf Configuration to be checked
* @param supported Tree of supported options
*
* If conf contains an entry that does not appear in supported
* an unknown_option exception is thrown. Sub-entries of "analysis"
* (if present) are not checked.
*
* @see unknown_option
*/
void assert_all_options_known(
YAML::Node const & conf, YAML::Node const & supported
);
namespace detail{
void set_from_yaml(fastjet::JetAlgorithm & setting, YAML::Node const & yaml);
void set_from_yaml(EventTreatment & setting, YAML::Node const & yaml);
void set_from_yaml(ParticleID & setting, YAML::Node const & yaml);
void set_from_yaml(OutputFile & setting, YAML::Node const & yaml);
inline
void set_from_yaml(YAML::Node & setting, YAML::Node const & yaml){
setting = yaml;
}
template<typename Scalar>
void set_from_yaml(Scalar & setting, YAML::Node const & yaml){
assert(yaml);
if(!yaml.IsScalar()){
throw invalid_type{"value is not a scalar"};
}
try{
setting = yaml.as<Scalar>();
}
catch(...){
throw invalid_type{
"value " + yaml.as<std::string>()
+ " cannot be converted to a " + type_string(setting)
};
}
}
template<typename T>
void set_from_yaml(optional<T> & setting, YAML::Node const & yaml){
T tmp;
set_from_yaml(tmp, yaml);
setting = tmp;
}
template<typename T>
void set_from_yaml(std::vector<T> & setting, YAML::Node const & yaml){
assert(yaml);
// special case: treat a single value like a vector with one element
if(yaml.IsScalar()){
setting.resize(1);
return set_from_yaml(setting.front(), yaml);
}
if(yaml.IsSequence()){
setting.resize(yaml.size());
for(size_t i = 0; i < setting.size(); ++i){
set_from_yaml(setting[i], yaml[i]);
}
return;
}
throw invalid_type{""};
}
template<typename T, typename FirstName, typename... YamlNames>
void set_from_yaml(
T & setting,
YAML::Node const & yaml, FirstName const & name,
YamlNames && ... names
){
if(!yaml[name]) throw missing_option{""};
set_from_yaml(
setting,
yaml[name], std::forward<YamlNames>(names)...
);
}
template<typename T>
void set_from_yaml_if_defined(T & setting, YAML::Node const & yaml){
return set_from_yaml(setting, yaml);
}
template<typename T, typename FirstName, typename... YamlNames>
void set_from_yaml_if_defined(
T & setting,
YAML::Node const & yaml, FirstName const & name,
YamlNames && ... names
){
if(!yaml[name]) return;
set_from_yaml_if_defined(
setting,
yaml[name], std::forward<YamlNames>(names)...
);
}
}
template<typename T, typename... YamlNames>
void set_from_yaml(
T & setting,
YAML::Node const & yaml, YamlNames const & ... names
){
try{
detail::set_from_yaml(setting, yaml, names...);
}
catch(invalid_type const & ex){
throw invalid_type{
"In option " + join(": ", names...) + ": " + ex.what()
};
}
catch(missing_option const &){
throw missing_option{
"No entry for mandatory option " + join(": ", names...)
};
}
catch(std::invalid_argument const & ex){
throw missing_option{
"In option " + join(": ", names...) + ":"
" invalid value " + ex.what()
};
}
}
template<typename T, typename... YamlNames>
void set_from_yaml_if_defined(
T & setting,
YAML::Node const & yaml, YamlNames const & ... names
){
try{
detail::set_from_yaml_if_defined(setting, yaml, names...);
}
catch(invalid_type const & ex){
throw invalid_type{
"In option " + join(": ", names...) + ": " + ex.what()
};
}
catch(std::invalid_argument const & ex){
throw missing_option{
"In option " + join(": ", names...) + ":"
" invalid value " + ex.what()
};
}
}
}
namespace YAML {
template<>
struct convert<HEJ::OutputFile> {
static Node encode(HEJ::OutputFile const & outfile);
static bool decode(Node const & node, HEJ::OutputFile & out);
};
}
diff --git a/include/HEJ/config.hh b/include/HEJ/config.hh
index 7c51c05..2b9d9f6 100644
--- a/include/HEJ/config.hh
+++ b/include/HEJ/config.hh
@@ -1,173 +1,175 @@
/** \file
* \brief HEJ 2 configuration parameters
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <string>
-#include <memory>
#include "fastjet/JetDefinition.hh"
#include "yaml-cpp/yaml.h"
#include "HEJ/event_types.hh"
-#include "HEJ/Event.hh"
#include "HEJ/HiggsCouplingSettings.hh"
#include "HEJ/optional.hh"
#include "HEJ/output_formats.hh"
#include "HEJ/ScaleFunction.hh"
-#include "HEJ/utility.hh"
-
namespace HEJ{
//! Jet parameters
struct JetParameters{
fastjet::JetDefinition def; /**< Jet Definition */
double min_pt; /**< Minimum Jet Transverse Momentum */
};
//! Settings for scale variation
struct ScaleConfig{
//! Base scale choices
std::vector<ScaleFunction> base;
//! Factors for multiplicative scale variation
std::vector<double> factors;
//! Maximum ratio between renormalisation and factorisation scale
double max_ratio;
};
//! Settings for random number generator
struct RNGConfig {
//! Random number generator name
std::string name;
//! Optional initial seed
optional<std::string> seed;
};
/**! Possible treatments for fixed-order input events.
*
* The program will decide on how to treat an event based on
* the value of this enumeration.
*/
enum class EventTreatment{
reweight, /**< Perform resummation */
keep, /**< Keep the event */
discard, /**< Discard the event */
};
//! Container to store the treatments for various event types
using EventTreatMap = std::map<event_type::EventType, EventTreatment>;
/**! Input parameters.
*
* This struct handles stores all configuration parameters
* needed in a HEJ 2 run.
*
* \internal To add a new option:
* 1. Add a member to the Config struct.
* 2. Inside "src/YAMLreader.cc":
* - Add the option name to the "supported" Node in
* get_supported_options.
* - Initialise the new Config member in to_Config.
* The functions set_from_yaml (for mandatory options) and
* set_from_yaml_if_defined (non-mandatory) may be helpful.
* 3. Add a new entry (with short description) to config.yaml
* 4. Update the user documentation in "doc/Sphinx/"
*/
struct Config {
//! Parameters for scale variation
ScaleConfig scales;
//! Resummation jet properties
JetParameters resummation_jets;
//! Fixed-order jet properties
JetParameters fixed_order_jets;
//! Minimum transverse momentum for extremal partons
double min_extparton_pt;
//! Maximum transverse momentum fraction from soft radiation in extremal jets
double max_ext_soft_pt_fraction;
//! Number of resummation configurations to generate per fixed-order event
int trials;
//! Whether to include the logarithmic correction from \f$\alpha_s\f$ running
bool log_correction;
- //! Whether to perform unweighting
- bool unweight;
//! Event output files names and formats
std::vector<OutputFile> output;
//! Parameters for random number generation
RNGConfig rng;
//! Map to decide what to do for different event types
EventTreatMap treat;
//! Parameters for custom analyses
YAML::Node analysis_parameters;
//! Settings for effective Higgs-gluon coupling
HiggsCouplingSettings Higgs_coupling;
};
//! Configuration options for the PhaseSpacePoint class
struct PhaseSpacePointConfig {
//! Properties of resummation jets
JetParameters jet_param;
//! Minimum transverse momentum for extremal partons
double min_extparton_pt;
//! Maximum transverse momentum fraction from soft radiation in extremal jets
double max_ext_soft_pt_fraction;
};
//! Configuration options for the MatrixElement class
struct MatrixElementConfig {
//! Whether to include the logarithmic correction from \f$\alpha_s\f$ running
bool log_correction;
//! Settings for effective Higgs-gluon coupling
HiggsCouplingSettings Higgs_coupling;
};
//! Configuration options for the EventReweighter class
struct EventReweighterConfig {
//! Settings for phase space point generation
PhaseSpacePointConfig psp_config;
//! Settings for matrix element calculation
MatrixElementConfig ME_config;
//! Properties of resummation jets
JetParameters jet_param;
//! Treatment of the various event types
EventTreatMap treat;
};
/**! Extract PhaseSpacePointConfig from Config
*
* \internal We do not provide a PhaseSpacePointConfig constructor from Config
* so that PhaseSpacePointConfig remains an aggregate.
* This faciliates writing client code (e.g. the HEJ fixed-order generator)
* that creates a PhaseSpacePointConfig *without* a Config object.
*
* @see to_MatrixElementConfig, to_EventReweighterConfig
*/
inline
PhaseSpacePointConfig to_PhaseSpacePointConfig(Config const & conf) {
- return {conf.resummation_jets, conf.min_extparton_pt, conf.max_ext_soft_pt_fraction};
+ return {
+ conf.resummation_jets,
+ conf.min_extparton_pt,
+ conf.max_ext_soft_pt_fraction
+ };
}
/**! Extract MatrixElementConfig from Config
*
* @see to_PhaseSpacePointConfig, to_EventReweighterConfig
*/
inline
MatrixElementConfig to_MatrixElementConfig(Config const & conf) {
return {conf.log_correction, conf.Higgs_coupling};
}
/**! Extract EventReweighterConfig from Config
*
* @see to_PhaseSpacePointConfig, to_MatrixElementConfig
*/
inline
EventReweighterConfig to_EventReweighterConfig(Config const & conf) {
return {
to_PhaseSpacePointConfig(conf),
to_MatrixElementConfig(conf),
conf.resummation_jets, conf.treat
};
}
} // namespace HEJ
diff --git a/include/HEJ/currents.hh b/include/HEJ/currents.hh
index db2e535..fb2ffaf 100644
--- a/include/HEJ/currents.hh
+++ b/include/HEJ/currents.hh
@@ -1,1332 +1,1333 @@
//////////////////////////////////////////////////
//////////////////////////////////////////////////
// This source code is Copyright (2012) of //
// Jeppe R. Andersen and Jennifer M. Smillie //
// and is distributed under the //
// Gnu Public License version 2 //
// http://www.gnu.org/licenses/gpl-2.0.html //
// You are allowed to distribute and alter the //
// source under the conditions of the GPLv2 //
// as long as this copyright notice //
// is unaltered and distributed with the source //
// Any use should comply with the //
// MCNET GUIDELINES //
// for Event Generator Authors and Users //
// as distributed with this source code //
//////////////////////////////////////////////////
//////////////////////////////////////////////////
/** \file
* \brief Functions computing the square of current contractions.
*
* This file contains all the necessary functions to compute the current
* contractions for all valid HEJ processes. PJETS, H+JETS and W+JETS along with
* some unordered counterparts.
*
* @TODO add a namespace
*/
-
#pragma once
-#include <CLHEP/Vector/LorentzVector.h>
#include <complex>
#include <vector>
#include <valarray>
#include <limits>
+#include <ostream>
+
+#include <CLHEP/Vector/LorentzVector.h>
typedef std::complex<double> COM;
typedef COM current[4];
typedef CLHEP::HepLorentzVector HLV;
//! Square of qQ->qenuQ W+Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @returns Square of the current contractions for qQ->qenuQ Scattering
*
* This returns the square of the current contractions in qQ->qenuQ scattering
* with an emission of a W Boson.
*/
double jMWqQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe,
CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qbarQ->qbarenuQ W+Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @returns Square of the current contractions for qbarQ->qbarenuQ Scattering
*
* This returns the square of the current contractions in qbarQ->qbarenuQ scattering
* with an emission of a W Boson.
*/
double jMWqbarQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe,
CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qQbar->qenuQbar W+Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @returns Square of the current contractions for qQbar->qenuQbar Scattering
*
* This returns the square of the current contractions in qQbar->qenuQbar scattering
* with an emission of a W Boson.
*/
double jMWqQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe,
CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qbarQbar->qbarenuQbar W+Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @returns Square of the current contractions for qbarQbar->qbarenuQbar Scattering
*
* This returns the square of the current contractions in qbarQbar->qbarenuQbar scattering
* with an emission of a W Boson.
*/
double jMWqbarQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe,
CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qg->qenug W+Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @returns Square of the current contractions for qg->qenug Scattering
*
* This returns the square of the current contractions in qg->qenug scattering
* with an emission of a W Boson.
*/
double jMWqg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe,
CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qbarg->qbarenug W+Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @returns Square of the current contractions for qbarg->qbarenug Scattering
*
* This returns the square of the current contractions in qbarg->qbarenug scattering
* with an emission of a W Boson.
*/
double jMWqbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe,
CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
// W+Jets Unordered Functions
//! qQg Wjets Unordered backwards opposite leg to W
/**
* @param p1out Momentum of final state quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state quark b
* @param p2in Momentum of intial state quark b
* @param pg Momentum of final state unordered gluon
* @returns Square of the current contractions for qQ->qQg Scattering
*
* This returns the square of the current contractions in qQg->qQg scattering
* with an emission of a W Boson.
*/
double junobMWqQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector pg);
//! qbarQg Wjets Unordered backwards opposite leg to W
/**
* @param p1out Momentum of final state anti-quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state anti-quark a
* @param p2out Momentum of final state quark b
* @param p2in Momentum of intial state quark b
* @param pg Momentum of final state unordered gluon
* @returns Square of the current contractions for qbarQ->qbarQg Scattering
*
* This returns the square of the current contractions in qbarQg->qbarQg scattering
* with an emission of a W Boson.
*/
double junobMWqbarQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector pg);
//! qQbarg Wjets Unordered backwards opposite leg to W
/**
* @param p1out Momentum of final state quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state anti-quark b
* @param p2in Momentum of intial state anti-quark b
* @param pg Momentum of final state unordered gluon
* @returns Square of the current contractions for qQbar->qQbarg Scattering
*
* This returns the square of the current contractions in qQbarg->qQbarg scattering
* with an emission of a W Boson.
*/
double junobMWqQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector pg);
//! qbarQbarg Wjets Unordered backwards opposite leg to W
/**
* @param p1out Momentum of final state anti-quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state anti-quark a
* @param p2out Momentum of final state anti-quark b
* @param p2in Momentum of intial state anti-quark b
* @param pg Momentum of final state unordered gluon
* @returns Square of the current contractions for qbarQbar->qbarQbarg Scattering
*
* This returns the square of the current contractions in qbarQbarg->qbarQbarg scattering
* with an emission of a W Boson.
*/
double junobMWqbarQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector pg);
//!Wjets Unordered forwards opposite leg to W
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state quark b
* @param p2in Momentum of intial state quark b
* @returns Square of the current contractions for qQ->gqQ Scattering
*
* This returns the square of the current contractions in qQg->gqQ scattering
* with an emission of a W Boson.
*/
double junofMWgqQ (CLHEP::HepLorentzVector pg,CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p2in);
//!Wjets Unordered forwards opposite leg to W
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state anti-quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state anti-quark a
* @param p2out Momentum of final state quark b
* @param p2in Momentum of intial state quark b
* @returns Square of the current contractions for qbarQ->gqbarQ Scattering
*
* This returns the square of the current contractions in qbarQg->gqbarQ scattering
* with an emission of a W Boson.
*/
double junofMWgqbarQ (CLHEP::HepLorentzVector pg,CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p2in);
//!Wjets Unordered forwards opposite leg to W
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state anti-quark b
* @param p2in Momentum of intial state anti-quark b
* @returns Square of the current contractions for qQbar->gqQbar Scattering
*
* This returns the square of the current contractions in qQbarg->gqQbar scattering
* with an emission of a W Boson.
*/
double junofMWgqQbar (CLHEP::HepLorentzVector pg,CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p2in);
//!Wjets Unordered forwards opposite leg to W
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state anti-quark a
* @param pe Momentum of final state electron
* @param pnu Momentum of final state Neutrino
* @param p1in Momentum of initial state anti-quark a
* @param p2out Momentum of final state anti-quark b
* @param p2in Momentum of intial state anti-quark b
* @returns Square of the current contractions for qbarQbar->gqbarQbar Scattering
*
* This returns the square of the current contractions in qbarQbarg->gqbarQbar scattering
* with an emission of a W Boson.
*/
double junofMWgqbarQbar (CLHEP::HepLorentzVector pg,CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector pe, CLHEP::HepLorentzVector pnu, CLHEP::HepLorentzVector p2in);
//!W+uno same leg
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state quark b
* @param p2in Momentum of intial state quark b
* @returns Square of the current contractions for qQ->qQg Scattering
*
* This returns the square of the current contractions in gqQ->gqQ scattering
* with an emission of a W Boson.
*/
double jM2WunogqQ(CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! @TODO What does this function do? Crossed contribution is Exqqx..?
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state quark b
* @param p2in Momentum of intial state quark b
* @returns Square of the current contractions for qQ->gqQ Scattering
*
* This returns the square of the current contractions in gqQ->gqQ scattering
* with an emission of a W Boson.
*/
double jM2WunogqQ_crossqQ(CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! W+uno same leg. quark anti-quark
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state anti-quark b
* @param p2in Momentum of intial state anti-quark b
* @returns Square of the current contractions for qQbar->gqQbar Scattering
*
* This returns the square of the current contractions in gqQbar->gqQbar scattering
* with an emission of a W Boson. (Unordered Same Leg)
*/
double jM2WunogqQbar(CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! W+uno same leg. quark gluon
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param p1in Momentum of initial state quark a
* @param p2out Momentum of final state gluon b
* @param p2in Momentum of intial state gluon b
* @returns Square of the current contractions for qg->gqg Scattering
*
* This returns the square of the current contractions in qg->gqg scattering
* with an emission of a W Boson.
*/
double jM2Wunogqg(CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! W+uno same leg. anti-quark quark
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state anti-quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param p1in Momentum of initial state anti-quark a
* @param p2out Momentum of final state quark b
* @param p2in Momentum of intial state quark b
* @returns Square of the current contractions for qbarQ->gqbarQ Scattering
*
* This returns the square of the current contractions in qbarQ->gqbarQ scattering
* with an emission of a W Boson.
*/
double jM2WunogqbarQ(CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! W+uno same leg. anti-quark anti-quark
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state anti-quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param p1in Momentum of initial state anti-quark a
* @param p2out Momentum of final state anti-quark b
* @param p2in Momentum of intial state anti-quark b
* @returns Square of the current contractions for qbarQbar->gqbarQbar Scattering
*
* This returns the square of the current contractions in gqbarQbar->qbarQbar scattering
* with an emission of a W Boson.
*/
double jM2WunogqbarQbar(CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! W+uno same leg. anti-quark gluon
/**
* @param pg Momentum of final state unordered gluon
* @param p1out Momentum of final state anti-quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param p1in Momentum of initial state anti-quark a
* @param p2out Momentum of final state gluon b
* @param p2in Momentum of intial state gluon b
* @returns Square of the current contractions for ->gqbarg Scattering
*
* This returns the square of the current contractions in qbarg->gqbarg scattering
* with an emission of a W Boson.
*/
double jM2Wunogqbarg(CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//W+Jets qqxExtremal
//! W+Extremal qqx. qxqQ
/**
* @param pgin Momentum of initial state gluon
* @param pqout Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param pqbarout Momentum of final state anti-quark a
* @param p2out Momentum of initial state anti-quark b
* @param p2in Momentum of final state gluon b
* @returns Square of the current contractions for ->qbarqQ Scattering
*
* Calculates the square of the current contractions with extremal qqbar pair
* production. This is calculated through the use of crossing symmetry.
*/
double jM2WgQtoqbarqQ(CLHEP::HepLorentzVector pgin, CLHEP::HepLorentzVector pqout,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector pqbarout, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//W+Jets qqxExtremal
//! W+Extremal qqx. qqxQ
/**
* @param pgin Momentum of initial state gluon
* @param pqout Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param pqbarout Momentum of final state anti-quark a
* @param p2out Momentum of initial state anti-quark b
* @param p2in Momentum of final state gluon b
* @returns Square of the current contractions for ->qqbarQ Scattering
*
* Calculates the square of the current contractions with extremal qqbar pair
* production. This is calculated through the use of crossing symmetry.
*/
double jM2WgQtoqqbarQ(CLHEP::HepLorentzVector pgin, CLHEP::HepLorentzVector pqout,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector pqbarout, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//W+Jets qqxExtremal
//! W+Extremal qqx. gg->qxqg
/**
* @param pgin Momentum of initial state gluon
* @param pqout Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param pqbarout Momentum of final state anti-quark a
* @param p2out Momentum of initial state gluon b
* @param p2in Momentum of final state gluon b
* @returns Square of the current contractions for gg->qbarqg Scattering
*
* Calculates the square of the current contractions with extremal qqbar pair
* production. This is calculated through the use of crossing symmetry.
*/
double jM2Wggtoqbarqg(CLHEP::HepLorentzVector pgin, CLHEP::HepLorentzVector pqout,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector pqbarout, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//W+Jets qqxExtremal
//! W+Extremal qqx. gg->qqxg
/**
* @param pgin Momentum of initial state gluon
* @param pqout Momentum of final state quark a
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param pqbarout Momentum of final state anti-quark a
* @param p2out Momentum of initial state gluon a
* @param p2in Momentum of final state gluon b
* @returns Square of the current contractions for gg->qqbarg Scattering
*
* Calculates the square of the current contractions with extremal qqbar pair
* production. This is calculated through the use of crossing symmetry.
*/
double jM2Wggtoqqbarg(CLHEP::HepLorentzVector pgin, CLHEP::HepLorentzVector pqbarout,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, CLHEP::HepLorentzVector pqout, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//W+Jets qqxExtremal, W emission from opposite leg
//! W+Extremal qqx. gg->qqxg. qqx on forwards leg, W emission backwards leg.
/**
* @param pa Momentum of initial state (anti-)quark
* @param pb Momentum of initial state gluon
* @param p1 Momentum of final state (anti-)quark (after W emission)
* @param p2 Momentum of final state anti-quark
* @param p3 Momentum of final state quark
* @param plbar Momentum of final state anti-lepton
* @param pl Momentum of final state lepton
* @param aqlinepa Is opposite extremal leg to qqx a quark or antiquark line
* @returns Square of the current contractions for gq->qqbarqW Scattering
*
* Calculates the square of the current contractions with extremal qqbar pair
* production. This is calculated via current contraction of existing currents.
* Assumes qqx split from forwards leg, W emission from backwards leg.
* Switch input (pa<->pb, p1<->pn) if calculating forwards qqx.
*/
double jM2WgqtoQQqW(CLHEP::HepLorentzVector pa, CLHEP::HepLorentzVector pb, CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector p2, CLHEP::HepLorentzVector p3,CLHEP::HepLorentzVector plbar,CLHEP::HepLorentzVector pl, bool aqlinepa);
//! W+Jets qqxCentral. qqx W emission.
/**
* @param pa Momentum of initial state particle a
* @param pb Momentum of initial state particle b
* @param pl Momentum of final state lepton
* @param plbar Momentum of final state anti-lepton
* @param partons Vector of outgoing parton momenta
* @param aqlinepa Bool: True= pa is anti-quark
* @param aqlinepb Bool: True= pb is anti-quark
* @param qqxmarker Bool: Ordering of the qqbar pair produced (qqx vs qxq)
* @param nabove Number of lipatov vertices "above" qqbar pair
* @param nbelow Number of lipatov vertices "below" qqbar pair
* @returns Square of the current contractions for qq>qQQbarWq Scattering
*
* Calculates the square of the current contractions with extremal qqbar pair
* production. This is calculated through the use of crossing symmetry.
*/
double jM2WqqtoqQQq(HLV pa, HLV pb,HLV pl,HLV plbar, std::vector<HLV> partons, bool aqlinepa, bool aqlinepb, bool qqxmarker, int nabove);
//emission from backwards leg
//! W+Jets qqxCentral. W emission from backwards leg.
/**
* @param ka HLV: Momentum of initial state particle a
* @param kb HLV: Momentum of initial state particle b
* @param pl HLV: Momentum of final state lepton
* @param plbar HLV: Momentum of final state anti-lepton
* @param partons Vector(HLV): outgoing parton momenta
* @param aqlinepa Bool: True= pa is anti-quark
* @param aqlinepb Bool: True= pb is anti-quark
* @param qqxmarker Bool: Ordering of the qqbar pair produced (qqx vs qxq)
* @param nabove Int: Number of lipatov vertices "above" qqbar pair
* @param nbelow Int: Number of lipatov vertices "below" qqbar pair
* @param forwards Bool: Swap to emission off front leg TODO:remove so args can be const
* @returns Square of the current contractions for qq>qQQbarWq Scattering
*
* Calculates the square of the current contractions with extremal qqbar pair
* production. This is calculated through the use of crossing symmetry.
*/
double jM2WqqtoqQQqW(HLV ka, HLV kb,HLV pl,HLV plbar, std::vector<HLV> partons, bool aqlinepa, bool aqlinepb, bool qqxmarker, int nabove, int nbelow, bool forwards); //Doing
//! Square of qQ->qQ Pure Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @returns Square of the current contractions for qQ->qQ Scattering
*
* This returns the square of the current contractions in qQ->qQ Pure Jet Scattering.
*/
double jM2qQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qQbar->qQbar Pure Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @returns Square of the current contractions for qQbar->qQbar Scattering
*
* This returns the square of the current contractions in qQbar->qQbar Pure Jet Scattering.
* Note this can be used for qbarQ->qbarQ Scattering by inputting arguments appropriately.
*/
double jM2qQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qbarQbar->qbarQbar Pure Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @returns Square of the current contractions for qbarQbar->qbarQbar Scattering
*
* This returns the square of the current contractions in qbarQbar->qbarQbar Pure Jet Scattering.
*/
double jM2qbarQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qg->qg Pure Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @returns Square of the current contractions for qg->qg Scattering
*
* This returns the square of the current contractions in qg->qg Pure Jet Scattering.
* Note this can be used for gq->gq Scattering by inputting arguments appropriately.
*/
double jM2qg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of qbarg->qbarg Pure Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @returns Square of the current contractions for qbarg->qbarg Scattering
*
* This returns the square of the current contractions in qbarg->qbarg Pure Jet Scattering.
* Note this can be used for gqbar->gqbar Scattering by inputting arguments appropriately.
*/
double jM2qbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of gg->gg Pure Jets Scattering Current
/**
* @param p1out Momentum of final state gluon
* @param p1in Momentum of initial state gluon
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @returns Square of the current contractions for gg->gg Scattering
*
* This returns the square of the current contractions in gg->gg Pure Jet Scattering.
*/
double jM2gg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in);
//! Square of gg->gg Higgs+Jets Scattering Current
/**
* @param p1out Momentum of final state gluon
* @param p1in Momentum of initial state gluon
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @param q1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for gg->gg Scattering
*
* This returns the square of the current contractions in gg->gg Higgs+Jet Scattering.
*
* g~p1 g~p2
* should be called with q1 meant to be contracted with p2 in first part of vertex
* (i.e. if g is backward, q1 is forward)
*/
double MH2gg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of gq->gq Higgs+Jets Scattering Current with Higgs before Gluon
/**
* @param p1out Momentum of final state gluon
* @param p1in Momentum of initial state gluon
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @param pH Momentum of Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contraction
*
*/
double MH2gq_outsideH(CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector pH,
double mt,
bool include_bottom, double mb);
//! Square of qg->qg Higgs+Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @param q1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qg->qg Scattering
*
* This returns the square of the current contractions in qg->qg Higgs+Jet Scattering.
*
* q~p1 g~p2 (i.e. ALWAYS p1 for quark, p2 for gluon)
* should be called with q1 meant to be contracted with p2 in first part of vertex
* (i.e. if g is backward, q1 is forward)
*/
double MH2qg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qbarg->qbarg Higgs+Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @param q1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarg->qbarg Scattering
*
* This returns the square of the current contractions in qbarg->qbarg Higgs+Jet Scattering.
*
* qbar~p1 g~p2 (i.e. ALWAYS p1 for anti-quark, p2 for gluon)
* should be called with q1 meant to be contracted with p2 in first part of vertex
* (i.e. if g is backward, q1 is forward)
*/
double MH2qbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qQ->qQ Higgs+Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @param q1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qQ->qQ Scattering
*
* This returns the square of the current contractions in qQ->qQ Higgs+Jet Scattering.
*
* q~p1 Q~p2 (i.e. ALWAYS p1 for quark, p2 for quark)
* should be called with q1 meant to be contracted with p2 in first part of vertex
* (i.e. if Q is backward, q1 is forward)
*/
double MH2qQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qQbar->qQbar Higgs+Jets Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @param q1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qQ->qQ Scattering
*
* This returns the square of the current contractions in qQbar->qQbar Higgs+Jet Scattering.
*
* q~p1 Qbar~p2 (i.e. ALWAYS p1 for quark, p2 for anti-quark)
* should be called with q1 meant to be contracted with p2 in first part of vertex
* (i.e. if Qbar is backward, q1 is forward)
*/
double MH2qQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qbarQ->qbarQ Higgs+Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @param q1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarQ->qbarQ Scattering
*
* This returns the square of the current contractions in qbarQ->qbarQ Higgs+Jet Scattering.
*
* qbar~p1 Q~p2 (i.e. ALWAYS p1 for anti-quark, p2 for quark)
* should be called with q1 meant to be contracted with p2 in first part of vertex
* (i.e. if Q is backward, q1 is forward)
*/
double MH2qbarQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qbarQbar->qbarQbar Higgs+Jets Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @param q1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarQbar->qbarQbar Scattering
*
* This returns the square of the current contractions in qbarQbar->qbarQbar Higgs+Jet Scattering.
*
* qbar~p1 Qbar~p2 (i.e. ALWAYS p1 for anti-quark, p2 for anti-quark)
* should be called with q1 meant to be contracted with p2 in first part of vertex
* (i.e. if Qbar is backward, q1 is forward)
*/
double MH2qbarQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
// Unordered f
//! Square of qQ->gqQ Higgs+Jets Unordered f Scattering Current
/**
* @param pg Momentum of unordered gluon
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qQ->gqQ Scattering
*
* This returns the square of the current contractions in qQ->gqQ Higgs+Jet Scattering.
*
* This construction is taking rapidity order: pg > p1out >> p2out
*/
double jM2unogqHQ (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,
CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qQbar->gqQbar Higgs+Jets Unordered f Scattering Current
/**
* @param pg Momentum of unordered gluon
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qQbar->gqQbar Scattering
*
* This returns the square of the current contractions in qQbar->gqQbar Higgs+Jet Scattering.
*
* This construction is taking rapidity order: pg > p1out >> p2out
*/
double jM2unogqHQbar (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,
CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qbarQ->gqbarQ Higgs+Jets Unordered f Scattering Current
/**
* @param pg Momentum of unordered gluon
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarQ->gqbarQ Scattering
*
* This returns the square of the current contractions in qbarQ->gqbarQ Higgs+Jet Scattering.
*
* This construction is taking rapidity order: pg > p1out >> p2out
*/
double jM2unogqbarHQ (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,
CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qbarQbar->gqbarQbar Higgs+Jets Unordered f Scattering Current
/**
* @param pg Momentum of unordered gluon
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarQbar->gqbarQbar Scattering
*
* This returns the square of the current contractions in qbarQbar->gqbarQbar Higgs+Jet Scattering.
*
* This construction is taking rapidity order: pg > p1out >> p2out
*/
double jM2unogqbarHQbar (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,
CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qg->gqg Higgs+Jets Unordered f Scattering Current
/**
* @param pg Momentum of unordered gluon
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qg->gqg Scattering
*
* This returns the square of the current contractions in qg->gqg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: pg > p1out >> p2out
*/
double jM2unogqHg (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,
CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qbarg->gqbarg Higgs+Jets Unordered f Scattering Current
/**
* @param pg Momentum of unordered gluon
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param p2out Momentum of final state gluon
* @param p2in Momentum of intial state gluon
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarg->gbarg Scattering
*
* This returns the square of the current contractions in qbarg->gqbarg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: pg > p1out >> p2out
*/
double jM2unogqbarHg (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out,
CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//Unordered b
//! Square of qbarQ->qbarQg Higgs+Jets Unordered b Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param pg Momentum of unordered b gluon
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarQ->qbarQg Scattering
*
* This returns the square of the current contractions in qbarQ->qbarQg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: p1out >> p2out > pg
*/
double jM2unobqbarHQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qQ->qQg Higgs+Jets Unordered b Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param pg Momentum of unordered b gluon
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qQ->qQg Scattering
*
* This returns the square of the current contractions in qQ->qQg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: p1out >> p2out > pg
*/
double jM2unobqHQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qQbar->qQbarg Higgs+Jets Unordered b Scattering Current
/**
* @param p1out Momentum of final state quark
* @param p1in Momentum of initial state quark
* @param pg Momentum of unordered b gluon
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qQbar->qQbarg Scattering
*
* This returns the square of the current contractions in qQbar->qQbarg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: p1out >> p2out > pg
*/
double jM2unobqHQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of qbarQbar->qbarQbarg Higgs+Jets Unordered b Scattering Current
/**
* @param p1out Momentum of final state anti-quark
* @param p1in Momentum of initial state anti-quark
* @param pg Momentum of unordered b gluon
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for qbarQbar->qbarQbarg Scattering
*
* This returns the square of the current contractions in qbarQbar->qbarQbarg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: p1out >> p2out > pg
*/
double jM2unobqbarHQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of gQbar->gQbarg Higgs+Jets Unordered b Scattering Current
/**
* @param p1out Momentum of final state gluon
* @param p1in Momentum of initial state gluon
* @param pg Momentum of unordered b gluon
* @param p2out Momentum of final state anti-quark
* @param p2in Momentum of intial state anti-quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for gQbar->gQbarg Scattering
*
* This returns the square of the current contractions in gQbar->gQbarg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: p1out >> p2out > pg
*/
double jM2unobgHQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
//! Square of gQ->gQg Higgs+Jets Unordered b Scattering Current
/**
* @param p1out Momentum of final state gluon
* @param p1in Momentum of initial state gluon
* @param pg Momentum of unordered b gluon
* @param p2out Momentum of final state quark
* @param p2in Momentum of intial state quark
* @param qH1 Momentum of t-channel propagator before Higgs
* @param qH2 Momentum of t-channel propagator after Higgs
* @param mt Top quark mass
* @param include_bottom Specifies whether bottom corrections are included
* @param mb Bottom quark mass
* @returns Square of the current contractions for gQ->gQg Scattering
*
* This returns the square of the current contractions in gQ->gQg Higgs+Jet Scattering.
*
* This construction is taking rapidity order: p1out >> p2out > pg
*/
double jM2unobgHQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out,
CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1,
CLHEP::HepLorentzVector qH2,
double mt,
bool include_bottom, double mb);
// impact factors for Higgs + jet
//! Implements Eq. (4.22) in hep-ph/0301013 with modifications to incoming plus momenta
/**
* @param p2 Momentum of Particle 2
* @param p1 Momentum of Particle 1
* @param pH Momentum of Higgs
* @returns Value of Eq. (4.22) in Hep-ph/0301013 with modifications
*
* This gives the impact factor. First it determines first whether this is the case
* p1p\sim php>>p3p or the opposite
*/
double C2gHgm(CLHEP::HepLorentzVector p2, CLHEP::HepLorentzVector p1,
CLHEP::HepLorentzVector pH);
//! Implements Eq. (4.23) in hep-ph/0301013 with modifications to incoming plus momenta
/**
* @param p2 Momentum of Particle 2
* @param p1 Momentum of Particle 1
* @param pH Momentum of Higgs
* @returns Value of Eq. (4.23) in Hep-ph/0301013
*
* This gives the impact factor. First it determines first whether this is the case
* p1p\sim php>>p3p or the opposite
*/
double C2gHgp(CLHEP::HepLorentzVector p2, CLHEP::HepLorentzVector p1,
CLHEP::HepLorentzVector pH);
//! Implements Eq. (4.22) in hep-ph/0301013
/**
* @param p2 Momentum of Particle 2
* @param p1 Momentum of Particle 1
* @param pH Momentum of Higgs
* @returns Value of Eq. (4.22) in Hep-ph/0301013
*
* This gives the impact factor. First it determines first whether this is the case
* p1p\sim php>>p3p or the opposite
*/
double C2qHqm(CLHEP::HepLorentzVector p2, CLHEP::HepLorentzVector p1,
CLHEP::HepLorentzVector pH);
/** \class CCurrent currents.hh "include/HEJ/currents.hh"
* \brief This is the a new class structure for currents.
*/
class CCurrent
{
public:
CCurrent(COM sc0, COM sc1, COM sc2, COM sc3)
:c0(sc0),c1(sc1),c2(sc2),c3(sc3)
{};
CCurrent(const CLHEP::HepLorentzVector p)
{
c0=p.e();
c1=p.px();
c2=p.py();
c3=p.pz();
};
CCurrent()
{};
CCurrent operator+(const CCurrent& other);
CCurrent operator-(const CCurrent& other);
CCurrent operator*(const double x);
CCurrent operator*(const COM x);
CCurrent operator/(const double x);
CCurrent operator/(const COM x);
friend std::ostream& operator<<(std::ostream& os, const CCurrent& cur);
COM dot(CLHEP::HepLorentzVector p1);
COM dot(CCurrent p1);
COM c0,c1,c2,c3;
private:
};
/* std::ostream& operator <<(std::ostream& os, const CCurrent& cur); */
CCurrent operator * ( double x, CCurrent& m);
CCurrent operator * ( COM x, CCurrent& m);
CCurrent operator / ( double x, CCurrent& m);
CCurrent operator / ( COM x, CCurrent& m);
//! Current <outgoing state | mu | incoming state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
//! @TODO remove
[[deprecated("Use joi instead")]]
void j (CLHEP::HepLorentzVector pout, bool helout, CLHEP::HepLorentzVector pin, bool helin,current &cur);
//! Current <incoming state | mu | outgoing state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
void jio(HLV pin, bool helin, HLV pout, bool helout, current &cur);
//! Current <outgoing state | mu | outgoing state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
void joo(HLV pi, bool heli, HLV pj, bool helj, current &cur);
//! Current <outgoing state | mu | incoming state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
void joi(HLV pout, bool helout, HLV pin, bool helin, current &cur);
//! Current <outgoing state | mu | incoming state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
//! @TODO remove
[[deprecated("Use joi instead")]]
CCurrent j (CLHEP::HepLorentzVector pout, bool helout, CLHEP::HepLorentzVector pin, bool helin);
//! Current <outgoing state | mu | incoming state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
CCurrent joi (CLHEP::HepLorentzVector pout, bool helout, CLHEP::HepLorentzVector pin, bool helin);
//! Current <incoming state | mu | outgoing state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
CCurrent jio (CLHEP::HepLorentzVector pout, bool helout, CLHEP::HepLorentzVector pin, bool helin);
//! Current <outgoing state | mu | outgoing state>
/**
* These functions are a mess. There are many more defined in the source file than declared in the
* header - and the arguments are mislabelled in some cases. Need to investigate.
*/
CCurrent joo (CLHEP::HepLorentzVector pout, bool helout, CLHEP::HepLorentzVector pin, bool helin);
inline COM cdot(const current & j1, const current & j2)
{
return j1[0]*j2[0]-j1[1]*j2[1]-j1[2]*j2[2]-j1[3]*j2[3];
}
inline COM cdot(const HLV & p, const current & j1) {
return j1[0]*p.e()-j1[1]*p.x()-j1[2]*p.y()-j1[3]*p.z();
}
inline void cmult(const COM & factor, const current & j1, current &cur)
{
cur[0]=factor*j1[0];
cur[1]=factor*j1[1];
cur[2]=factor*j1[2];
cur[3]=factor*j1[3];
}
// WHY!?!
inline void cadd(const current & j1, const current & j2, const current & j3,
const current & j4, const current & j5, current &sum)
{
sum[0]=j1[0]+j2[0]+j3[0]+j4[0]+j5[0];
sum[1]=j1[1]+j2[1]+j3[1]+j4[1]+j5[1];
sum[2]=j1[2]+j2[2]+j3[2]+j4[2]+j5[2];
sum[3]=j1[3]+j2[3]+j3[3]+j4[3]+j5[3];
}
inline void cadd(const current & j1, const current & j2, const current & j3,
const current & j4, current &sum) {
sum[0] = j1[0] + j2[0] + j3[0] + j4[0];
sum[1] = j1[1] + j2[1] + j3[1] + j4[1];
sum[2] = j1[2] + j2[2] + j3[2] + j4[2];
sum[3] = j1[3] + j2[3] + j3[3] + j4[3];
}
inline void cadd(const current & j1, const current & j2, const current & j3,
current &sum)
{
sum[0]=j1[0]+j2[0]+j3[0];
sum[1]=j1[1]+j2[1]+j3[1];
sum[2]=j1[2]+j2[2]+j3[2];
sum[3]=j1[3]+j2[3]+j3[3];
}
inline void cadd(const current & j1, const current & j2, current &sum)
{
sum[0]=j1[0]+j2[0];
sum[1]=j1[1]+j2[1];
sum[2]=j1[2]+j2[2];
sum[3]=j1[3]+j2[3];
}
inline double abs2(const COM & a)
{
return (a*conj(a)).real();
}
inline double vabs2(const CCurrent & cur)
{
return abs2(cur.c0)-abs2(cur.c1)-abs2(cur.c2)-abs2(cur.c3);
}
inline double vre(const CCurrent & a, const CCurrent & b)
{
return real(a.c0*conj(b.c0)-a.c1*conj(b.c1)-a.c2*conj(b.c2)-a.c3*conj(b.c3));
}
// @TODO: These are not currents and should be moved elsewhere.
double K_g(double p1minus, double paminus);
double K_g(CLHEP::HepLorentzVector const & pout, CLHEP::HepLorentzVector const & pin);
diff --git a/include/HEJ/event_types.hh b/include/HEJ/event_types.hh
index 1aee605..d2e6097 100644
--- a/include/HEJ/event_types.hh
+++ b/include/HEJ/event_types.hh
@@ -1,77 +1,80 @@
/** \file
* \brief Define different types of events.
*
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include "HEJ/utility.hh"
namespace HEJ{
//! Namespace for event types
namespace event_type{
//! Possible event types
enum EventType: size_t{
FKL, /**< FKL-type event */
unordered_backward, /**< event with unordered backward emission */
unordered_forward, /**< event with unordered forward emission */
extremal_qqxb, /**< event with a backward extremal qqbar */
extremal_qqxf, /**< event with a forward extremal qqbar */
central_qqx, /**< event with a central qqbar */
nonHEJ, /**< event configuration not covered by HEJ */
no_2_jets, /**< event with less than two jets */
bad_final_state, /**< event with an unsupported final state */
unob = unordered_backward,
unof = unordered_forward,
qqxexb = extremal_qqxb,
qqxexf = extremal_qqxf,
qqxmid = central_qqx,
first_type = FKL,
last_type = bad_final_state
};
//! Event type names
/**
* For example, names[FKL] is the string "FKL"
*/
static constexpr auto names = make_array(
"FKL",
"unordered backward",
"unordered forward",
"extremal qqbar backward",
"extremal qqbar forward",
"central qqbar",
"nonHEJ",
"no 2 jets",
"bad final state"
);
inline
bool is_HEJ(EventType type) {
switch(type) {
case FKL:
case unordered_backward:
case unordered_forward:
case extremal_qqxb:
case extremal_qqxf:
case central_qqx:
return true;
default:
return false;
}
}
inline
bool is_uno(EventType type) {
return type == unordered_backward || type == unordered_forward;
}
inline
bool is_qqx(EventType type) {
return type == extremal_qqxb || type == extremal_qqxf || type == central_qqx;
}
}
}
diff --git a/include/HEJ/exceptions.hh b/include/HEJ/exceptions.hh
index 687edf1..8fdeabf 100644
--- a/include/HEJ/exceptions.hh
+++ b/include/HEJ/exceptions.hh
@@ -1,53 +1,57 @@
/** \file
* \brief Custom exception classes
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <stdexcept>
namespace HEJ{
//! Exception indicating wrong option type
/**
* This exception is thrown if a configuration option has
* the wrong type (e.g. 'trials' is not set to a number)
*/
struct invalid_type: std::invalid_argument {
explicit invalid_type(std::string const & what):
std::invalid_argument{what} {};
explicit invalid_type(char const * what):
std::invalid_argument{what} {};
};
//! Exception indicating unknown option
/**
* This exception is thrown if an unknown configuration option
* is set (e.g. the 'trials' setting is misspelt as 'trails')
*/
struct unknown_option: std::invalid_argument {
explicit unknown_option(std::string const & what):
std::invalid_argument{what} {};
explicit unknown_option(char const * what):
std::invalid_argument{what} {};
};
//! Exception indicating missing option setting
/**
* This exception is thrown if a mandatory configuration option
* (e.g. 'trials') is not set.
*/
struct missing_option: std::logic_error {
explicit missing_option(std::string const & what):
std::logic_error{what} {};
explicit missing_option(char const * what):
std::logic_error{what} {};
};
//! Exception indicating functionality that has not been implemented yet
struct not_implemented: std::logic_error {
explicit not_implemented(std::string const & what):
std::logic_error{what} {};
explicit not_implemented(char const * what):
std::logic_error{what} {};
};
}
diff --git a/include/HEJ/get_analysis.hh b/include/HEJ/get_analysis.hh
index 46d3fc3..8572f44 100644
--- a/include/HEJ/get_analysis.hh
+++ b/include/HEJ/get_analysis.hh
@@ -1,30 +1,32 @@
/** \file
* \brief Contains the get_analysis function
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <memory>
-#include <string>
-#include "HEJ/optional.hh"
#include "HEJ/Analysis.hh"
namespace YAML{
class Node;
}
namespace HEJ{
//! Load an analysis
/**
* @param parameters Analysis parameters
* @returns A pointer to an Analysis instance
*
* If parameters["plugin"] exists, an analysis (deriving from the
* \ref Analysis class) will be loaded from the library parameters["plugin"].
* Otherwise, if parameters["rivet"] exists, the corresponding RivetAnalysis
* will be loaded. If none of these parameters are specified, a pointer to
* the default EmptyAnalysis is returned.
*/
std::unique_ptr<Analysis> get_analysis(YAML::Node const & parameters);
}
diff --git a/include/HEJ/kinematics.hh b/include/HEJ/kinematics.hh
index 01473ac..3a2b909 100644
--- a/include/HEJ/kinematics.hh
+++ b/include/HEJ/kinematics.hh
@@ -1,21 +1,25 @@
/** \file
* \brief Contains function to compute the incoming momentum from outgoing.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <tuple>
#include <vector>
namespace fastjet{
class PseudoJet;
}
namespace HEJ{
class Particle;
/** \brief Compute the incoming momentum from momentum conservation.
*/
std::tuple<fastjet::PseudoJet, fastjet::PseudoJet> incoming_momenta(
std::vector<Particle> const & outgoing /**< Outgoing particles */
);
}
diff --git a/include/HEJ/make_RNG.hh b/include/HEJ/make_RNG.hh
index 227a109..b6ee632 100644
--- a/include/HEJ/make_RNG.hh
+++ b/include/HEJ/make_RNG.hh
@@ -1,28 +1,32 @@
/** \file
* \brief Declares a factory function for random number generators
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <memory>
#include <string>
-#include "HEJ/RNG.hh"
#include "HEJ/optional.hh"
+#include "HEJ/RNG.hh"
namespace HEJ {
//! Factory function for random number generators
/**
* @param name Name of the random number generator
* @param seed Optional seed
* @returns A pointer to an instance of a random number generator
*
* At present, name should be one of "ranlux64" or "mixmax" (case insensitive).
* The interpretation of the seed depends on the random number generator.
* For ranlux64, it is the name of a seed file. For mixmax it should be a
* string convertible to a long integer.
*/
std::unique_ptr<HEJ::RNG> make_RNG(
std::string const & name,
optional<std::string> const & seed
);
}
diff --git a/include/HEJ/make_writer.hh b/include/HEJ/make_writer.hh
index 0c1479b..71a7de5 100644
--- a/include/HEJ/make_writer.hh
+++ b/include/HEJ/make_writer.hh
@@ -1,33 +1,37 @@
/** \file
* \brief Declares a factory function for event writers
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <string>
#include <memory>
+#include <string>
-#include "HEJ/output_formats.hh"
#include "HEJ/EventWriter.hh"
+#include "HEJ/output_formats.hh"
namespace LHEF{
struct HEPRUP;
}
namespace HEJ{
//! Factory function for event writers
/**
* @param format The format of the output file
* @param outfile The name of the output file
* @param heprup General process information
* @returns A pointer to an instance of an EventWriter
* for the desired format
*/
std::unique_ptr<EventWriter> make_format_writer(
FileFormat format,
std::string const & outfile,
LHEF::HEPRUP const & heprup
);
}
diff --git a/include/HEJ/optional.hh b/include/HEJ/optional.hh
index 2f57eab..32be64e 100644
--- a/include/HEJ/optional.hh
+++ b/include/HEJ/optional.hh
@@ -1,24 +1,28 @@
/** \file
* \brief Defines the optional type
*
* The C++14 standard introduces the std::optional type.
* If C++14 is not available, we use the optional type from boost instead.
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#if __cplusplus <= 201402L
#include <boost/optional.hpp>
#else
#include <optional>
#endif
namespace HEJ{
#if __cplusplus <= 201402L
template<typename T>
using optional = boost::optional<T>;
#else
template<typename T>
using optional = std::optional<T>;
#endif
}
diff --git a/include/HEJ/output_formats.hh b/include/HEJ/output_formats.hh
index 09cb884..5ee6e51 100644
--- a/include/HEJ/output_formats.hh
+++ b/include/HEJ/output_formats.hh
@@ -1,34 +1,38 @@
/** \file
* \brief Defines formats for output to event files
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <string>
#include <stdexcept>
+#include <string>
namespace HEJ{
//! Supported event file formats
enum FileFormat{
Les_Houches, /*!< Les Houches Output */
HepMC /*!< HepMC Output */
};
//! Convert a file format to a string
inline std::string to_string(FileFormat f){
switch(f){
case Les_Houches: return "Les Houches";
case HepMC: return "HepMC";
default:
throw std::logic_error("unhandled file format");
}
}
//! Output file specification
struct OutputFile{
std::string name; /**< Output File Name */
FileFormat format; /**< Output File Format */
};
}
diff --git a/include/HEJ/resummation_jet.hh b/include/HEJ/resummation_jet.hh
index 726d70d..409b5a2 100644
--- a/include/HEJ/resummation_jet.hh
+++ b/include/HEJ/resummation_jet.hh
@@ -1,39 +1,43 @@
/** \file
* \brief Functions to calculate the kinematics of resummation jets,
* i.e. resuffling the jet momenta
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
#include <vector>
namespace fastjet{
struct PseudoJet;
}
namespace HEJ{
/**
* \brief Calculate the resummation jet momenta
* @param p_born born Jet Momenta
* @param qperp Sum of non-jet Parton Transverse Momenta
* @returns Resummation Jet Momenta
*/
std::vector<fastjet::PseudoJet> resummation_jet_momenta(
std::vector<fastjet::PseudoJet> const & p_born,
fastjet::PseudoJet const & qperp
);
/**
* \brief Calculate additional weight from changing the jet momenta
* @param p_born born Jet Momenta
* @param qperp Sum of non-jet Parton Transverse Momenta
*
* Computes the Jacobian for changing the original delta functions
* expressed in terms of jet momenta to delta functions of the
* parton momenta in the resummation phase space
*/
double resummation_jet_weight(
std::vector<fastjet::PseudoJet> const & p_born,
fastjet::PseudoJet const & qperp
);
}
diff --git a/include/HEJ/stream.hh b/include/HEJ/stream.hh
index 8f27516..55ab077 100644
--- a/include/HEJ/stream.hh
+++ b/include/HEJ/stream.hh
@@ -1,33 +1,39 @@
/** \file
* \brief Declares input streams
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <memory>
#include <fstream>
+#include <memory>
+#include <string>
+
#include <boost/iostreams/filtering_stream.hpp>
namespace HEJ{
//! Small wrapper around boost's filtering_istream
class istream {
using boost_istream = boost::iostreams::filtering_istream;
public:
//! Constructor
/**
* @param filename Name of input file
*/
explicit istream(std::string const & filename);
//! Conversion to boost_istream
operator boost_istream& () const noexcept {
return *stream_;
}
private:
std::ifstream file_;
std::unique_ptr<boost_istream> stream_;
};
}
diff --git a/include/HEJ/utility.hh b/include/HEJ/utility.hh
index 96a1961..398875d 100644
--- a/include/HEJ/utility.hh
+++ b/include/HEJ/utility.hh
@@ -1,238 +1,114 @@
/**
* \file
* \brief Contains various utilities
+ *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
#pragma once
-#include <algorithm>
-#include <cassert>
+#include <memory>
#include <boost/core/demangle.hpp>
-// FastJet Includes
#include "fastjet/PseudoJet.hh"
-#include "fastjet/ClusterSequence.hh"
-
-#include "HEJ/PDG_codes.hh"
namespace HEJ{
- //! Class representing a particle
- struct Particle {
- //! particle type
- ParticleID type;
- //! particle momentum
- fastjet::PseudoJet p;
-
- //! get rapidity
- double rapidity() const{
- return p.rapidity();
- }
- //! get transverse momentum
- double perp() const{
- return p.perp();
- }
- //! get momentum in x direction
- double px() const{
- return p.px();
- }
- //! get momentum in y direction
- double py() const{
- return p.py();
- }
- //! get momentum in z direction
- double pz() const{
- return p.pz();
- }
- //! get energy
- double E() const{
- return p.E();
- }
- //! get mass
- double m() const{
- return p.m();
- }
- };
-
- //! Functor to compare rapidities
- /**
- * This can be used whenever a rapidity comparison function is needed,
- * for example in many standard library functions.
- *
- * @see pz_less
- */
- struct rapidity_less{
- template<class FourVector>
- bool operator()(FourVector const & p1, FourVector const & p2){
- return p1.rapidity() < p2.rapidity();
- }
- };
-
- //! Functor to compare momenta in z direction
- /**
- * This can be used whenever a pz comparison function is needed,
- * for example in many standard library functions.
- *
- * @see rapidity_less
- */
- struct pz_less{
- template<class FourVector>
- bool operator()(FourVector const & p1, FourVector const & p2){
- return p1.pz() < p2.pz();
- }
- };
-
-
- //! Convert a vector of Particles to a vector of particle momenta
- inline
- std::vector<fastjet::PseudoJet> to_PseudoJet(
- std::vector<Particle> const & v
- ){
- std::vector<fastjet::PseudoJet> result;
- for(auto && sp: v) result.emplace_back(sp.p);
- return result;
- }
-
- //! Check if a particle is a parton, i.e. quark, antiquark, or gluon
- inline
- bool is_parton(Particle const & p){
- return is_parton(p.type);
- }
-
- //! Check if a particle is a quark
- inline
- bool is_quark(Particle const & p){
- return is_quark(p.type);
- }
-
- //! Check if a particle is an anti-quark
- inline
- bool is_antiquark(Particle const & p){
- return is_antiquark(p.type);
- }
-
- //! Check if a particle is a quark or any-quark
- inline
- bool is_anyquark(Particle const & p){
- return is_anyquark(p.type);
- }
-
- //! Check if a particle is a photon, W or Z boson
- inline bool is_AWZ_boson(Particle const & particle){
- return is_AWZ_boson(particle.type);
- }
-
- //! Check if a particle is a photon, W, Z, or Higgs boson
- inline bool is_AWZH_boson(Particle const & particle){
- return is_AWZH_boson(particle.type);
- }
-
- //! Extract all partons from a vector of particles
- inline
- std::vector<Particle> filter_partons(
- std::vector<Particle> const & v
- ){
- std::vector<Particle> result;
- result.reserve(v.size());
- std::copy_if(
- begin(v), end(v), std::back_inserter(result),
- [](Particle const & p){ return is_parton(p); }
- );
- return result;
- }
//! Create a std::unique_ptr to a T object
/**
* For non-array types this works like std::make_unique,
* which is not available under C++11
*/
template<class T, class... Args>
std::unique_ptr<T> make_unique(Args&&... a){
return std::unique_ptr<T>{new T{std::forward<Args>(a)...}};
}
//! Create an array containing the passed arguments
template<typename T, typename... U>
constexpr
std::array<T, 1 + sizeof...(U)> make_array(T t, U&&... rest){
return {{t, std::forward<U>(rest)...}};
}
inline
std::string join(
std::string const & /* delim */
){
return "";
}
inline
std::string join(
std::string const & /* delim */, std::string const & str
){
return str;
}
//! Join strings with a delimiter
/**
* @param delim Delimiter to be put between consecutive strings
* @param first First string
* @param second Second string
* @param rest Remaining strings
*/
template<typename... Strings>
std::string join(
std::string const & delim,
std::string const & first, std::string const & second,
Strings&&... rest
){
return join(delim, first + delim + second, std::forward<Strings>(rest)...);
}
//! Return the name of the argument's type
template<typename T>
std::string type_string(T&&){
return boost::core::demangle(typeid(T).name());
}
//! Eliminate compiler warnings for unused variables
template<typename... T>
constexpr void ignore(T&&...) {}
//! Check whether two doubles are closer than ep > 0 to each other
inline
bool nearby_ep(double a, double b, double ep){
assert(ep > 0);
return std::abs(a-b) < ep;
}
//! Check whether all components of two PseudoJets are closer than ep to each other
inline
bool nearby_ep(
fastjet::PseudoJet const & pa, fastjet::PseudoJet const & pb,
double ep
){
assert(ep > 0);
for(size_t i = 0; i < 4; ++i){
if(!nearby_ep(pa[i], pb[i], ep)) return false;
}
return true;
}
inline
bool nearby(
fastjet::PseudoJet const & pa, fastjet::PseudoJet const & pb, double const norm = 1.
){
return nearby_ep(pa, pb, 1e-7*norm);
}
//! Check whether two rapidities are close
inline
bool nearby_rap(
double rapa, double rapb, double rap
){
assert(rap > 0);
if(!nearby_ep(rapa, rapb, rap)) return false;
return true;
}
}
diff --git a/src/CMakeLists.txt b/src/CMakeLists.txt
index bc6180c..1e54b15 100644
--- a/src/CMakeLists.txt
+++ b/src/CMakeLists.txt
@@ -1,18 +1,19 @@
file(GLOB src_files *.cc)
add_library(hejlib SHARED ${src_files})
set_target_properties(hejlib PROPERTIES OUTPUT_NAME "HEJ")
-set(libraries ${CMAKE_DL_LIBS} ${LHAPDF_LIBRARIES} ${CLHEP_LIBRARIES} ${FASTJET_LIBRARIES} ${Boost_LIBRARIES} ${YAML_CPP_LIBRARIES} yaml-cpp)
+set(libraries ${CMAKE_DL_LIBS} ${LHAPDF_LIBRARIES} ${CLHEP_LIBRARIES}
+ ${FASTJET_LIBRARIES} ${Boost_LIBRARIES} ${YAML_CPP_LIBRARIES} yaml-cpp)
if(${QCDloop_FOUND})
list(APPEND libraries ${QCDloop_LIBRARIES} quadmath)
endif()
if(${HepMC_FOUND})
list(APPEND libraries ${HepMC_LIBRARIES})
if(${rivet_FOUND})
list(APPEND libraries ${rivet_LIBRARIES})
endif()
endif()
target_link_libraries(hejlib ${libraries})
install(TARGETS hejlib DESTINATION ${INSTALL_LIB_DIR})
diff --git a/src/CombinedEventWriter.cc b/src/CombinedEventWriter.cc
index fe79ac5..6ea7623 100644
--- a/src/CombinedEventWriter.cc
+++ b/src/CombinedEventWriter.cc
@@ -1,21 +1,28 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/CombinedEventWriter.hh"
+#include "HEJ/make_writer.hh"
+
namespace HEJ{
CombinedEventWriter::CombinedEventWriter(
std::vector<OutputFile> const & outfiles,
LHEF::HEPRUP const & heprup
){
writers_.reserve(outfiles.size());
for(OutputFile const & outfile: outfiles){
writers_.emplace_back(
make_format_writer(outfile.format, outfile.name, heprup)
);
}
}
void CombinedEventWriter::write(Event const & ev){
for(auto & writer: writers_) writer->write(ev);
}
}
diff --git a/src/EmptyAnalysis.cc b/src/EmptyAnalysis.cc
index aadd820..bed8f77 100644
--- a/src/EmptyAnalysis.cc
+++ b/src/EmptyAnalysis.cc
@@ -1,62 +1,68 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/EmptyAnalysis.hh"
-#include "HEJ/exceptions.hh"
-#include <iostream>
#include <string>
#include <vector>
+
#include "yaml-cpp/yaml.h"
+#include "HEJ/exceptions.hh"
+
namespace HEJ{
namespace{
std::vector<std::string> param_as_strings(YAML::Node const & parameters){
using YAML::NodeType;
switch(parameters.Type()){
case NodeType::Null:
case NodeType::Undefined:
return {};
case NodeType::Scalar:
return {parameters.as<std::string>()};
case NodeType::Sequence: {
std::vector<std::string> param_strings;
for(auto && param: parameters){
param_strings.emplace_back(param.as<std::string>());
}
return param_strings;
}
case NodeType::Map: {
std::vector<std::string> param_strings;
for(auto && param: parameters){
param_strings.emplace_back(param.first.as<std::string>());
}
return param_strings;
}
default:;
}
throw std::logic_error{"unreachable"};
}
}
std::unique_ptr<Analysis> EmptyAnalysis::create(
YAML::Node const & parameters
){
const auto param_strings = param_as_strings(parameters);
if(! param_strings.empty()){
std::string error{"Unknown analysis parameter(s):"};
for(auto && p: param_strings) error += " " + p;
throw unknown_option{error};
}
return std::unique_ptr<Analysis>{new EmptyAnalysis{}};
}
void EmptyAnalysis::fill(Event const &, Event const &){
// do nothing
}
bool EmptyAnalysis::pass_cuts(Event const &, Event const &){
return true;
}
void EmptyAnalysis::finalise(){
// do nothing
}
}
diff --git a/src/Event.cc b/src/Event.cc
index 21744ed..6f04831 100644
--- a/src/Event.cc
+++ b/src/Event.cc
@@ -1,649 +1,692 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/Event.hh"
-#include "HEJ/utility.hh"
+#include <algorithm>
+#include <assert.h>
+#include <numeric>
+#include <utility>
+
+#include "LHEF/LHEF.h"
+
+#include "fastjet/JetDefinition.hh"
+
+#include "HEJ/exceptions.hh"
+#include "HEJ/PDG_codes.hh"
namespace HEJ{
namespace{
constexpr int status_in = -1;
constexpr int status_decayed = 2;
constexpr int status_out = 1;
/// @name helper functions to determine event type
//@{
/**
* \brief check if final state valid for HEJ
*
* check if there is at most one photon, W, H, Z in the final state
* and all the rest are quarks or gluons
*/
bool final_state_ok(std::vector<Particle> const & outgoing){
bool has_AWZH_boson = false;
for(auto const & out: outgoing){
if(is_AWZH_boson(out.type)){
if(has_AWZH_boson) return false;
has_AWZH_boson = true;
}
else if(! is_parton(out.type)) return false;
}
return true;
}
template<class Iterator>
Iterator remove_AWZH(Iterator begin, Iterator end){
return std::remove_if(
begin, end, [](Particle const & p){return is_AWZH_boson(p);}
);
}
template<class Iterator>
bool valid_outgoing(Iterator begin, Iterator end){
return std::distance(begin, end) >= 2
&& std::is_sorted(begin, end, rapidity_less{})
&& std::count_if(
begin, end, [](Particle const & s){return is_AWZH_boson(s);}
) < 2;
}
/**
* \brief function which determines if type change is consistent with W emission.
* @param in incoming Particle
* @param out outgoing Particle
*
* Ensures that change type of quark line is possible by a flavour changing
* W emission.
*/
bool is_W_Current(ParticleID in, ParticleID out){
if((in==1 && out==2)||(in==2 && out==1)){
return true;
}
else if((in==-1 && out==-2)||(in==-2 && out==-1)){
return true;
}
else if((in==3 && out==4)||(in==4 && out==3)){
return true;
}
else if((in==-3 && out==-4)||(in==-4 && out==-3)){
return true;
}
else{
return false;
}
}
/**
* \brief checks if particle type remains same from incoming to outgoing
* @param in incoming Particle
* @param out outgoing Particle
*/
bool is_Pure_Current(ParticleID in, ParticleID out){
if(abs(in)<=6 || in==21) return (in==out);
else return false;
}
// @note that this changes the outgoing range!
template<class ConstIterator, class Iterator>
bool is_FKL(
ConstIterator begin_incoming, ConstIterator end_incoming,
Iterator begin_outgoing, Iterator end_outgoing
){
assert(std::distance(begin_incoming, end_incoming) == 2);
assert(std::distance(begin_outgoing, end_outgoing) >= 2);
// One photon, W, H, Z in the final state is allowed.
// Remove it for remaining tests,
end_outgoing = remove_AWZH(begin_outgoing, end_outgoing);
if(std::all_of(
begin_outgoing + 1, end_outgoing - 1,
[](Particle const & p){ return p.type == pid::gluon; })
){
// Test if this is a standard FKL configuration.
if (is_Pure_Current(begin_incoming->type, begin_outgoing->type)
&& is_Pure_Current((end_incoming-1)->type, (end_outgoing-1)->type)){
return true;
}
}
return false;
}
template<class ConstIterator, class Iterator>
bool is_W_FKL(
ConstIterator begin_incoming, ConstIterator end_incoming,
Iterator begin_outgoing, Iterator end_outgoing
){
assert(std::distance(begin_incoming, end_incoming) == 2);
assert(std::distance(begin_outgoing, end_outgoing) >= 2);
// One photon, W, H, Z in the final state is allowed.
// Remove it for remaining tests,
end_outgoing = remove_AWZH(begin_outgoing, end_outgoing);
if(std::all_of(
begin_outgoing + 1, end_outgoing - 1,
[](Particle const & p){ return p.type == pid::gluon; })
){
// Test if this is a standard FKL configuration.
if(is_W_Current(begin_incoming->type, begin_outgoing->type)
&& is_Pure_Current((end_incoming-1)->type, (end_outgoing-1)->type)){
return true;
}
else if(is_Pure_Current(begin_incoming->type, begin_outgoing->type)
&& is_W_Current((end_incoming-1)->type, (end_outgoing-1)->type)){
return true;
}
}
return false;
}
bool is_FKL(
std::array<Particle, 2> const & incoming,
std::vector<Particle> outgoing
){
assert(std::is_sorted(begin(incoming), end(incoming), pz_less{}));
assert(valid_outgoing(begin(outgoing), end(outgoing)));
const auto WEmit = std::find_if(
begin(outgoing), end(outgoing),
[](Particle const & s){ return abs(s.type) == pid::Wp; }
);
if (abs(WEmit->type) == pid::Wp){
return is_W_FKL(
begin(incoming), end(incoming),
begin(outgoing), end(outgoing)
);
}
else{
return is_FKL(
begin(incoming), end(incoming),
begin(outgoing), end(outgoing)
);
}
}
bool has_2_jets(Event const & event){
return event.jets().size() >= 2;
}
/**
* \brief Checks whether event is unordered backwards
* @param ev Event
* @returns Is Event Unordered Backwards
*
* - Checks there is more than 3 constuents in the final state
* - Checks there is more than 3 jets
* - Checks the most backwards parton is a gluon
* - Checks the most forwards jet is not a gluon
* - Checks the rest of the event is FKL
* - Checks the second most backwards is not a different boson
* - Checks the unordered gluon actually forms a jet
*/
bool is_unordered_backward(Event const & ev){
auto const & in = ev.incoming();
auto const & out = ev.outgoing();
assert(std::is_sorted(begin(in), end(in), pz_less{}));
assert(valid_outgoing(begin(out), end(out)));
if(out.size() < 3) return false;
if(ev.jets().size() < 3) return false;
if(in.front().type == pid::gluon) return false;
if(out.front().type != pid::gluon) return false;
// When skipping the unordered emission
// the remainder should be a regular FKL event,
// except that the (new) first outgoing particle must not be a A,W,Z,H.
const auto FKL_begin = next(begin(out));
if(is_AWZH_boson(*FKL_begin)) return false;
if(!is_FKL(in, {FKL_begin, end(out)})) return false;
// check that the unordered gluon forms an extra jet
const auto jets = sorted_by_rapidity(ev.jets());
const auto indices = ev.particle_jet_indices({jets.front()});
return indices[0] >= 0 && indices[1] == -1;
}
/**
* \brief Checks for a forward unordered gluon emission
* @param ev Event
* @returns Is the event a forward unordered emission
*
* \see is_unordered_backward
*/
bool is_unordered_forward(Event const & ev){
auto const & in = ev.incoming();
auto const & out = ev.outgoing();
assert(std::is_sorted(begin(in), end(in), pz_less{}));
assert(valid_outgoing(begin(out), end(out)));
if(out.size() < 3) return false;
if(ev.jets().size() < 3) return false;
if(in.back().type == pid::gluon) return false;
if(out.back().type != pid::gluon) return false;
// When skipping the unordered emission
// the remainder should be a regular FKL event,
// except that the (new) last outgoing particle must not be a A,W,Z,H.
const auto FKL_end = prev(end(out));
if(is_AWZH_boson(*prev(FKL_end))) return false;
if(!is_FKL(in, {begin(out), FKL_end})) return false;
// check that the unordered gluon forms an extra jet
const auto jets = sorted_by_rapidity(ev.jets());
const auto indices = ev.particle_jet_indices({jets.back()});
return indices.back() >= 0 && indices[indices.size()-2] == -1;
}
/**
* \brief Checks for a forward extremal qqx
* @param ev Event
* @returns Is the event a forward extremal qqx event
*
* Checks there is 3 or more than 3 constituents in the final state
* Checks there is 3 or more than 3 jets
* Checks most forwards incoming is gluon
* Checks most extremal particle is not a Higgs (either direction)
* Checks the second most forwards particle is not Higgs boson
* Checks the most forwards parton is a either quark or anti-quark.
* Checks the second most forwards parton is anti-quark or quark.
* Checks the qqbar pair form 2 separate jets.
*/
bool is_Ex_qqxf(Event const & ev){
auto const & in = ev.incoming();
auto const & out = ev.outgoing();
assert(std::is_sorted(begin(in), end(in), pz_less{}));
assert(valid_outgoing(begin(out), end(out)));
int fkl_end=2;
if(out.size() < 3) return false;
if(ev.jets().size() < 3) return false;
if(in.back().type != pid::gluon) return false;
if(out.back().type == pid::Higgs || out.front().type == pid::Higgs
|| out.rbegin()[1].type == pid::Higgs) return false;
// if extremal AWZ
if(is_AWZ_boson(out.back())){ // if extremal AWZ
fkl_end++;
if (is_quark(out.rbegin()[1])){ //if second quark
if (!(is_antiquark(out.rbegin()[2]))) return false;// third must be anti-quark
}
else if (is_antiquark(out.rbegin()[1])){ //if second anti-quark
if (!(is_quark(out.rbegin()[2]))) return false;// third must be quark
}
else return false;
}
else if (is_quark(out.rbegin()[0])){ //if extremal quark
if(is_AWZ_boson(out.rbegin()[1])){ // if second AWZ
fkl_end++;
if (!(is_antiquark(out.rbegin()[2]))) return false;// third must be anti-quark
}
else if (!(is_antiquark(out.rbegin()[1]))) return false;// second must be anti-quark
}
else if (is_antiquark(out.rbegin()[0])){ //if extremal anti-quark
if(is_AWZ_boson(out.rbegin()[1])){ // if second AWZ
fkl_end++;
if (!(is_quark(out.rbegin()[2]))) return false;// third must be quark
}
else if (!(is_quark(out.rbegin()[1]))) return false;// second must be quark
}
else return false;
// When skipping the qqbar
// New last outgoing particle must not be a Higgs
if (out.rbegin()[fkl_end].type == pid::Higgs) return false;
const auto jets = fastjet::sorted_by_rapidity(ev.jets());
const auto indices = ev.particle_jet_indices({jets});
// Ensure qqbar pair are in separate jets
if(indices[indices.size()-2] != indices[indices.size()-1]-1) return false;
// Opposite current should be logical to process
if (is_AWZ_boson(out.front().type)){
return (is_Pure_Current(in.front().type, out[1].type)
|| is_W_Current(in.front().type,out[1].type));
}
else
return (is_Pure_Current(in.front().type, out[0].type)
|| is_W_Current(in.front().type,out[0].type));
}
/**
* \brief Checks for a backward extremal qqx
* @param ev Event
* @returns Is the event a backward extremal qqx event
*
* Checks there is 3 or more than 3 constituents in the final state
* Checks there is 3 or more than 3 jets
* Checks most backwards incoming is gluon
* Checks most extremal particle is not a Higgs (either direction) y
* Checks the second most backwards particle is not Higgs boson y
* Checks the most backwards parton is a either quark or anti-quark. y
* Checks the second most backwards parton is anti-quark or quark. y
* Checks the qqbar pair form 2 separate jets.
*/
bool is_Ex_qqxb(Event const & ev){
auto const & in = ev.incoming();
auto const & out = ev.outgoing();
assert(std::is_sorted(begin(in), end(in), pz_less{}));
assert(valid_outgoing(begin(out), end(out)));
int fkl_start=2;
if(out.size() < 3) return false;
if(ev.jets().size() < 3) return false;
if(in.front().type != pid::gluon) return false;
if(out.back().type == pid::Higgs || out.front().type == pid::Higgs
|| out[1].type == pid::Higgs) return false;
if(is_AWZ_boson(out.front())){ // if extremal AWZ
fkl_start++;
if (is_quark(out[1])){ //if second quark
if (!(is_antiquark(out[2]))) return false;// third must be anti-quark
}
else if (is_antiquark(out[1])){ //if second anti-quark
if (!(is_quark(out[2]))) return false;// third must be quark
}
else return false;
}
else if (is_quark(out[0])){ // if extremal quark
if(is_AWZ_boson(out[1])){ // if second AWZ
fkl_start++;
if (!(is_antiquark(out[2]))) return false;// third must be anti-quark
}
else if (!(is_antiquark(out[1]))) return false;// second must be anti-quark
}
else if (is_antiquark(out[0])){ //if extremal anti-quark
if(is_AWZ_boson(out[1])){ // if second AWZ
fkl_start++;
if (!(is_quark(out[2]))) return false;// third must be quark
}
else if (!(is_quark(out[1]))) return false;// second must be quark
}
else return false;
// When skipping the qqbar
// New last outgoing particle must not be a Higgs.
if (out[fkl_start].type == pid::Higgs) return false;
const auto jets = fastjet::sorted_by_rapidity(ev.jets());
const auto indices = ev.particle_jet_indices({jets});
// Ensure qqbar pair form separate jets.
if(indices[0] != indices[1]-1) return false;
// Other current should be logical to process
if (is_AWZ_boson(out.back())){
return (is_Pure_Current(in.back().type, out.rbegin()[1].type)
|| is_W_Current(in.back().type,out.rbegin()[1].type));
}
else
return (is_Pure_Current(in.back().type, out.rbegin()[0].type)
|| is_W_Current(in.back().type, out.rbegin()[0].type));
}
/**
* \brief Checks for a central qqx
* @param ev Event
* @returns Is the event a central extremal qqx event
*
* Checks there is 4 or more than 4 constuents in the final state
* Checks there is 4 or more than 4 jets
* Checks most extremal particle is not a Higgs (either direction) y
* Checks for a central quark in the outgoing states
* Checks for adjacent anti-quark parton. (allowing for AWZ boson emission between)
* Checks external currents are logically sound.
*/
bool is_Mid_qqx(Event const & ev){
auto const & in = ev.incoming();
auto const & out = ev.outgoing();
assert(std::is_sorted(begin(in), end(in), pz_less{}));
assert(valid_outgoing(begin(out), end(out)));
if(out.size() < 4) return false;
if(ev.jets().size() < 4) return false;
if(out.back().type == pid::Higgs || out.front().type == pid::Higgs)
return false;
size_t start_FKL=0;
size_t end_FKL=0;
if (is_AWZ_boson(out.back())){
end_FKL++;
}
if (is_AWZ_boson(out.front())){
start_FKL++;
}
if ((is_Pure_Current(in.back().type,out.rbegin()[end_FKL].type)
&& is_Pure_Current(in.front().type,out[start_FKL].type))){
//nothing to do
}
else if (is_W_Current(in.back().type,out.rbegin()[end_FKL].type)
&& is_Pure_Current(in.front().type,out[start_FKL].type)){
//nothing to do
}
else if (!(is_Pure_Current(in.back().type,out.rbegin()[end_FKL].type)
&& is_W_Current(in.front().type,out[start_FKL].type))){
return false;
}
const auto jets = fastjet::sorted_by_rapidity(ev.jets());
const auto indices = ev.particle_jet_indices({jets});
auto const out_partons = filter_partons(out);
for (size_t i = 1; i<out_partons.size()-2; i++){
if ((is_quark(out_partons[i]) && (is_antiquark(out_partons[i+1])))
|| (is_antiquark(out_partons[i]) && (is_quark(out_partons[i+1])))){
return (indices[i+1] == indices[i]+1 && indices[i] != -1);
}
}
return false;
}
using event_type::EventType;
EventType classify(Event const & ev){
if(! final_state_ok(ev.outgoing()))
return EventType::bad_final_state;
if(! has_2_jets(ev))
return EventType::no_2_jets;
if(is_FKL(ev.incoming(), ev.outgoing()))
return EventType::FKL;
if(is_unordered_backward(ev))
return EventType::unordered_backward;
if(is_unordered_forward(ev))
return EventType::unordered_forward;
if(is_Ex_qqxb(ev))
return EventType::extremal_qqxb;
if(is_Ex_qqxf(ev))
return EventType::extremal_qqxf;
if(is_Mid_qqx(ev))
return EventType::central_qqx;
return EventType::nonHEJ;
}
//@}
Particle extract_particle(LHEF::HEPEUP const & hepeup, int i){
return Particle{
static_cast<ParticleID>(hepeup.IDUP[i]),
fastjet::PseudoJet{
hepeup.PUP[i][0], hepeup.PUP[i][1],
hepeup.PUP[i][2], hepeup.PUP[i][3]
}
};
}
bool is_decay_product(std::pair<int, int> const & mothers){
if(mothers.first == 0) return false;
return mothers.second == 0 || mothers.first == mothers.second;
}
} // namespace anonymous
UnclusteredEvent::UnclusteredEvent(LHEF::HEPEUP const & hepeup):
central(EventParameters{
hepeup.scales.mur, hepeup.scales.muf, hepeup.weight()
})
{
size_t in_idx = 0;
for (int i = 0; i < hepeup.NUP; ++i) {
// skip decay products
// we will add them later on, but we have to ensure that
// the decayed particle is added before
if(is_decay_product(hepeup.MOTHUP[i])) continue;
auto particle = extract_particle(hepeup, i);
// needed to identify mother particles for decay products
particle.p.set_user_index(i+1);
if(hepeup.ISTUP[i] == status_in){
if(in_idx > incoming.size()) {
throw std::invalid_argument{
"Event has too many incoming particles"
};
}
incoming[in_idx++] = std::move(particle);
}
else outgoing.emplace_back(std::move(particle));
}
- std::sort(
- begin(incoming), end(incoming),
- [](Particle o1, Particle o2){return o1.p.pz()<o2.p.pz();}
- );
- std::sort(begin(outgoing), end(outgoing), rapidity_less{});
// add decay products
for (int i = 0; i < hepeup.NUP; ++i) {
if(!is_decay_product(hepeup.MOTHUP[i])) continue;
const int mother_id = hepeup.MOTHUP[i].first;
const auto mother = std::find_if(
begin(outgoing), end(outgoing),
[mother_id](Particle const & particle){
return particle.p.user_index() == mother_id;
}
);
if(mother == end(outgoing)){
throw std::invalid_argument{"invalid decay product parent"};
}
const int mother_idx = std::distance(begin(outgoing), mother);
assert(mother_idx >= 0);
decays[mother_idx].emplace_back(extract_particle(hepeup, i));
}
}
Event::Event(
UnclusteredEvent ev,
fastjet::JetDefinition const & jet_def, double min_jet_pt
):
ev_{std::move(ev)},
cs_{to_PseudoJet(filter_partons(ev_.outgoing)), jet_def},
min_jet_pt_{min_jet_pt}
{
+ // sort particles
+ std::sort(
+ begin(ev_.incoming), end(ev_.incoming),
+ [](Particle o1, Particle o2){return o1.p.pz()<o2.p.pz();}
+ );
+
+ auto old_outgoing = std::move(ev_.outgoing);
+ std::vector<size_t> idx(old_outgoing.size());
+ std::iota(idx.begin(), idx.end(), 0);
+ std::sort(idx.begin(), idx.end(), [&old_outgoing](size_t i, size_t j){
+ return old_outgoing[i].rapidity() < old_outgoing[j].rapidity();
+ });
+ ev_.outgoing.clear();
+ ev_.outgoing.reserve(old_outgoing.size());
+ for(size_t i: idx) {
+ ev_.outgoing.emplace_back(std::move(old_outgoing[i]));
+ }
+
+ // find decays again
+ if(!ev_.decays.empty()){
+ auto old_decays = std::move(ev_.decays);
+ ev_.decays.clear();
+ for(size_t i=0; i<idx.size(); ++i) {
+ auto decay = old_decays.find(idx[i]);
+ if(decay != old_decays.end())
+ ev_.decays.emplace(i, std::move(decay->second));
+ }
+ assert(old_decays.size() == ev_.decays.size());
+ }
+
+ // classify event
type_ = classify(*this);
+
+ assert(std::is_sorted(begin(outgoing()), end(outgoing()), rapidity_less{}));
}
std::vector<fastjet::PseudoJet> Event::jets() const{
return cs_.inclusive_jets(min_jet_pt_);
}
/**
* \brief Returns the invarient mass of the event
* @param ev Event
* @returns s hat
*
* Makes use of the FastJet PseudoJet function m2().
* Applies this function to the sum of the incoming partons.
*/
double shat(Event const & ev){
return (ev.incoming()[0].p + ev.incoming()[1].p).m2();
}
namespace{
// colour flow according to Les Houches standard
// TODO: stub
std::vector<std::pair<int, int>> colour_flow(
std::array<Particle, 2> const & incoming,
std::vector<Particle> const & outgoing
){
std::vector<std::pair<int, int>> result(
incoming.size() + outgoing.size()
);
for(auto & col: result){
col = std::make_pair(-1, -1);
}
return result;
}
}
LHEF::HEPEUP to_HEPEUP(Event const & event, LHEF::HEPRUP * heprup){
LHEF::HEPEUP result;
result.heprup = heprup;
result.weights = {{event.central().weight, nullptr}};
for(auto const & var: event.variations()){
result.weights.emplace_back(var.weight, nullptr);
}
size_t num_particles = event.incoming().size() + event.outgoing().size();
for(auto const & decay: event.decays()) num_particles += decay.second.size();
result.NUP = num_particles;
// the following entries are pretty much meaningless
result.IDPRUP = event.type()+1; // event ID
result.AQEDUP = 1./128.; // alpha_EW
//result.AQCDUP = 0.118 // alpha_QCD
// end meaningless part
result.XWGTUP = event.central().weight;
result.SCALUP = event.central().muf;
result.scales.muf = event.central().muf;
result.scales.mur = event.central().mur;
result.scales.SCALUP = event.central().muf;
result.pdfinfo.p1 = event.incoming().front().type;
result.pdfinfo.p2 = event.incoming().back().type;
result.pdfinfo.scale = event.central().muf;
for(Particle const & in: event.incoming()){
result.IDUP.emplace_back(in.type);
result.ISTUP.emplace_back(status_in);
result.PUP.push_back({in.p[0], in.p[1], in.p[2], in.p[3], in.p.m()});
result.MOTHUP.emplace_back(0, 0);
}
for(size_t i = 0; i < event.outgoing().size(); ++i){
Particle const & out = event.outgoing()[i];
result.IDUP.emplace_back(out.type);
const int status = event.decays().count(i)?status_decayed:status_out;
result.ISTUP.emplace_back(status);
result.PUP.push_back({out.p[0], out.p[1], out.p[2], out.p[3], out.p.m()});
result.MOTHUP.emplace_back(1, 2);
}
result.ICOLUP = colour_flow(
event.incoming(), filter_partons(event.outgoing())
);
if(result.ICOLUP.size() < num_particles){
const size_t AWZH_boson_idx = std::find_if(
begin(event.outgoing()), end(event.outgoing()),
[](Particle const & s){ return is_AWZH_boson(s); }
) - begin(event.outgoing()) + event.incoming().size();
assert(AWZH_boson_idx <= result.ICOLUP.size());
result.ICOLUP.insert(
begin(result.ICOLUP) + AWZH_boson_idx,
std::make_pair(0,0)
);
}
for(auto const & decay: event.decays()){
for(auto const out: decay.second){
result.IDUP.emplace_back(out.type);
result.ISTUP.emplace_back(status_out);
result.PUP.push_back({out.p[0], out.p[1], out.p[2], out.p[3], out.p.m()});
const size_t mother_idx = 1 + event.incoming().size() + decay.first;
result.MOTHUP.emplace_back(mother_idx, mother_idx);
result.ICOLUP.emplace_back(0,0);
}
}
assert(result.ICOLUP.size() == num_particles);
static constexpr double unknown_spin = 9.; //per Les Houches accord
result.VTIMUP = std::vector<double>(num_particles, unknown_spin);
result.SPINUP = result.VTIMUP;
return result;
}
}
diff --git a/src/EventReweighter.cc b/src/EventReweighter.cc
index 9c58543..28cebd9 100644
--- a/src/EventReweighter.cc
+++ b/src/EventReweighter.cc
@@ -1,317 +1,333 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/EventReweighter.hh"
+#include <algorithm>
+#include <assert.h>
+#include <limits>
+#include <math.h>
+#include <stddef.h>
#include <string>
#include <unordered_map>
+#include "fastjet/ClusterSequence.hh"
+
+#include "LHEF/LHEF.h"
+
+#include "HEJ/Event.hh"
#include "HEJ/exceptions.hh"
-#include "HEJ/PhaseSpacePoint.hh"
+#include "HEJ/Particle.hh"
#include "HEJ/PDG_codes.hh"
-#include "HEJ/utility.hh"
+#include "HEJ/PhaseSpacePoint.hh"
+#include "HEJ/Weights.hh"
namespace HEJ{
using EventType = event_type::EventType;
namespace {
static_assert(
std::numeric_limits<double>::has_quiet_NaN,
"no quiet NaN for double"
);
constexpr double NaN = std::numeric_limits<double>::quiet_NaN();
UnclusteredEvent to_UnclusteredEvent(PhaseSpacePoint const & psp){
UnclusteredEvent result;
result.incoming = psp.incoming();
std::sort(
begin(result.incoming), end(result.incoming),
[](Particle o1, Particle o2){return o1.p.pz()<o2.p.pz();}
);
assert(result.incoming.size() == 2);
result.outgoing = psp.outgoing();
assert(
std::is_sorted(
begin(result.outgoing), end(result.outgoing),
rapidity_less{}
)
);
assert(result.outgoing.size() >= 2);
result.decays = psp.decays();
result.central.mur = NaN;
result.central.muf = NaN;
result.central.weight = psp.weight();
return result;
}
} // namespace anonymous
EventReweighter::EventReweighter(
LHEF::HEPRUP const & heprup,
ScaleGenerator scale_gen,
EventReweighterConfig conf,
HEJ::RNG & ran
):
EventReweighter{
HEJ::Beam{
heprup.EBMUP.first,
{{
static_cast<HEJ::ParticleID>(heprup.IDBMUP.first),
static_cast<HEJ::ParticleID>(heprup.IDBMUP.second)
}}
},
heprup.PDFSUP.first,
std::move(scale_gen),
std::move(conf),
ran
}
{
if(heprup.EBMUP.second != E_beam_){
throw std::invalid_argument(
"asymmetric beam: " + std::to_string(E_beam_)
+ " ---> <--- " + std::to_string(heprup.EBMUP.second)
);
};
if(heprup.PDFSUP.second != pdf_.id()){
throw std::invalid_argument(
"conflicting PDF ids: " + std::to_string(pdf_.id())
+ " vs. " + std::to_string(heprup.PDFSUP.second)
);
}
}
EventReweighter::EventReweighter(
Beam beam,
int pdf_id,
ScaleGenerator scale_gen,
EventReweighterConfig conf,
HEJ::RNG & ran
):
param_{std::move(conf)},
E_beam_{beam.E},
pdf_{pdf_id, beam.type.front(), beam.type.back()},
MEt2_{
[this](double mu){ return pdf_.Halphas(mu); },
param_.ME_config
},
scale_gen_(std::move(scale_gen)),
ran_{ran}
{}
PDF const & EventReweighter::pdf() const{
return pdf_;
}
std::vector<Event> EventReweighter::reweight(
Event const & input_ev, int num_events
){
auto res_events = gen_res_events(input_ev, num_events);
if(res_events.empty()) return {};
for(auto & event: res_events) event = scale_gen_(event);
return rescale(input_ev, std::move(res_events));
}
/**
* \brief main generation/reweighting function:
* generate phase space points and divide out Born factors
*/
std::vector<Event> EventReweighter::gen_res_events(
Event const & ev,
int phase_space_points
){
assert(ev.variations().empty());
switch(param_.treat.at(ev.type())){
case EventTreatment::discard: return {};
case EventTreatment::keep:
if(! jets_pass_resummation_cuts(ev)) return {};
else return {ev};
default:;
}
const double Born_shat = shat(ev);
std::vector<Event> resummation_events;
for(int psp_number = 0; psp_number < phase_space_points; ++psp_number){
PhaseSpacePoint psp{ev, param_.psp_config, ran_};
if(psp.weight() == 0.) continue;
if(psp.incoming()[0].E() > E_beam_ || psp.incoming()[1].E() > E_beam_) continue;
resummation_events.emplace_back(
to_UnclusteredEvent(std::move(psp)),
param_.jet_param.def, param_.jet_param.min_pt
);
auto & new_event = resummation_events.back();
assert(new_event.variations().empty());
new_event.central().mur = ev.central().mur;
new_event.central().muf = ev.central().muf;
const double resum_shat = shat(new_event);
new_event.central().weight *= ev.central().weight*Born_shat*Born_shat/
(phase_space_points*resum_shat*resum_shat);
}
return resummation_events;
}
std::vector<Event> EventReweighter::rescale(
Event const & Born_ev,
std::vector<Event> events
) const{
const double Born_pdf = pdf_factors(Born_ev).central;
const double Born_ME = tree_matrix_element(Born_ev);
for(auto & cur_event: events){
const auto pdf = pdf_factors(cur_event);
assert(pdf.variations.size() == cur_event.variations().size());
const auto ME = matrix_elements(cur_event);
assert(ME.variations.size() == cur_event.variations().size());
cur_event.central().weight *= pdf.central*ME.central/(Born_pdf*Born_ME);
for(size_t i = 0; i < cur_event.variations().size(); ++i){
cur_event.variations(i).weight *=
pdf.variations[i]*ME.variations[i]/(Born_pdf*Born_ME);
}
}
return events;
};
/**
* \brief Do the Jets pass the resummation Cuts?
*
* @param ev Event in Question
* @returns 0 or 1 depending on if ev passes Jet Cuts
*/
bool EventReweighter::jets_pass_resummation_cuts(
Event const & ev
) const{
const auto out_as_PseudoJet = to_PseudoJet(filter_partons(ev.outgoing()));
fastjet::ClusterSequence cs{out_as_PseudoJet, param_.jet_param.def};
return cs.inclusive_jets(param_.jet_param.min_pt).size() == ev.jets().size();
}
/**
* \brief pdf_factors Function
*
* @param ev Event in Question
* @returns Event weights due to PDFs
*
* Calculates the Central value and the variation due
* to the PDF choice made.
*/
Weights
EventReweighter::pdf_factors(Event const & ev) const{
auto const & a = ev.incoming().front();
auto const & b = ev.incoming().back();
const double xa = a.p.e()/E_beam_;
const double xb = b.p.e()/E_beam_;
Weights result;
std::unordered_map<double, double> known_pdf;
result.central =
pdf_.pdfpt(0,xa,ev.central().muf,a.type)*
pdf_.pdfpt(1,xb,ev.central().muf,b.type);
known_pdf.emplace(ev.central().muf, result.central);
result.variations.reserve(ev.variations().size());
for(auto const & ev_param: ev.variations()){
const double muf = ev_param.muf;
auto cur_pdf = known_pdf.find(muf);
if(cur_pdf == known_pdf.end()){
cur_pdf = known_pdf.emplace(
muf,
pdf_.pdfpt(0,xa,muf,a.type)*pdf_.pdfpt(1,xb,muf,b.type)
).first;
}
result.variations.emplace_back(cur_pdf->second);
}
assert(result.variations.size() == ev.variations().size());
return result;
}
/**
* \brief matrix_elements Function
*
* @param ev Event in question
* @returns Event Weights due to MatrixElements
*
* Calculates the Central value and the variation due
* to the Matrix Element.
*/
Weights
EventReweighter::matrix_elements(Event const & ev) const{
assert(param_.treat.count(ev.type()) > 0);
if(param_.treat.find(ev.type())->second == EventTreatment::keep){
return fixed_order_scale_ME(ev);
}
- return MEt2_(ev, true);
+ return MEt2_(ev);
}
/**
* \brief Computes the tree level matrix element
*
* @param ev Event in Question
* @returns HEJ approximation to Tree level Matrix Element
*
* This computes the HEJ approximation to the tree level FO
* Matrix element which is used within the LO weighting process.
*/
double EventReweighter::tree_matrix_element(Event const & ev) const{
assert(ev.variations().empty());
assert(param_.treat.count(ev.type()) > 0);
if(param_.treat.find(ev.type())->second == EventTreatment::keep){
return fixed_order_scale_ME(ev).central;
}
- return MEt2_.tree(ev, false).central;
+ return MEt2_.tree(ev).central;
}
/**
* \brief Scale-dependent part of fixed-order matrix element
*
* @param ev Event in question
* @returns Scale variation due to FO-ME.
*
* This is only called to compute the scale variation for events where
* we don't do resummation (e.g. non-FKL).
* Since at tree level the scale dependence is just due to alpha_s,
* it is enough to return the alpha_s(mur) factors in the matrix element.
* The rest drops out in the ratio of (output event ME)/(input event ME),
* so we never have to compute it.
*/
Weights
EventReweighter::fixed_order_scale_ME(Event const & ev) const{
int alpha_s_power = 0;
for(auto const & part: ev.outgoing()){
if(is_parton(part))
++alpha_s_power;
else {
switch(part.type){
case pid::Higgs: {
alpha_s_power += 2;
break;
}
// TODO
case pid::Wp:{
break;
}
case pid::Wm:{
break;
}
case pid::photon:
case pid::Z:
default:
throw not_implemented("Emission of boson of unsupported type");
}
}
}
Weights result;
result.central = pow(pdf_.Halphas(ev.central().mur), alpha_s_power);
for(auto const & var: ev.variations()){
result.variations.emplace_back(
pow(pdf_.Halphas(var.mur), alpha_s_power)
);
}
return result;
}
} // namespace HEJ
diff --git a/src/HepMCInterface.cc b/src/HepMCInterface.cc
index 86a6a41..a50c8f8 100644
--- a/src/HepMCInterface.cc
+++ b/src/HepMCInterface.cc
@@ -1,170 +1,177 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/HepMCInterface.hh"
-#include <cassert>
+#include "HEJ/exceptions.hh"
#ifdef HEJ_BUILD_WITH_HepMC_VERSION
+#include <math.h>
+#include <utility>
+
#include "HEJ/Event.hh"
+#include "HEJ/Particle.hh"
+#include "HepMC/GenCrossSection.h"
#include "HepMC/GenEvent.h"
-#include "HepMC/GenVertex.h"
#include "HepMC/GenParticle.h"
-#include "HepMC/GenCrossSection.h"
-
-#include "LHEF/LHEF.h"
+#include "HepMC/GenVertex.h"
namespace HEJ{
namespace {
HepMC::FourVector to_FourVector(Particle const & sp){
return {sp.px(), sp.py(), sp.pz(), sp.E()};
}
constexpr int status_in = -1;
constexpr int status_decayed = 3;
constexpr int status_out = 1;
template<class HepMCClass, typename... Args>
auto make_ptr(Args&&... args){
#if HEJ_BUILD_WITH_HepMC_VERSION >= 3
return HepMC::make_shared<HepMCClass>(std::forward<Args>(args)...);
#else
return new HepMCClass(std::forward<Args>(args)...);
#endif
}
} // namespace anonymous
HepMCInterface::HepMCInterface():
event_count_(0.), tot_weight_(0.), tot_weight2_(0.)
{}
HepMC::GenCrossSection HepMCInterface::cross_section() const {
HepMC::GenCrossSection xs;
#if HEJ_BUILD_WITH_HepMC_VERSION >= 3
xs.set_cross_section(tot_weight_, sqrt(tot_weight2_), event_count_);
/// @TODO add number of attempted events
#else // HepMC 2
xs.set_cross_section(tot_weight_, sqrt(tot_weight2_));
#endif
return xs;
}
HepMC::GenEvent HepMCInterface::init_kinematics(Event const & event) {
HepMC::GenEvent out_ev{HepMC::Units::GEV, HepMC::Units::MM};
auto vx = make_ptr<HepMC::GenVertex>();
for(auto const & in: event.incoming()){
vx->add_particle_in(
make_ptr<HepMC::GenParticle>(
to_FourVector(in), static_cast<int>(in.type), status_in
)
);
}
for(size_t i=0; i < event.outgoing().size(); ++i){
auto const & out = event.outgoing()[i];
auto particle = make_ptr<HepMC::GenParticle>(
to_FourVector(out), static_cast<int>(out.type), status_out
);
const int status = event.decays().count(i)?status_decayed:status_out;
particle->set_status(status);
if( status == status_decayed){
auto vx_decay = make_ptr<HepMC::GenVertex>();
vx_decay->add_particle_in(particle);
for( auto const & out: event.decays().at(i)){
vx_decay->add_particle_out(
make_ptr<HepMC::GenParticle>(
to_FourVector(out), static_cast<int>(out.type), status_out
)
);
}
out_ev.add_vertex(vx_decay);
}
vx->add_particle_out(particle);
}
out_ev.add_vertex(vx);
return out_ev;
}
void HepMCInterface::set_central(HepMC::GenEvent & out_ev, Event const & event,
ssize_t const weight_index
) {
EventParameters event_param;
if(weight_index < 0)
event_param = event.central();
else if ( (size_t) weight_index < event.variations().size())
event_param = event.variations(weight_index);
else
throw std::invalid_argument{
"HepMCInterface tried to access a weight outside of the variation range."
};
const double wt = event_param.weight;
tot_weight_ += wt;
tot_weight2_ += wt * wt;
if(out_ev.weights().size() == 0){
out_ev.weights().push_back(wt);
} else { // central always on first
out_ev.weights()[0] = wt;
}
#if HEJ_BUILD_WITH_HepMC_VERSION >= 3
out_ev.set_cross_section(
HepMC::make_shared<HepMC::GenCrossSection>(cross_section()) );
#else // HepMC 2
out_ev.set_cross_section( cross_section() );
out_ev.set_signal_process_id(event.type()+1); // "+1": conistent with lhe
out_ev.set_event_scale(event_param.mur);
#endif
++event_count_;
out_ev.set_event_number(event_count_);
/// @TODO add alphaQCD (need function) and alphaQED
/// @TODO output pdf (currently not avaiable from event alone)
}
void HepMCInterface::add_variation(HepMC::GenEvent & out_ev,
std::vector<EventParameters> const & varis
) {
for(auto const & var: varis){
out_ev.weights().push_back(var.weight);
}
/// @TODO add name list for weights
}
HepMC::GenEvent HepMCInterface::operator()(Event const & event,
ssize_t const weight_index
) {
HepMC::GenEvent out_ev(init_kinematics(event));
set_central(out_ev, event, weight_index);
add_variation(out_ev, event.variations());
return out_ev;
}
}
#else // no HepMC => empty class
namespace HepMC {
class GenEvent {};
class GenCrossSection {};
}
namespace HEJ{
HepMCInterface::HepMCInterface(){
throw std::invalid_argument(
"Failed to create HepMCInterface: "
"HEJ 2 was built without HepMC support"
);
}
HepMC::GenEvent HepMCInterface::operator()(Event const &, ssize_t)
{return HepMC::GenEvent();}
HepMC::GenEvent HepMCInterface::init_kinematics(Event const &)
{return HepMC::GenEvent();}
void HepMCInterface::add_variation(HepMC::GenEvent &,
std::vector<EventParameters> const &){}
void HepMCInterface::set_central(HepMC::GenEvent &, Event const &, ssize_t) {}
HepMC::GenCrossSection HepMCInterface::cross_section() const
{return HepMC::GenCrossSection();}
}
#endif
diff --git a/src/HepMCWriter.cc b/src/HepMCWriter.cc
index de08051..e09c538 100644
--- a/src/HepMCWriter.cc
+++ b/src/HepMCWriter.cc
@@ -1,139 +1,148 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/HepMCWriter.hh"
#include <cassert>
+#include "LHEF/LHEF.h"
+
#ifdef HEJ_BUILD_WITH_HepMC_VERSION
#if HEJ_BUILD_WITH_HepMC_VERSION >= 3
-#include "HepMC/WriterAscii.h"
#include "HepMC/LHEFAttributes.h"
+#include "HepMC/WriterAscii.h"
#include "HEJ/Version.hh"
+
#else
#include "HepMC/IO_GenEvent.h"
#endif
-#include "HepMC/GenVertex.h"
+#include <utility>
+
#include "HepMC/GenParticle.h"
+#include "HepMC/GenVertex.h"
-#include "HEJ/utility.hh"
#include "HEJ/Event.hh"
#include "HEJ/exceptions.hh"
#include "HEJ/HepMCInterface.hh"
#if HEJ_BUILD_WITH_HepMC_VERSION >= 3
namespace {
void reset_weight_info(LHEF::HEPRUP & heprup){
heprup.IDWTUP = 2;
// use placeholders for unknown init block values
// we can overwrite them after processing all events
heprup.XSECUP = {0.};
heprup.XERRUP = {0.};
heprup.XMAXUP = {0.};
}
HepMC::shared_ptr<HepMC::GenRunInfo> init_runinfo(LHEF::HEPRUP && heprup){
reset_weight_info(heprup);
HepMC::GenRunInfo runinfo;
auto hepr = HepMC::make_shared<HepMC::HEPRUPAttribute>();
hepr->heprup = heprup;
runinfo.add_attribute(std::string("HEPRUP"), hepr);
for (int i = 0, N = hepr->heprup.generators.size(); i < N; ++i ){
HepMC::GenRunInfo::ToolInfo tool;
tool.name = hepr->heprup.generators[i].name;
tool.version = hepr->heprup.generators[i].version;
tool.description = hepr->heprup.generators[i].contents;
runinfo.tools().push_back(tool);
}
return HepMC::make_shared<HepMC::GenRunInfo>(runinfo);
}
} // namespace anonymous
#endif // HepMC 3
namespace HEJ{
struct HepMCWriter::HepMCWriterImpl{
HepMCInterface hepmc_;
HepMCWriterImpl & operator=(HepMCWriterImpl const & other) = delete;
HepMCWriterImpl(HepMCWriterImpl const & other) = delete;
HepMCWriterImpl & operator=(HepMCWriterImpl && other) = delete;
HepMCWriterImpl(HepMCWriterImpl && other) = delete;
#if HEJ_BUILD_WITH_HepMC_VERSION >= 3
HepMC::WriterAscii writer_;
HepMCWriterImpl(
std::string const & file, LHEF::HEPRUP && heprup
):
hepmc_(),
writer_{file, init_runinfo(std::move(heprup))}
{}
~HepMCWriterImpl(){
writer_.close();
}
#else // HepMC 2
HepMC::IO_GenEvent writer_;
HepMCWriterImpl(
std::string const & file, LHEF::HEPRUP &&
):
hepmc_(),
writer_{file}
{}
#endif
void write(Event const & ev){
auto out_ev = hepmc_(ev);
#if HEJ_BUILD_WITH_HepMC_VERSION >= 3
writer_.write_event(out_ev);
#else // HepMC 2
writer_.write_event(&out_ev);
#endif
}
};
void HepMCWriter::HepMCWriterImplDeleter::operator()(HepMCWriterImpl* p) {
delete p;
}
HepMCWriter::HepMCWriter(std::string const & file, LHEF::HEPRUP heprup):
impl_{std::unique_ptr<HepMCWriterImpl, HepMCWriterImplDeleter>{
new HepMCWriterImpl(file, std::move(heprup))
}}
{}
void HepMCWriter::write(Event const & ev){
impl_->write(ev);
}
} // namespace HEJ
#else // no HepMC
namespace HEJ{
class HepMCWriter::HepMCWriterImpl{};
HepMCWriter::HepMCWriter(std::string const &, LHEF::HEPRUP){
throw std::invalid_argument(
"Failed to create HepMC writer: "
"HEJ 2 was built without HepMC support"
);
}
void HepMCWriter::write(Event const &){
assert(false);
}
void HepMCWriter::HepMCWriterImplDeleter::operator()(HepMCWriterImpl* p) {
delete p;
}
}
#endif
diff --git a/src/JetSplitter.cc b/src/JetSplitter.cc
index 8417141..3d8c3f1 100644
--- a/src/JetSplitter.cc
+++ b/src/JetSplitter.cc
@@ -1,174 +1,184 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/JetSplitter.hh"
+#include <array>
+#include <assert.h>
#include <numeric>
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/PseudoJet.hh"
+
#include "HEJ/Constants.hh"
-#include "HEJ/PhaseSpacePoint.hh"
+#include "HEJ/exceptions.hh"
namespace HEJ {
namespace{
constexpr double ccut=HEJ::CMINPT; // min parton pt
template<class Iterator>
bool same_pt_and_rapidity(
Iterator begin, Iterator end,
fastjet::PseudoJet const & jet
){
static constexpr double ep = 1e-2;
const fastjet::PseudoJet reconstructed_jet = std::accumulate(
begin, end, fastjet::PseudoJet{}
);
return
(std::abs(reconstructed_jet.pt() - jet.pt()) < ep)
&& (std::abs(reconstructed_jet.rapidity() - jet.rapidity()) < ep)
;
}
bool all_in_one_jet(
std::vector<fastjet::PseudoJet> const & partons,
fastjet::JetDefinition jet_def, double min_jet_pt
){
fastjet::ClusterSequence ev(partons, jet_def);
const std::vector<fastjet::PseudoJet> testjet = ev.inclusive_jets(min_jet_pt);
return testjet.size() == 1u
&& testjet[0].constituents().size() == partons.size();
}
}
using SplitResult = JetSplitter::SplitResult;
SplitResult JetSplitter::split(
fastjet::PseudoJet const & j2split, int ncons
) const{
if(ncons <= 0) {
throw std::invalid_argument{
"number of requested jet constituents less than 1"
};
}
double swt = 1.;
std::vector<fastjet::PseudoJet> jcons;
if(ncons == 1){
jcons.emplace_back(j2split);
jcons.back().set_user_index(0);
return {jcons, swt};
}
if(ncons == 2){
return Split2(j2split);
}
const double R_max = R_factor*R_;
assert(R_max < M_PI);
double pt_remaining = j2split.pt();
const double phi_jet = j2split.phi();
const double y_jet = j2split.rapidity();
for(int i = 0; i < ncons - 1; ++i){
/**
* Generate rapidity and azimuthal angle with a distance
* R = sqrt(delta_y^2 + delta_phi^2) < R_max
* from the jet centre
*/
const double R = R_max*ran_.get().flat();
const double theta = 2*M_PI*ran_.get().flat();
const double delta_phi = R*cos(theta);
const double delta_y = R*sin(theta);
/**
* Generate pt such that the total contribution of all partons
* along the jet pt axis does not exceed the jet pt
*/
const double pt_max = pt_remaining/cos(delta_phi);
assert(pt_max > 0);
if(pt_max < ccut) return {}; // no pt remaining for this parton
const double pt = (pt_max - ccut)*ran_.get().flat() + ccut;
pt_remaining -= pt*cos(delta_phi);
jcons.emplace_back(
pt*cos(phi_jet + delta_phi), pt*sin(phi_jet + delta_phi),
pt*sinh(y_jet + delta_y), pt*cosh(y_jet + delta_y)
);
jcons.back().set_user_index(i);
swt *= 2*M_PI*R*R_max*pt*(pt_max - ccut);
}
const fastjet::PseudoJet p_total = std::accumulate(
jcons.begin(), jcons.end(), fastjet::PseudoJet{}
);
// Calculate the pt of the last parton
const double last_px = j2split.px() - p_total.px();
const double last_py = j2split.py() - p_total.py();
const double last_pt = sqrt(last_px*last_px + last_py*last_py);
if(last_pt < ccut) return {};
// Calculate the rapidity of the last parton using the requirement that the
// new jet must have the same rapidity as the LO jet.
const double exp_2y_jet = (j2split.e() + j2split.pz())/(j2split.e() - j2split.pz());
const double bb = (p_total.e()+p_total.pz()) - exp_2y_jet*(p_total.e()-p_total.pz());
const double lasty = log((-bb+sqrt(bb*bb+4.*exp_2y_jet*last_pt*last_pt))/(2.*last_pt));
jcons.emplace_back(
last_px, last_py, last_pt*sinh(lasty), last_pt*cosh(lasty)
);
jcons.back().set_user_index(ncons-1);
assert(same_pt_and_rapidity(begin(jcons), end(jcons), j2split));
// Test that the last parton is not too far away from the jet centre.
if (jcons.back().delta_R(j2split) > R_max) return {};
if(! all_in_one_jet(jcons, jet_def_, min_jet_pt_)) return {};
return {jcons, swt};
}
//! sample y-phi distance to jet pt axis for a jet splitting into two partons
/**
* @param wt Multiplied by the weight of the sampling point
* @returns The distance in units of the jet radius
*/
double JetSplitter::sample_distance_2p(double & wt) const{
static constexpr double x_small = 0.1;
static constexpr double p_small = 0.4;
const double pR = ran_.get().flat();
if(pR < p_small){
wt *= x_small/p_small;
return x_small/p_small*pR;
}
wt *= (1-x_small)/(1-p_small);
return (1-x_small)/(1-p_small)*(pR-p_small) + x_small;
}
// split jet into two partons
SplitResult JetSplitter::Split2(fastjet::PseudoJet const & j2split) const{
static constexpr size_t ncons = 2;
std::vector<fastjet::PseudoJet> jcons(ncons);
std::array<double, ncons> R, phi, y, pt;
double wt = 1;
const double theta = 2*M_PI*ran_.get().flat(); // angle in y-phi plane
// empiric observation: we are always within the jet radius
R[0] = sample_distance_2p(wt)*R_;
R[1] = -sample_distance_2p(wt)*R_;
for(size_t i = 0; i <= 1; ++i){
phi[i] = j2split.phi() + R[i]*cos(theta);
y[i] = j2split.rapidity() + R[i]*sin(theta);
}
for(size_t i = 0; i <= 1; ++i){
pt[i] = (j2split.py() - tan(phi[1-i])*j2split.px())/
(sin(phi[i]) - tan(phi[1-i])*cos(phi[i]));
if(pt[i] < ccut) return {};
jcons[i].reset_PtYPhiM(pt[i], y[i], phi[i]);
jcons[i].set_user_index(i);
}
assert(same_pt_and_rapidity(begin(jcons), end(jcons), j2split));
if(! all_in_one_jet(jcons, jet_def_, min_jet_pt_)) return {};
wt *= 2*M_PI*pt[0]*R[0]*R_*R_;
// from transformation of delta(R[1] - ...) to delta(pt[0] - ...)
const double dphi0 = phi[0] - j2split.phi();
const double ptJ = j2split.pt();
const double jacobian = cos(theta)*pt[1]*pt[1]/(ptJ*sin(dphi0));
return {jcons, jacobian*wt};
}
}
diff --git a/src/LesHouchesWriter.cc b/src/LesHouchesWriter.cc
index 4605ac1..d5f0149 100644
--- a/src/LesHouchesWriter.cc
+++ b/src/LesHouchesWriter.cc
@@ -1,90 +1,95 @@
-#include <stdexcept>
-#include <memory>
-#include <cassert>
-
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/LesHouchesWriter.hh"
-#include "HEJ/event_types.hh"
-#include "HEJ/Version.hh"
+
+#include <cassert>
+#include <utility>
+#include <vector>
#include "HEJ/Event.hh"
+#include "HEJ/event_types.hh"
+#include "HEJ/utility.hh"
namespace HEJ{
namespace{
template<class T, class... Args>
std::unique_ptr<T> make_unique(Args&&... a){
return std::unique_ptr<T>{new T{std::forward<Args>(a)...}};
}
}
LesHouchesWriter::LesHouchesWriter(
std::string const & file, LHEF::HEPRUP heprup
):
out_{file, std::fstream::in | std::fstream::out | std::fstream::trunc},
writer_{HEJ::make_unique<LHEF::Writer>(out_)}
{
if(! out_.is_open()){
throw std::ios_base::failure("Failed to open " + file);
};
writer_->heprup = std::move(heprup);
// lhe Stardard: IDWTUP (negative => weights = +/-)
// 1: weighted events, xs = mean(weight), XMAXUP given
// 2: weighted events, xs = XSECUP, XMAXUP given
// 3: unweighted events, no additional information given
// 4: unweighted events, xs = mean(weight), no additional information given
writer_->heprup.IDWTUP = 2;
// use placeholders for unknown init block values
// we can overwrite them after processing all events
writer_->heprup.XSECUP = std::vector<double>(event_type::last_type+1, 0.);
writer_->heprup.XERRUP = std::vector<double>(event_type::last_type+1, 0.);
writer_->heprup.XMAXUP = std::vector<double>(event_type::last_type+1, 0.);
write_init();
}
void LesHouchesWriter::write(Event const & ev){
assert(writer_ && out_.is_open());
const double wt = ev.central().weight;
writer_->hepeup = HEJ::to_HEPEUP(std::move(ev), &heprup());
writer_->writeEvent();
heprup().XSECUP[ev.type()] += wt;
heprup().XERRUP[ev.type()] += wt*wt;
if(wt > heprup().XMAXUP[ev.type()]){
heprup().XMAXUP[ev.type()] = wt;
}
}
// this function is called after overwritting the Les Houches init block
// assert that we have overwritten *exactly* the init block,
// i.e. an intact event block is next
void assert_next_event_intact(std::istream & out){
(void) out; // suppress compiler warnings if not in debug mode
#ifndef NDEBUG
std::string line;
getline(out, line);
assert(line == "<event>");
#endif
}
void LesHouchesWriter::rewrite_init(){
assert(writer_ && out_.is_open());
// replace placeholder entries
const auto pos = out_.tellp();
out_.seekp(0);
writer_->init();
assert_next_event_intact(out_);
out_.seekp(pos);
}
LesHouchesWriter::~LesHouchesWriter(){
assert(writer_ && out_.is_open());
for(auto & xs_err: heprup().XERRUP)
{
xs_err = sqrt(xs_err);
}
rewrite_init();
}
}
diff --git a/src/MatrixElement.cc b/src/MatrixElement.cc
index 503bf37..ef84b92 100644
--- a/src/MatrixElement.cc
+++ b/src/MatrixElement.cc
@@ -1,1801 +1,1794 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/MatrixElement.hh"
+#include <algorithm>
+#include <assert.h>
+#include <limits>
+#include <math.h>
+#include <stddef.h>
#include <unordered_map>
+#include <utility>
-#include <CLHEP/Random/Randomize.h>
-#include <CLHEP/Random/RanluxEngine.h>
+#include "CLHEP/Vector/LorentzVector.h"
+
+#include "fastjet/ClusterSequence.hh"
#include "HEJ/Constants.hh"
#include "HEJ/currents.hh"
-#include "HEJ/exceptions.hh"
#include "HEJ/PDG_codes.hh"
+#include "HEJ/event_types.hh"
+#include "HEJ/Event.hh"
+#include "HEJ/exceptions.hh"
+#include "HEJ/Particle.hh"
#include "HEJ/utility.hh"
namespace HEJ{
//cf. last line of eq. (22) in \ref Andersen:2011hs
double MatrixElement::omega0(
double alpha_s, double mur,
fastjet::PseudoJet const & q_j, double lambda
) const {
const double result = - alpha_s*N_C/M_PI*log(q_j.perp2()/(lambda*lambda));
if(! param_.log_correction) return result;
// use alpha_s(sqrt(q_j*lambda)), evolved to mur
return (
1. + alpha_s/(4.*M_PI)*beta0*log(mur*mur/(q_j.perp()*lambda))
)*result;
}
Weights MatrixElement::operator()(
- Event const & event,
- bool check_momenta
+ Event const & event
) const {
- return tree(event, check_momenta)*virtual_corrections(event);
+ return tree(event)*virtual_corrections(event);
}
Weights MatrixElement::tree(
- Event const & event,
- bool check_momenta
+ Event const & event
) const {
- if(! is_HEJ(event.type())) {
- return Weights{0., std::vector<double>(event.variations().size(), 0.)};
- }
- return tree_param(event)*tree_kin(event, check_momenta);
+ return tree_param(event)*tree_kin(event);
}
Weights MatrixElement::tree_param(
Event const & event
) const {
+ if(! is_HEJ(event.type())) {
+ return Weights{0., std::vector<double>(event.variations().size(), 0.)};
+ }
Weights result;
// only compute once for each renormalisation scale
std::unordered_map<double, double> known;
result.central = tree_param(event, event.central().mur);
known.emplace(event.central().mur, result.central);
for(auto const & var: event.variations()) {
const auto ME_it = known.find(var.mur);
if(ME_it == end(known)) {
const double wt = tree_param(event, var.mur);
result.variations.emplace_back(wt);
known.emplace(var.mur, wt);
}
else {
result.variations.emplace_back(ME_it->second);
}
}
return result;
}
Weights MatrixElement::virtual_corrections(
Event const & event
) const {
if(! is_HEJ(event.type())) {
return Weights{0., std::vector<double>(event.variations().size(), 0.)};
}
Weights result;
// only compute once for each renormalisation scale
std::unordered_map<double, double> known;
result.central = virtual_corrections(event, event.central().mur);
known.emplace(event.central().mur, result.central);
for(auto const & var: event.variations()) {
const auto ME_it = known.find(var.mur);
if(ME_it == end(known)) {
const double wt = virtual_corrections(event, var.mur);
result.variations.emplace_back(wt);
known.emplace(var.mur, wt);
}
else {
result.variations.emplace_back(ME_it->second);
}
}
return result;
}
double MatrixElement::virtual_corrections_W(
Event const & event,
double mur,
Particle const & WBoson
) const{
auto const & in = event.incoming();
const auto partons = filter_partons(event.outgoing());
fastjet::PseudoJet const & pa = in.front().p;
#ifndef NDEBUG
fastjet::PseudoJet const & pb = in.back().p;
double const norm = (in.front().p + in.back().p).E();
#endif
assert(std::is_sorted(partons.begin(), partons.end(), rapidity_less{}));
assert(partons.size() >= 2);
assert(pa.pz() < pb.pz());
fastjet::PseudoJet q = pa - partons[0].p;
size_t first_idx = 0;
size_t last_idx = partons.size() - 1;
bool wc = true;
bool wqq = false;
// With extremal qqx or unordered gluon outside the extremal
// partons then it is not part of the FKL ladder and does not
// contribute to the virtual corrections. W emitted from the
// most backward leg must be taken into account in t-channel
if (event.type() == event_type::FKL) {
if (in[0].type != partons[0].type ){
q -= WBoson.p;
wc = false;
}
}
else if (event.type() == event_type::unob) {
q -= partons[1].p;
++first_idx;
if (in[0].type != partons[1].type ){
q -= WBoson.p;
wc = false;
}
}
else if (event.type() == event_type::qqxexb) {
q -= partons[1].p;
++first_idx;
if (abs(partons[0].type) != abs(partons[1].type)){
q -= WBoson.p;
wc = false;
}
}
if(event.type() == event_type::unof
|| event.type() == event_type::qqxexf){
--last_idx;
}
size_t first_idx_qqx = last_idx;
size_t last_idx_qqx = last_idx;
bool backwards_FKL = (event.type() == event_type::unob || event.type() == event_type::qqxexb);
//if qqxMid event, virtual correction do not occur between
//qqx pair.
if(event.type() == event_type::qqxmid){
const auto backquark = std::find_if(
begin(partons) + 1, end(partons) - 1 ,
[](Particle const & s){ return (s.type != pid::gluon); }
);
if(backquark == end(partons) || (backquark+1)->type==pid::gluon) return 0;
if(abs(backquark->type) != abs((backquark+1)->type)) {
wqq=true;
wc=false;
}
last_idx = std::distance(begin(partons), backquark);
first_idx_qqx = last_idx+1;
}
double exponent = 0;
const double alpha_s = alpha_s_(mur);
for(size_t j = first_idx; j < last_idx; ++j){
exponent += omega0(alpha_s, mur, q, CLAMBDA)*(
partons[j+1].rapidity() - partons[j].rapidity()
);
q -=partons[j+1].p;
} // End Loop one
if (last_idx != first_idx_qqx) q -= partons[last_idx+1].p;
if (wqq) q -= WBoson.p;
for(size_t j = first_idx_qqx; j < last_idx_qqx; ++j){
exponent += omega0(alpha_s, mur, q, CLAMBDA)*(
partons[j+1].rapidity() - partons[j].rapidity()
);
q -= partons[j+1].p;
}
if (wc) q -= WBoson.p;
assert(
nearby(q, -1*pb, norm)
|| is_AWZH_boson(partons.back().type)
|| event.type() == event_type::unof
|| event.type() == event_type::qqxexf
);
return exp(exponent);
}
double MatrixElement::virtual_corrections(
Event const & event,
double mur
) const{
auto const & in = event.incoming();
auto const & out = event.outgoing();
fastjet::PseudoJet const & pa = in.front().p;
#ifndef NDEBUG
fastjet::PseudoJet const & pb = in.back().p;
double const norm = (in.front().p + in.back().p).E();
#endif
const auto AWZH_boson = std::find_if(
begin(out), end(out),
[](Particle const & p){ return is_AWZH_boson(p); }
);
if(AWZH_boson != end(out) && abs(AWZH_boson->type) == pid::Wp){
return virtual_corrections_W(event, mur, *AWZH_boson);
}
assert(std::is_sorted(out.begin(), out.end(), rapidity_less{}));
assert(out.size() >= 2);
assert(pa.pz() < pb.pz());
fastjet::PseudoJet q = pa - out[0].p;
size_t first_idx = 0;
size_t last_idx = out.size() - 1;
// if there is a Higgs boson, extremal qqx or unordered gluon
// outside the extremal partons then it is not part of the FKL
// ladder and does not contribute to the virtual corrections
if((out.front().type == pid::Higgs)
|| event.type() == event_type::unob
|| event.type() == event_type::qqxexb){
q -= out[1].p;
++first_idx;
}
if((out.back().type == pid::Higgs)
|| event.type() == event_type::unof
|| event.type() == event_type::qqxexf){
--last_idx;
}
size_t first_idx_qqx = last_idx;
size_t last_idx_qqx = last_idx;
//if qqxMid event, virtual correction do not occur between
//qqx pair.
if(event.type() == event_type::qqxmid){
const auto backquark = std::find_if(
begin(out) + 1, end(out) - 1 ,
[](Particle const & s){ return (s.type != pid::gluon && is_parton(s.type)); }
);
if(backquark == end(out) || (backquark+1)->type==pid::gluon) return 0;
last_idx = std::distance(begin(out), backquark);
first_idx_qqx = last_idx+1;
}
double exponent = 0;
const double alpha_s = alpha_s_(mur);
for(size_t j = first_idx; j < last_idx; ++j){
exponent += omega0(alpha_s, mur, q, CLAMBDA)*(
out[j+1].rapidity() - out[j].rapidity()
);
q -= out[j+1].p;
}
if (last_idx != first_idx_qqx) q -= out[last_idx+1].p;
for(size_t j = first_idx_qqx; j < last_idx_qqx; ++j){
exponent += omega0(alpha_s, mur, q, CLAMBDA)*(
out[j+1].rapidity() - out[j].rapidity()
);
q -= out[j+1].p;
}
assert(
nearby(q, -1*pb, norm)
|| out.back().type == pid::Higgs
|| event.type() == event_type::unof
|| event.type() == event_type::qqxexf
);
return exp(exponent);
}
} // namespace HEJ
namespace {
//! Lipatov vertex for partons emitted into extremal jets
double C2Lipatov(CLHEP::HepLorentzVector qav, CLHEP::HepLorentzVector qbv,
CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector p2)
{
CLHEP::HepLorentzVector temptrans=-(qav+qbv);
CLHEP::HepLorentzVector p5=qav-qbv;
CLHEP::HepLorentzVector CL=temptrans
+ p1*(qav.m2()/p5.dot(p1) + 2.*p5.dot(p2)/p1.dot(p2))
- p2*(qbv.m2()/p5.dot(p2) + 2.*p5.dot(p1)/p1.dot(p2));
-
- // cout << "#Fadin qa : "<<qav<<endl;
- // cout << "#Fadin qb : "<<qbv<<endl;
- // cout << "#Fadin p1 : "<<p1<<endl;
- // cout << "#Fadin p2 : "<<p2<<endl;
- // cout << "#Fadin p5 : "<<p5<<endl;
- // cout << "#Fadin Gauge Check : "<< CL.dot(p5)<<endl;
- // cout << "#Fadin C2L : "<< -CL.dot(CL)<<" "<<-CL.dot(CL)/(qav.m2()*qbv.m2())/(4./p5.perp2())<<endl;
-
- // TODO can this dead test go?
- // if (-CL.dot(CL)<0.)
- // if (fabs(CL.dot(p5))>fabs(CL.dot(CL))) // not sufficient!
- // return 0.;
- // else
return -CL.dot(CL);
}
//! Lipatov vertex with soft subtraction for partons emitted into extremal jets
double C2Lipatovots(CLHEP::HepLorentzVector qav, CLHEP::HepLorentzVector qbv,
CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector p2)
{
double kperp=(qav-qbv).perp();
if (kperp>HEJ::CLAMBDA)
return C2Lipatov(qav, qbv, p1, p2)/(qav.m2()*qbv.m2());
else {
double Cls=(C2Lipatov(qav, qbv, p1, p2)/(qav.m2()*qbv.m2()));
return Cls-4./(kperp*kperp);
}
}
//! Lipatov vertex
double C2Lipatov(CLHEP::HepLorentzVector qav, CLHEP::HepLorentzVector qbv,
CLHEP::HepLorentzVector pim, CLHEP::HepLorentzVector pip,
CLHEP::HepLorentzVector pom, CLHEP::HepLorentzVector pop) // B
{
CLHEP::HepLorentzVector temptrans=-(qav+qbv);
CLHEP::HepLorentzVector p5=qav-qbv;
CLHEP::HepLorentzVector CL=temptrans
+ qav.m2()*(1./p5.dot(pip)*pip + 1./p5.dot(pop)*pop)/2.
- qbv.m2()*(1./p5.dot(pim)*pim + 1./p5.dot(pom)*pom)/2.
+ ( pip*(p5.dot(pim)/pip.dot(pim) + p5.dot(pom)/pip.dot(pom))
+ pop*(p5.dot(pim)/pop.dot(pim) + p5.dot(pom)/pop.dot(pom))
- pim*(p5.dot(pip)/pip.dot(pim) + p5.dot(pop)/pop.dot(pim))
- pom*(p5.dot(pip)/pip.dot(pom) + p5.dot(pop)/pop.dot(pom)) )/2.;
return -CL.dot(CL);
}
//! Lipatov vertex with soft subtraction
double C2Lipatovots(CLHEP::HepLorentzVector qav, CLHEP::HepLorentzVector qbv,
CLHEP::HepLorentzVector pa, CLHEP::HepLorentzVector pb,
CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector p2)
{
double kperp=(qav-qbv).perp();
if (kperp>HEJ::CLAMBDA)
return C2Lipatov(qav, qbv, pa, pb, p1, p2)/(qav.m2()*qbv.m2());
else {
double Cls=(C2Lipatov(qav, qbv, pa, pb, p1, p2)/(qav.m2()*qbv.m2()));
double temp=Cls-4./(kperp*kperp);
return temp;
}
}
/** Matrix element squared for tree-level current-current scattering
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param pn Particle n Momentum
* @param pb Particle b Momentum
* @param p1 Particle 1 Momentum
* @param pa Particle a Momentum
* @returns ME Squared for Tree-Level Current-Current Scattering
*/
double ME_current(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & pa
){
if (aptype==21&&bptype==21) {
return jM2gg(pn,pb,p1,pa);
} else if (aptype==21&&bptype!=21) {
if (bptype > 0)
return jM2qg(pn,pb,p1,pa);
else
return jM2qbarg(pn,pb,p1,pa);
}
else if (bptype==21&&aptype!=21) { // ----- || -----
if (aptype > 0)
return jM2qg(p1,pa,pn,pb);
else
return jM2qbarg(p1,pa,pn,pb);
}
else { // they are both quark
if (bptype>0) {
if (aptype>0)
return jM2qQ(pn,pb,p1,pa);
else
return jM2qQbar(pn,pb,p1,pa);
}
else {
if (aptype>0)
return jM2qQbar(p1,pa,pn,pb);
else
return jM2qbarQbar(pn,pb,p1,pa);
}
}
throw std::logic_error("unknown particle types");
}
/** Matrix element squared for tree-level current-current scattering With W+Jets
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param pn Particle n Momentum
* @param pb Particle b Momentum
* @param p1 Particle 1 Momentum
* @param pa Particle a Momentum
* @returns ME Squared for Tree-Level Current-Current Scattering
*/
double ME_W_current(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & plbar,
CLHEP::HepLorentzVector const & pl,
bool const wc
){
// We know it cannot be gg incoming.
assert(!(aptype==21 && bptype==21));
if (aptype==21&&bptype!=21) {
if (bptype > 0)
return jMWqg(pn,plbar,pl,pb,p1,pa);
else
return jMWqbarg(pn,plbar,pl,pb,p1,pa);
}
else if (bptype==21&&aptype!=21) { // ----- || -----
if (aptype > 0)
return jMWqg(p1,plbar,pl,pa,pn,pb);
else
return jMWqbarg(p1,plbar,pl,pa,pn,pb);
}
else { // they are both quark
if (wc==true){ // emission off b, (first argument pbout)
if (bptype>0) {
if (aptype>0)
return jMWqQ(pn,plbar,pl,pb,p1,pa);
else
return jMWqQbar(pn,plbar,pl,pb,p1,pa);
}
else {
if (aptype>0)
return jMWqbarQ(pn,plbar,pl,pb,p1,pa);
else
return jMWqbarQbar(pn,plbar,pl,pb,p1,pa);
}
}
else{ // emission off a, (first argument paout)
if (aptype > 0) {
if (bptype > 0)
return jMWqQ(p1,plbar,pl,pa,pn,pb);
else
return jMWqQbar(p1,plbar,pl,pa,pn,pb);
}
else { // a is anti-quark
if (bptype > 0)
return jMWqbarQ(p1,plbar,pl,pa,pn,pb);
else
return jMWqbarQbar(p1,plbar,pl,pa,pn,pb);
}
}
}
throw std::logic_error("unknown particle types");
}
/** Matrix element squared for backwards uno tree-level current-current scattering With W+Jets
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param pn Particle n Momentum
* @param pb Particle b Momentum
* @param p1 Particle 1 Momentum
* @param pa Particle a Momentum
* @param pg Unordered gluon momentum
* @returns ME Squared for unob Tree-Level Current-Current Scattering
*/
double ME_W_unob_current(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & pg,
CLHEP::HepLorentzVector const & plbar,
CLHEP::HepLorentzVector const & pl,
bool const wc
){
// we know they are not both gluons
if (bptype == 21 && aptype != 21) { // b gluon => W emission off a
if (aptype > 0)
return jM2Wunogqg(pg,p1,plbar,pl,pa,pn,pb);
else
return jM2Wunogqbarg(pg,p1,plbar,pl,pa,pn,pb);
}
else { // they are both quark
if (wc==true) {// emission off b, i.e. b is first current
if (bptype>0){
if (aptype>0)
return junobMWqQg(pn,plbar,pl,pb,p1,pa,pg);
else
return junobMWqQbarg(pn,plbar,pl,pb,p1,pa,pg);
}
else{
if (aptype>0)
return junobMWqbarQg(pn,plbar,pl,pb,p1,pa,pg);
else
return junobMWqbarQbarg(pn,plbar,pl,pb,p1,pa,pg);
}
}
else {// wc == false, emission off a, i.e. a is first current
if (aptype > 0) {
if (bptype > 0) //qq
return jM2WunogqQ(pg,p1,plbar,pl,pa,pn,pb);
else //qqbar
return jM2WunogqQbar(pg,p1,plbar,pl,pa,pn,pb);
}
else { // a is anti-quark
if (bptype > 0) //qbarq
return jM2WunogqbarQ(pg,p1,plbar,pl,pa,pn,pb);
else //qbarqbar
return jM2WunogqbarQbar(pg,p1,plbar,pl,pa,pn,pb);
}
}
}
}
/** Matrix element squared for uno forward tree-level current-current scattering With W+Jets
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param pn Particle n Momentum
* @param pb Particle b Momentum
* @param p1 Particle 1 Momentum
* @param pa Particle a Momentum
* @param pg Unordered gluon momentum
* @returns ME Squared for unof Tree-Level Current-Current Scattering
*/
double ME_W_unof_current(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & pg,
CLHEP::HepLorentzVector const & plbar,
CLHEP::HepLorentzVector const & pl,
bool const wc
){
// we know they are not both gluons
if (aptype==21 && bptype!=21) {//a gluon => W emission off b
if (bptype > 0)
return jM2Wunogqg(pg, pn,plbar, pl, pb, p1, pa);
else
return jM2Wunogqbarg(pg, pn,plbar, pl, pb, p1, pa);
}
else { // they are both quark
if (wc==true) {// emission off b, i.e. b is first current
if (bptype>0){
if (aptype>0)
return jM2WunogqQ(pg,pn,plbar,pl,pb,p1,pa);
else
return jM2WunogqQbar(pg,pn,plbar,pl,pb,p1,pa);
}
else{
if (aptype>0)
return jM2WunogqbarQ(pg,pn,plbar,pl,pb,p1,pa);
else
return jM2WunogqbarQbar(pg,pn,plbar,pl,pb,p1,pa);
}
}
else {// wc == false, emission off a, i.e. a is first current
if (aptype > 0) {
if (bptype > 0) //qq
return junofMWgqQ(pg,pn,pb,p1,plbar,pl,pa);
else //qqbar
return junofMWgqQbar(pg,pn,pb,p1,plbar,pl,pa);
}
else { // a is anti-quark
if (bptype > 0) //qbarq
return junofMWgqbarQ(pg,pn,pb,p1,plbar,pl,pa);
else //qbarqbar
return junofMWgqbarQbar(pg,pn,pb,p1,plbar,pl,pa);
}
}
}
}
/** \brief Matrix element squared for backward qqx tree-level current-current scattering With W+Jets
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param pa Initial state a Momentum
* @param pb Initial state b Momentum
* @param pq Final state q Momentum
* @param pqbar Final state qbar Momentum
* @param pn Final state n Momentum
* @param plbar Final state anti-lepton momentum
* @param pl Final state lepton momentum
* @returns ME Squared for qqxb Tree-Level Current-Current Scattering
*/
double ME_W_qqxb_current(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & pq,
CLHEP::HepLorentzVector const & pqbar,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & plbar,
CLHEP::HepLorentzVector const & pl,
bool const wc
){
// CAM factors for the qqx amps, and qqbar ordering (default, qbar extremal)
bool swapQuarkAntiquark=false;
double CFbackward;
if (pqbar.rapidity() > pq.rapidity()){
swapQuarkAntiquark=true;
CFbackward = (0.5*(3.-1./3.)*(pa.minus()/(pq.minus())+(pq.minus())/pa.minus())+1./3.)*3./4.;
}
else{
CFbackward = (0.5*(3.-1./3.)*(pa.minus()/(pqbar.minus())+(pqbar.minus())/pa.minus())+1./3.)*3./4.;
}
// With qqbar we could have 2 incoming gluons and W Emission
if (aptype==21&&bptype==21) {//a gluon, b gluon gg->qqbarWg
// This will be a wqqx emission as there is no other possible W Emission Site.
if (swapQuarkAntiquark){
return jM2Wggtoqqbarg(pa, pqbar, plbar, pl, pq, pn,pb)*CFbackward;}
else {
return jM2Wggtoqbarqg(pa, pq, plbar, pl, pqbar, pn,pb)*CFbackward;}
}
else if (aptype==21&&bptype!=21 ) {//a gluon => W emission off b leg or qqx
if (wc!=1){ // W Emitted from backwards qqx
if (swapQuarkAntiquark){
return jM2WgQtoqqbarQ(pa, pq, plbar, pl, pqbar, pn, pb)*CFbackward;}
else{
return jM2WgQtoqbarqQ(pa, pq, plbar, pl, pqbar, pn, pb)*CFbackward;}
}
else { // W Must be emitted from forwards leg.
if(bptype > 0){
if (swapQuarkAntiquark){
return jM2WgqtoQQqW(pb, pa, pn, pqbar, pq, plbar, pl, false)*CFbackward;}
else{
return jM2WgqtoQQqW(pb, pa, pn, pq, pqbar, plbar, pl, false)*CFbackward;}
} else {
if (swapQuarkAntiquark){
return jM2WgqtoQQqW(pb, pa, pn, pqbar, pq, plbar, pl, true)*CFbackward;}
else{
return jM2WgqtoQQqW(pb, pa, pn, pq, pqbar, plbar, pl, true)*CFbackward;}
}
}
}
else{
throw std::logic_error("Incompatible incoming particle types with qqxb");
}
}
/* \brief Matrix element squared for forward qqx tree-level current-current scattering With W+Jets
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param pa Initial state a Momentum
* @param pb Initial state b Momentum
* @param pq Final state q Momentum
* @param pqbar Final state qbar Momentum
* @param p1 Final state 1 Momentum
* @param plbar Final state anti-lepton momentum
* @param pl Final state lepton momentum
* @returns ME Squared for qqxf Tree-Level Current-Current Scattering
*/
double ME_W_qqxf_current(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & pq,
CLHEP::HepLorentzVector const & pqbar,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & plbar,
CLHEP::HepLorentzVector const & pl,
bool const wc
){
// CAM factors for the qqx amps, and qqbar ordering (default, qbar extremal)
bool swapQuarkAntiquark=false;
double CFforward;
if (pqbar.rapidity() < pq.rapidity()){
swapQuarkAntiquark=true;
CFforward = (0.5*(3.-1./3.)*(pb.plus()/(pq.plus())+(pq.plus())/pb.plus())+1./3.)*3./4.;
}
else{
CFforward = (0.5*(3.-1./3.)*(pb.plus()/(pqbar.plus())+(pqbar.plus())/pb.plus())+1./3.)*3./4.;
}
// With qqbar we could have 2 incoming gluons and W Emission
if (aptype==21&&bptype==21) {//a gluon, b gluon gg->qqbarWg
// This will be a wqqx emission as there is no other possible W Emission Site.
if (swapQuarkAntiquark){
return jM2Wggtoqqbarg(pb, pqbar, plbar, pl, pq, p1,pa)*CFforward;}
else {
return jM2Wggtoqbarqg(pb, pq, plbar, pl, pqbar, p1,pa)*CFforward;}
}
else if (bptype==21&&aptype!=21) {// b gluon => W emission off a or qqx
if (wc==1){ // W Emitted from forwards qqx
if (swapQuarkAntiquark){
return jM2WgQtoqbarqQ(pb, pq, plbar,pl, pqbar, p1, pa)*CFforward;}
else {
return jM2WgQtoqqbarQ(pb, pq, plbar,pl, pqbar, p1, pa)*CFforward;}
}
// W Must be emitted from backwards leg.
if (aptype > 0){
if (swapQuarkAntiquark){
return jM2WgqtoQQqW(pa,pb, p1, pqbar, pq, plbar, pl, false)*CFforward;}
else{
return jM2WgqtoQQqW(pa,pb, p1, pq, pqbar, plbar, pl, false)*CFforward;}
} else
{
if (swapQuarkAntiquark){
return jM2WgqtoQQqW(pa,pb, p1, pqbar, pq, plbar, pl, true)*CFforward;}
else{
return jM2WgqtoQQqW(pa,pb, p1, pq, pqbar, plbar, pl, true)*CFforward;}
}
}
else{
throw std::logic_error("Incompatible incoming particle types with qqxf");
}
}
/* \brief Matrix element squared for central qqx tree-level current-current scattering With W+Jets
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param nabove Number of gluons emitted before central qqxpair
* @param nbelow Number of gluons emitted after central qqxpair
* @param pa Initial state a Momentum
* @param pb Initial state b Momentum\
* @param pq Final state qbar Momentum
* @param pqbar Final state q Momentum
* @param partons Vector of all outgoing partons
* @param plbar Final state anti-lepton momentum
* @param pl Final state lepton momentum
* @param wqq Boolean. True siginfies W boson is emitted from Central qqx
* @param wc Boolean. wc=true signifies w boson emitted from leg b; if wqq=false.
* @returns ME Squared for qqxmid Tree-Level Current-Current Scattering
*/
double ME_W_qqxmid_current(
int aptype, int bptype,
int nabove, int nbelow,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & pq,
CLHEP::HepLorentzVector const & pqbar,
std::vector<HLV> partons,
CLHEP::HepLorentzVector const & plbar,
CLHEP::HepLorentzVector const & pl,
bool const wqq, bool const wc
){
// CAM factors for the qqx amps, and qqbar ordering (default, pq backwards)
bool swapQuarkAntiquark=false;
if (pqbar.rapidity() < pq.rapidity()){
swapQuarkAntiquark=true;
}
double CFforward = (0.5*(3.-1./3.)*(pb.plus()/(partons[partons.size()-1].plus())+(partons[partons.size()-1].plus())/pb.plus())+1./3.)*3./4.;
double CFbackward = (0.5*(3.-1./3.)*(pa.minus()/(partons[0].minus())+(partons[0].minus())/pa.minus())+1./3.)*3./4.;
double wt=1.;
if (aptype==21) wt*=CFbackward;
if (bptype==21) wt*=CFforward;
if (aptype <=0 && bptype <=0){ // Both External AntiQuark
if (wqq==1){//emission from central qqbar
return wt*jM2WqqtoqQQq(pa, pb, pl,plbar, partons,true,true, swapQuarkAntiquark, nabove);
}
else if (wc==1){//emission from b leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons, true,true, swapQuarkAntiquark, nabove, nbelow, true);
}
else { // emission from a leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons, true,true, swapQuarkAntiquark, nabove, nbelow, false);
}
} // end both antiquark
else if (aptype<=0){ // a is antiquark
if (wqq==1){//emission from central qqbar
return wt*jM2WqqtoqQQq(pa, pb, pl,plbar, partons, false, true, swapQuarkAntiquark, nabove);
}
else if (wc==1){//emission from b leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons,false,true, swapQuarkAntiquark, nabove, nbelow, true);
}
else { // emission from a leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons, false, true, swapQuarkAntiquark, nabove, nbelow, false);
}
} // end a is antiquark
else if (bptype<=0){ // b is antiquark
if (wqq==1){//emission from central qqbar
return wt*jM2WqqtoqQQq(pa, pb, pl,plbar, partons, true, false, swapQuarkAntiquark, nabove);
}
else if (wc==1){//emission from b leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons, true, false, swapQuarkAntiquark, nabove, nbelow, true);
}
else { // emission from a leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons, true, false, swapQuarkAntiquark, nabove, nbelow, false);
}
} //end b is antiquark
else{ //Both Quark or gluon
if (wqq==1){//emission from central qqbar
return wt*jM2WqqtoqQQq(pa, pb, pl, plbar, partons, false, false, swapQuarkAntiquark, nabove);}
else if (wc==1){//emission from b leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons, false, false, swapQuarkAntiquark, nabove, nbelow, true);
}
else { // emission from a leg
return wt*jM2WqqtoqQQqW(pa, pb, pl,plbar, partons, false, false, swapQuarkAntiquark, nabove, nbelow, false);
}
}
}
/** \brief Matrix element squared for tree-level current-current scattering with Higgs
* @param aptype Particle a PDG ID
* @param bptype Particle b PDG ID
* @param pn Particle n Momentum
* @param pb Particle b Momentum
* @param p1 Particle 1 Momentum
* @param pa Particle a Momentum
* @param qH t-channel momentum before Higgs
* @param qHp1 t-channel momentum after Higgs
* @returns ME Squared for Tree-Level Current-Current Scattering with Higgs
*/
double ME_Higgs_current(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & qH, // t-channel momentum before Higgs
CLHEP::HepLorentzVector const & qHp1, // t-channel momentum after Higgs
double mt, bool include_bottom, double mb
){
if (aptype==21&&bptype==21) // gg initial state
return MH2gg(pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
else if (aptype==21&&bptype!=21) {
if (bptype > 0)
return MH2qg(pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb)*4./9.;
else
return MH2qbarg(pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb)*4./9.;
}
else if (bptype==21&&aptype!=21) {
if (aptype > 0)
return MH2qg(p1,pa,pn,pb,-qH,-qHp1,mt,include_bottom,mb)*4./9.;
else
return MH2qbarg(p1,pa,pn,pb,-qH,-qHp1,mt,include_bottom,mb)*4./9.;
}
else { // they are both quark
if (bptype>0) {
if (aptype>0)
return MH2qQ(pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb)*4.*4./(9.*9.);
else
return MH2qQbar(pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb)*4.*4./(9.*9.);
}
else {
if (aptype>0)
return MH2qQbar(p1,pa,pn,pb,-qH,-qHp1,mt,include_bottom,mb)*4.*4./(9.*9.);
else
return MH2qbarQbar(pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb)*4.*4./(9.*9.);
}
}
throw std::logic_error("unknown particle types");
}
/** \brief Current matrix element squared with Higgs and unordered forward emission
* @param aptype Particle A PDG ID
* @param bptype Particle B PDG ID
* @param punof Unordered Particle Momentum
* @param pn Particle n Momentum
* @param pb Particle b Momentum
* @param p1 Particle 1 Momentum
* @param pa Particle a Momentum
* @param qH t-channel momentum before Higgs
* @param qHp1 t-channel momentum after Higgs
* @returns ME Squared with Higgs and unordered forward emission
*/
double ME_Higgs_current_unof(
int aptype, int bptype,
CLHEP::HepLorentzVector const & punof,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & qH, // t-channel momentum before Higgs
CLHEP::HepLorentzVector const & qHp1, // t-channel momentum after Higgs
double mt, bool include_bottom, double mb
){
if (aptype==21&&bptype!=21) {
if (bptype > 0)
return jM2unogqHg(punof,pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
else
return jM2unogqbarHg(punof,pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
}
else { // they are both quark
if (bptype>0) {
if (aptype>0)
return jM2unogqHQ(punof,pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
else
return jM2unogqHQbar(punof,pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
}
else {
if (aptype>0)
return jM2unogqbarHQ(punof,pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
else
return jM2unogqbarHQbar(punof,pn,pb,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
}
}
throw std::logic_error("unknown particle types");
}
/** \brief Current matrix element squared with Higgs and unordered backward emission
* @param aptype Particle A PDG ID
* @param bptype Particle B PDG ID
* @param pn Particle n Momentum
* @param pb Particle b Momentum
* @param punob Unordered back Particle Momentum
* @param p1 Particle 1 Momentum
* @param pa Particle a Momentum
* @param qH t-channel momentum before Higgs
* @param qHp1 t-channel momentum after Higgs
* @returns ME Squared with Higgs and unordered backward emission
*/
double ME_Higgs_current_unob(
int aptype, int bptype,
CLHEP::HepLorentzVector const & pn,
CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & punob,
CLHEP::HepLorentzVector const & p1,
CLHEP::HepLorentzVector const & pa,
CLHEP::HepLorentzVector const & qH, // t-channel momentum before Higgs
CLHEP::HepLorentzVector const & qHp1, // t-channel momentum after Higgs
double mt, bool include_bottom, double mb
){
if (bptype==21&&aptype!=21) {
if (aptype > 0)
return jM2unobgHQg(pn,pb,punob,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
else
return jM2unobgHQbarg(pn,pb,punob,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
}
else { // they are both quark
if (aptype>0) {
if (bptype>0)
return jM2unobqHQg(pn,pb,punob,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
else
return jM2unobqbarHQg(pn,pb,punob,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
}
else {
if (bptype>0)
return jM2unobqHQbarg(pn,pb,punob,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
else
return jM2unobqbarHQbarg(pn,pb,punob,p1,pa,-qHp1,-qH,mt,include_bottom,mb);
}
}
throw std::logic_error("unknown particle types");
}
CLHEP::HepLorentzVector to_HepLorentzVector(HEJ::Particle const & particle){
return {particle.p.px(), particle.p.py(), particle.p.pz(), particle.p.E()};
}
void validate(HEJ::MatrixElementConfig const & config) {
#ifndef HEJ_BUILD_WITH_QCDLOOP
if(!config.Higgs_coupling.use_impact_factors) {
throw std::invalid_argument{
"Invalid Higgs coupling settings.\n"
"HEJ without QCDloop support can only use impact factors.\n"
"Set use_impact_factors to true or recompile HEJ.\n"
};
}
#endif
if(config.Higgs_coupling.use_impact_factors
&& config.Higgs_coupling.mt != std::numeric_limits<double>::infinity()) {
throw std::invalid_argument{
"Conflicting settings: "
"impact factors may only be used in the infinite top mass limit"
};
}
}
} // namespace anonymous
namespace HEJ{
MatrixElement::MatrixElement(
std::function<double (double)> alpha_s,
MatrixElementConfig conf
):
alpha_s_{std::move(alpha_s)},
param_{std::move(conf)}
{
validate(param_);
}
double MatrixElement::tree_kin(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const {
+ if(! is_HEJ(ev.type())) return 0.;
auto AWZH_boson = std::find_if(
begin(ev.outgoing()), end(ev.outgoing()),
[](Particle const & p){return is_AWZH_boson(p);}
);
if(AWZH_boson == end(ev.outgoing())){
- return tree_kin_jets(ev, check_momenta);
+ return tree_kin_jets(ev);
}
switch(AWZH_boson->type){
case pid::Higgs: {
- return tree_kin_Higgs(ev, check_momenta);
+ return tree_kin_Higgs(ev);
}
// TODO
case pid::Wp: {
- return tree_kin_W(ev, true, check_momenta);
+ return tree_kin_W(ev, true);
}
case pid::Wm: {
- return tree_kin_W(ev, false, check_momenta);
+ return tree_kin_W(ev, false);
}
case pid::photon:
case pid::Z:
default:
throw not_implemented("Emission of boson of unsupported type");
}
}
namespace{
constexpr int extremal_jet_idx = 1;
constexpr int no_extremal_jet_idx = 0;
bool treat_as_extremal(Particle const & parton){
return parton.p.user_index() == extremal_jet_idx;
}
template<class InputIterator>
double FKL_ladder_weight(
InputIterator begin_gluon, InputIterator end_gluon,
CLHEP::HepLorentzVector const & q0,
CLHEP::HepLorentzVector const & pa, CLHEP::HepLorentzVector const & pb,
CLHEP::HepLorentzVector const & p1, CLHEP::HepLorentzVector const & pn
){
double wt = 1;
auto qi = q0;
for(auto gluon_it = begin_gluon; gluon_it != end_gluon; ++gluon_it){
assert(gluon_it->type == pid::gluon);
const auto g = to_HepLorentzVector(*gluon_it);
const auto qip1 = qi - g;
if(treat_as_extremal(*gluon_it)){
wt *= C2Lipatovots(qip1, qi, pa, pb)*C_A;
} else{
wt *= C2Lipatovots(qip1, qi, pa, pb, p1, pn)*C_A;
}
qi = qip1;
}
return wt;
}
} // namespace anonymous
std::vector<Particle> MatrixElement::tag_extremal_jet_partons(
- Event const & ev, bool check_momenta
+ Event const & ev
) const{
auto out_partons = filter_partons(ev.outgoing());
- if(!check_momenta){
+ if(out_partons.size() == ev.jets().size()){
+ // no additional emissions in extremal jets, don't need to tag anything
for(auto & parton: out_partons){
parton.p.set_user_index(no_extremal_jet_idx);
}
return out_partons;
}
// TODO: avoid reclustering
fastjet::ClusterSequence cs(to_PseudoJet(out_partons), ev.jet_def());
const auto jets = sorted_by_rapidity(cs.inclusive_jets(ev.min_jet_pt()));
assert(jets.size() >= 2);
auto most_backward = begin(jets);
auto most_forward = end(jets) - 1;
// skip jets caused by unordered emission or qqx
if(ev.type() == event_type::unob || ev.type() == event_type::qqxexb){
assert(jets.size() >= 3);
++most_backward;
}
else if(ev.type() == event_type::unof || ev.type() == event_type::qqxexf){
assert(jets.size() >= 3);
--most_forward;
}
const auto extremal_jet_indices = cs.particle_jet_indices(
{*most_backward, *most_forward}
);
assert(extremal_jet_indices.size() == out_partons.size());
for(size_t i = 0; i < out_partons.size(); ++i){
assert(HEJ::is_parton(out_partons[i]));
const int idx = (extremal_jet_indices[i]>=0)?
extremal_jet_idx:
no_extremal_jet_idx;
out_partons[i].p.set_user_index(idx);
}
return out_partons;
}
double MatrixElement::tree_kin_jets(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const {
auto const & incoming = ev.incoming();
- const auto partons = tag_extremal_jet_partons(ev, check_momenta);
+ const auto partons = tag_extremal_jet_partons(ev);
if(is_uno(ev.type())){
throw not_implemented("unordered emission not implemented for pure jets");
}
const auto pa = to_HepLorentzVector(incoming[0]);
const auto pb = to_HepLorentzVector(incoming[1]);
const auto p1 = to_HepLorentzVector(partons.front());
const auto pn = to_HepLorentzVector(partons.back());
return ME_current(
incoming[0].type, incoming[1].type,
pn, pb, p1, pa
)/(4*(N_C*N_C - 1))*FKL_ladder_weight(
begin(partons) + 1, end(partons) - 1,
pa - p1, pa, pb, p1, pn
);
}
namespace{
double tree_kin_W_FKL(
int aptype, int bptype, HLV pa, HLV pb,
std::vector<Particle> const & partons,
HLV plbar, HLV pl, bool WPlus
) {
auto p1 = to_HepLorentzVector(partons[0]);
auto pn = to_HepLorentzVector(partons[partons.size() - 1]);
auto q0 = pa - p1;
auto begin_ladder = begin(partons) + 1;
auto end_ladder = end(partons) - 1;
bool wc;
if (aptype==partons[0].type) { //leg b emits w
wc = true;
}
else{
wc = false;
q0 -=pl + plbar;
}
double current_factor;
if (WPlus){
current_factor = ME_W_current(
aptype, bptype, pn, pb,
p1, pa, pl, plbar, wc
);
}
else{
current_factor = ME_W_current(
aptype, bptype, pn, pb,
p1, pa, plbar, pl, wc
);
}
const double ladder_factor = FKL_ladder_weight(
begin_ladder, end_ladder,
q0, pa, pb, p1, pn
);
return current_factor*C_A*C_A/(N_C*N_C-1.)*ladder_factor;
}
double tree_kin_W_unob(
int aptype, int bptype, HLV pa, HLV pb,
std::vector<Particle> const & partons,
HLV plbar, HLV pl, bool WPlus
) {
auto pg = to_HepLorentzVector(partons[0]);
auto p1 = to_HepLorentzVector(partons[1]);
auto pn = to_HepLorentzVector(partons[partons.size() - 1]);
auto q0 = pa - p1- pg;
auto begin_ladder = begin(partons) + 2;
auto end_ladder = end(partons) - 1;
bool wc;
if (aptype==partons[1].type) { //leg b emits w
wc = true;
}
else{
wc = false;
q0 -=pl + plbar;
}
double current_factor;
if (WPlus){
current_factor = ME_W_unob_current(
aptype, bptype, pn, pb,
p1, pa, pg, pl, plbar, wc
);
}
else{
current_factor = ME_W_unob_current(
aptype, bptype, pn, pb,
p1, pa, pg, plbar, pl, wc
);
}
const double ladder_factor = FKL_ladder_weight(
begin_ladder, end_ladder,
q0, pa, pb, p1, pn
);
return current_factor*C_A*C_A/(N_C*N_C-1.)*ladder_factor;
}
double tree_kin_W_unof(
int aptype, int bptype, HLV pa, HLV pb,
std::vector<Particle> const & partons,
HLV plbar, HLV pl, bool WPlus
) {
auto p1 = to_HepLorentzVector(partons[0]);
auto pn = to_HepLorentzVector(partons[partons.size() - 2]);
auto pg = to_HepLorentzVector(partons[partons.size() - 1]);
auto q0 = pa - p1;
auto begin_ladder = begin(partons) + 1;
auto end_ladder = end(partons) - 2;
bool wc;
if (aptype==partons[0].type) { //leg b emits w
wc = true;}
else{
wc = false;
q0 -=pl + plbar;
}
double current_factor;
if (WPlus){
current_factor = ME_W_unof_current(
aptype, bptype, pn, pb,
p1, pa, pg, pl, plbar, wc
);
}
else{
current_factor = ME_W_unof_current(
aptype, bptype, pn, pb,
p1, pa, pg, plbar, pl, wc
);
}
const double ladder_factor = FKL_ladder_weight(
begin_ladder, end_ladder,
q0, pa, pb, p1, pn
);
return current_factor*C_A*C_A/(N_C*N_C-1.)*ladder_factor;
}
double tree_kin_W_qqxb(
int aptype, int bptype, HLV pa, HLV pb,
std::vector<Particle> const & partons,
HLV plbar, HLV pl, bool WPlus
) {
HLV pq,pqbar;
if(is_quark(partons[0])){
pq = to_HepLorentzVector(partons[0]);
pqbar = to_HepLorentzVector(partons[1]);
}
else{
pq = to_HepLorentzVector(partons[1]);
pqbar = to_HepLorentzVector(partons[0]);
}
auto p1 = to_HepLorentzVector(partons[0]);
auto pn = to_HepLorentzVector(partons[partons.size() - 1]);
auto q0 = pa - pq - pqbar;
auto begin_ladder = begin(partons) + 2;
auto end_ladder = end(partons) - 1;
bool wc;
if (partons[0].type==-partons[1].type) { //leg b emits w
wc = true;}
else{
wc = false;
q0 -=pl + plbar;
}
double current_factor;
if (WPlus){
current_factor = ME_W_qqxb_current(
aptype, bptype, pa, pb,
pq, pqbar, pn, pl, plbar, wc
);
}
else{
current_factor = ME_W_qqxb_current(
aptype, bptype, pa, pb,
pq, pqbar, pn, plbar, pl, wc
);
}
const double ladder_factor = FKL_ladder_weight(
begin_ladder, end_ladder,
q0, pa, pb, p1, pn
);
return current_factor*C_A*C_A/(N_C*N_C-1.)*ladder_factor;
}
double tree_kin_W_qqxf(
int aptype, int bptype, HLV pa, HLV pb,
std::vector<Particle> const & partons,
HLV plbar, HLV pl, bool WPlus
) {
HLV pq,pqbar;
if(is_quark(partons[partons.size() - 1])){
pq = to_HepLorentzVector(partons[partons.size() - 1]);
pqbar = to_HepLorentzVector(partons[partons.size() - 2]);
}
else{
pq = to_HepLorentzVector(partons[partons.size() - 2]);
pqbar = to_HepLorentzVector(partons[partons.size() - 1]);
}
auto p1 = to_HepLorentzVector(partons[0]);
auto pn = to_HepLorentzVector(partons[partons.size() - 1]);
auto q0 = pa - p1;
auto begin_ladder = begin(partons) + 1;
auto end_ladder = end(partons) - 2;
bool wc;
if (aptype==partons[0].type) { //leg b emits w
wc = true;}
else{
wc = false;
q0 -=pl + plbar;
}
double current_factor;
if (WPlus){
current_factor = ME_W_qqxf_current(
aptype, bptype, pa, pb,
pq, pqbar, p1, pl, plbar, wc
);
}
else{
current_factor = ME_W_qqxf_current(
aptype, bptype, pa, pb,
pq, pqbar, p1, plbar, pl, wc
);
}
const double ladder_factor = FKL_ladder_weight(
begin_ladder, end_ladder,
q0, pa, pb, p1, pn
);
return current_factor*C_A*C_A/(N_C*N_C-1.)*ladder_factor;
}
double tree_kin_W_qqxmid(
int aptype, int bptype, HLV pa, HLV pb,
std::vector<Particle> const & partons,
HLV plbar, HLV pl, bool WPlus
) {
HLV pq,pqbar;
const auto backmidquark = std::find_if(
begin(partons)+1, end(partons)-1,
[](Particle const & s){ return s.type != pid::gluon; }
);
if (is_quark(backmidquark->type)){
pq = to_HepLorentzVector(*backmidquark);
pqbar = to_HepLorentzVector(*(backmidquark+1));
}
else {
pqbar = to_HepLorentzVector(*backmidquark);
pq = to_HepLorentzVector(*(backmidquark+1));
}
auto p1 = to_HepLorentzVector(partons[0]);
auto pn = to_HepLorentzVector(partons[partons.size() - 1]);
auto q0 = pa - p1;
// t-channel momentum after qqx
auto qqxt = q0;
bool wc, wqq;
if (backmidquark->type == -(backmidquark+1)->type){ // Central qqx does not emit
wqq=false;
if (aptype==partons[0].type) {
wc = true;
}
else{
wc = false;
q0-=pl+plbar;
}
}
else{
wqq = true;
wc = false;
qqxt-=pl+plbar;
}
auto begin_ladder = begin(partons) + 1;
auto end_ladder_1 = (backmidquark);
auto begin_ladder_2 = (backmidquark+2);
auto end_ladder = end(partons) - 1;
for(auto parton_it = begin_ladder; parton_it < begin_ladder_2; ++parton_it){
qqxt -= to_HepLorentzVector(*parton_it);
}
int nabove = std::distance(begin_ladder, backmidquark);
int nbelow = std::distance(begin_ladder_2, end_ladder);
std::vector<HLV> partonsHLV;
partonsHLV.reserve(partons.size());
for (size_t i = 0; i != partons.size(); ++i) {
partonsHLV.push_back(to_HepLorentzVector(partons[i]));
}
double current_factor;
if (WPlus){
current_factor = ME_W_qqxmid_current(
aptype, bptype, nabove, nbelow, pa, pb,
pq, pqbar, partonsHLV, pl, plbar, wqq, wc
);
}
else{
current_factor = ME_W_qqxmid_current(
aptype, bptype, nabove, nbelow, pa, pb,
pq, pqbar, partonsHLV, plbar, pl, wqq, wc
);
}
const double ladder_factor = FKL_ladder_weight(
begin_ladder, end_ladder_1,
q0, pa, pb, p1, pn
)*FKL_ladder_weight(
begin_ladder_2, end_ladder,
qqxt, pa, pb, p1, pn
);
return current_factor*C_A*C_A/(N_C*N_C-1.)*ladder_factor;
}
} // namespace anonymous
double MatrixElement::tree_kin_W(
Event const & ev,
- bool WPlus,
- bool check_momenta
+ bool WPlus
) const {
using namespace event_type;
auto const & incoming(ev.incoming());
auto const & outgoing(ev.outgoing());
auto const & decays(ev.decays());
HLV plbar, pl;
for (auto& x: decays) {
if (x.second.at(0).type < 0){
plbar = to_HepLorentzVector(x.second.at(0));
pl = to_HepLorentzVector(x.second.at(1));
}
else{
pl = to_HepLorentzVector(x.second.at(0));
plbar = to_HepLorentzVector(x.second.at(1));
}
}
const auto pa = to_HepLorentzVector(incoming[0]);
const auto pb = to_HepLorentzVector(incoming[1]);
const auto the_W = std::find_if(
begin(outgoing), end(outgoing),
[](Particle const & s){ return abs(s.type) == pid::Wp; }
);
std::vector<Particle> partons(begin(outgoing), the_W);
partons.insert(end(partons), the_W + 1, end(outgoing));
- partons = tag_extremal_jet_partons(ev, check_momenta);
if(ev.type() == unordered_backward){
return tree_kin_W_unob(incoming[0].type, incoming[1].type,
pa, pb, partons, plbar, pl, WPlus);
}
if(ev.type() == unordered_forward){
return tree_kin_W_unof(incoming[0].type, incoming[1].type,
pa, pb, partons, plbar, pl, WPlus);
}
if(ev.type() == extremal_qqxb){
return tree_kin_W_qqxb(incoming[0].type, incoming[1].type,
pa, pb, partons, plbar, pl, WPlus);
}
if(ev.type() == extremal_qqxf){
return tree_kin_W_qqxf(incoming[0].type, incoming[1].type,
pa, pb, partons, plbar, pl, WPlus);
}
if(ev.type() == central_qqx){
return tree_kin_W_qqxmid(incoming[0].type, incoming[1].type,
pa, pb, partons, plbar, pl, WPlus);
}
return tree_kin_W_FKL(incoming[0].type, incoming[1].type,
pa, pb, partons, plbar, pl, WPlus);
}
double MatrixElement::tree_kin_Higgs(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const {
if(is_uno(ev.type())){
- return tree_kin_Higgs_between(ev, check_momenta);
+ return tree_kin_Higgs_between(ev);
}
if(ev.outgoing().front().type == pid::Higgs){
- return tree_kin_Higgs_first(ev, check_momenta);
+ return tree_kin_Higgs_first(ev);
}
if(ev.outgoing().back().type == pid::Higgs){
- return tree_kin_Higgs_last(ev, check_momenta);
+ return tree_kin_Higgs_last(ev);
}
- return tree_kin_Higgs_between(ev, check_momenta);
+ return tree_kin_Higgs_between(ev);
}
namespace {
// Colour acceleration multipliers, for gluons see eq. (7) in arXiv:0910.5113
// TODO: code duplication with currents.cc
double K_g(double p1minus, double paminus) {
return 1./2.*(p1minus/paminus + paminus/p1minus)*(C_A - 1./C_A) + 1./C_A;
}
double K_g(
CLHEP::HepLorentzVector const & pout,
CLHEP::HepLorentzVector const & pin
) {
if(pin.z() > 0) return K_g(pout.plus(), pin.plus());
return K_g(pout.minus(), pin.minus());
}
double K(
ParticleID type,
CLHEP::HepLorentzVector const & pout,
CLHEP::HepLorentzVector const & pin
) {
if(type == ParticleID::gluon) return K_g(pout, pin);
return C_F;
}
// Colour factor in strict MRK limit
double K_MRK(ParticleID type) {
return (type == ParticleID::gluon)?C_A:C_F;
}
}
double MatrixElement::MH2_forwardH(
CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
ParticleID type2,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector pH,
double t1, double t2
) const{
ignore(p2out, p2in);
const double shat = p1in.invariantMass2(p2in);
// gluon case
#ifdef HEJ_BUILD_WITH_QCDLOOP
if(!param_.Higgs_coupling.use_impact_factors){
return K(type2, p2out, p2in)*C_A*1./(16*M_PI*M_PI)*t1/t2*MH2gq_outsideH(
p1out, p1in, p2out, p2in, pH,
param_.Higgs_coupling.mt, param_.Higgs_coupling.include_bottom,
param_.Higgs_coupling.mb
)/(4*(N_C*N_C - 1));
}
#endif
return K_MRK(type2)/C_A*9./2.*shat*shat*(
C2gHgp(p1in,p1out,pH) + C2gHgm(p1in,p1out,pH)
)/(t1*t2);
}
double MatrixElement::tree_kin_Higgs_first(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const {
auto const & incoming = ev.incoming();
auto const & outgoing = ev.outgoing();
assert(outgoing.front().type == pid::Higgs);
if(outgoing[1].type != pid::gluon) {
assert(incoming.front().type == outgoing[1].type);
- return tree_kin_Higgs_between(ev, check_momenta);
+ return tree_kin_Higgs_between(ev);
}
const auto pH = to_HepLorentzVector(outgoing.front());
const auto partons = tag_extremal_jet_partons(
- ev, check_momenta
+ ev
);
const auto pa = to_HepLorentzVector(incoming[0]);
const auto pb = to_HepLorentzVector(incoming[1]);
const auto p1 = to_HepLorentzVector(partons.front());
const auto pn = to_HepLorentzVector(partons.back());
const auto q0 = pa - p1 - pH;
const double t1 = q0.m2();
const double t2 = (pn - pb).m2();
return MH2_forwardH(
p1, pa, incoming[1].type, pn, pb, pH,
t1, t2
)*FKL_ladder_weight(
begin(partons) + 1, end(partons) - 1,
q0, pa, pb, p1, pn
);
}
double MatrixElement::tree_kin_Higgs_last(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const {
auto const & incoming = ev.incoming();
auto const & outgoing = ev.outgoing();
assert(outgoing.back().type == pid::Higgs);
if(outgoing[outgoing.size()-2].type != pid::gluon) {
assert(incoming.back().type == outgoing[outgoing.size()-2].type);
- return tree_kin_Higgs_between(ev, check_momenta);
+ return tree_kin_Higgs_between(ev);
}
const auto pH = to_HepLorentzVector(outgoing.back());
const auto partons = tag_extremal_jet_partons(
- ev, check_momenta
+ ev
);
const auto pa = to_HepLorentzVector(incoming[0]);
const auto pb = to_HepLorentzVector(incoming[1]);
auto p1 = to_HepLorentzVector(partons.front());
const auto pn = to_HepLorentzVector(partons.back());
auto q0 = pa - p1;
const double t1 = q0.m2();
const double t2 = (pn + pH - pb).m2();
return MH2_forwardH(
pn, pb, incoming[0].type, p1, pa, pH,
t2, t1
)*FKL_ladder_weight(
begin(partons) + 1, end(partons) - 1,
q0, pa, pb, p1, pn
);
}
double MatrixElement::tree_kin_Higgs_between(
- Event const & ev,
- bool check_momenta
+ Event const & ev
) const {
using namespace event_type;
auto const & incoming = ev.incoming();
auto const & outgoing = ev.outgoing();
const auto the_Higgs = std::find_if(
begin(outgoing), end(outgoing),
[](Particle const & s){ return s.type == pid::Higgs; }
);
assert(the_Higgs != end(outgoing));
const auto pH = to_HepLorentzVector(*the_Higgs);
- const auto partons = tag_extremal_jet_partons(ev, check_momenta);
+ const auto partons = tag_extremal_jet_partons(ev);
const auto pa = to_HepLorentzVector(incoming[0]);
const auto pb = to_HepLorentzVector(incoming[1]);
auto p1 = to_HepLorentzVector(
partons[(ev.type() == unob)?1:0]
);
auto pn = to_HepLorentzVector(
partons[partons.size() - ((ev.type() == unof)?2:1)]
);
auto first_after_Higgs = begin(partons) + (the_Higgs-begin(outgoing));
assert(
(first_after_Higgs == end(partons) && (
(ev.type() == unob)
|| partons.back().type != pid::gluon
))
|| first_after_Higgs->rapidity() >= the_Higgs->rapidity()
);
assert(
(first_after_Higgs == begin(partons) && (
(ev.type() == unof)
|| partons.front().type != pid::gluon
))
|| (first_after_Higgs-1)->rapidity() <= the_Higgs->rapidity()
);
// always treat the Higgs as if it were in between the extremal FKL partons
if(first_after_Higgs == begin(partons)) ++first_after_Higgs;
else if(first_after_Higgs == end(partons)) --first_after_Higgs;
// t-channel momentum before Higgs
auto qH = pa;
for(auto parton_it = begin(partons); parton_it != first_after_Higgs; ++parton_it){
qH -= to_HepLorentzVector(*parton_it);
}
auto q0 = pa - p1;
auto begin_ladder = begin(partons) + 1;
auto end_ladder = end(partons) - 1;
double current_factor;
if(ev.type() == unob){
current_factor = C_A*C_A/2.*ME_Higgs_current_unob( // 1/2 = "K_uno"
incoming[0].type, incoming[1].type,
pn, pb, to_HepLorentzVector(partons.front()), p1, pa, qH, qH - pH,
param_.Higgs_coupling.mt,
param_.Higgs_coupling.include_bottom, param_.Higgs_coupling.mb
);
const auto p_unob = to_HepLorentzVector(partons.front());
q0 -= p_unob;
p1 += p_unob;
++begin_ladder;
}
else if(ev.type() == unof){
current_factor = C_A*C_A/2.*ME_Higgs_current_unof( // 1/2 = "K_uno"
incoming[0].type, incoming[1].type,
- to_HepLorentzVector(partons.back()), pn, pb, p1, pa, qH, qH - pH,
+ to_HepLorentzVector(partons.back()), pn, pb, p1, pa, qH, qH - pH,
param_.Higgs_coupling.mt,
param_.Higgs_coupling.include_bottom, param_.Higgs_coupling.mb
);
pn += to_HepLorentzVector(partons.back());
--end_ladder;
}
else{
current_factor = ME_Higgs_current(
incoming[0].type, incoming[1].type,
pn, pb, p1, pa, qH, qH - pH,
param_.Higgs_coupling.mt,
param_.Higgs_coupling.include_bottom, param_.Higgs_coupling.mb
);
}
const double ladder_factor = FKL_ladder_weight(
begin_ladder, first_after_Higgs,
q0, pa, pb, p1, pn
)*FKL_ladder_weight(
first_after_Higgs, end_ladder,
qH - pH, pa, pb, p1, pn
);
return current_factor*C_A*C_A/(N_C*N_C-1.)*ladder_factor;
}
double MatrixElement::tree_param_partons(
double alpha_s, double mur,
std::vector<Particle> const & partons
) const{
const double gs2 = 4.*M_PI*alpha_s;
double wt = std::pow(gs2, partons.size());
if(param_.log_correction){
// use alpha_s(q_perp), evolved to mur
assert(partons.size() >= 2);
for(size_t i = 1; i < partons.size()-1; ++i){
wt *= 1 + alpha_s/(2*M_PI)*beta0*log(mur/partons[i].p.perp());
}
}
return wt;
}
double MatrixElement::tree_param(
Event const & ev,
double mur
) const{
assert(is_HEJ(ev.type()));
const auto & out = ev.outgoing();
const double alpha_s = alpha_s_(mur);
auto AWZH_boson = std::find_if(
begin(out), end(out),
[](auto const & p){return is_AWZH_boson(p);}
);
double AWZH_coupling = 1.;
if(AWZH_boson != end(out)){
switch(AWZH_boson->type){
case pid::Higgs: {
AWZH_coupling = alpha_s*alpha_s;
break;
}
// TODO
case pid::Wp:{
AWZH_coupling = gw*gw*gw*gw/4;
break;
}
case pid::Wm:{
AWZH_coupling = gw*gw*gw*gw/4;
break;
}
case pid::photon:
case pid::Z:
default:
throw not_implemented("Emission of boson of unsupported type");
}
}
if(ev.type() == event_type::unob || ev.type() == event_type::qqxexb){
return AWZH_coupling*4*M_PI*alpha_s*tree_param_partons(
alpha_s, mur, filter_partons({begin(out) + 1, end(out)})
);
}
if(ev.type() == event_type::unof || ev.type() == event_type::qqxexf){
return AWZH_coupling*4*M_PI*alpha_s*tree_param_partons(
alpha_s, mur, filter_partons({begin(out), end(out) - 1})
);
}
return AWZH_coupling*tree_param_partons(alpha_s, mur, filter_partons(out));
}
} // namespace HEJ
diff --git a/src/PDF.cc b/src/PDF.cc
index feeee8a..3a82e18 100644
--- a/src/PDF.cc
+++ b/src/PDF.cc
@@ -1,113 +1,112 @@
/**
- * \file PDF.cc
- * Author: Tuomas Hapola
- * \brief PDF source file
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
+#include "HEJ/PDF.hh"
+#include <iostream>
#include <stdexcept>
#include <string>
-#include "HEJ/PDF.hh"
-#include "HEJ/PDG_codes.hh"
-
namespace HEJ{
namespace{
int to_beam(ParticleID id){
if(std::abs(id) == pid::proton){
return (id > 0)?1:-1;
}
throw std::invalid_argument(
"unknown beam type: " + std::to_string(id)
);
}
}
#if defined LHAPDF_MAJOR_VERSION && LHAPDF_MAJOR_VERSION == 6
PDF::PDF(int id, ParticleID beam1, ParticleID beam2):
pdf{LHAPDF::mkPDF(id)},
beamtype{{to_beam(beam1), to_beam(beam2)}}
{}
double PDF::pdfpt(size_t beam_idx, double x, double q, ParticleID id) const{
if(!(inRangeQ(q) && inRangeX(x))) return 0.;
if(id == pid::gluon){
return pdf->xfxQ(21,x,q);
}
else if(abs(id) < 7){
return pdf->xfxQ(id*beamtype[beam_idx],x,q);
}
else {
std::cerr << "particle type unknown: "<< id << std::endl;
return 0.0;
}
}
double PDF::Halphas(double q) const{
double as = pdf->alphasQ(q);
if (std::isnan(as) || as > 0.5) {
as = 0.5;
}
return as;
}
int PDF::id() const{
return pdf->lhapdfID();
};
bool PDF::inRangeQ(double q) const{
return pdf->inRangeQ(q);
}
bool PDF::inRangeX(double x) const{
return pdf->inRangeX(x);
}
#else /* LHAPDF version unknown or older than 6 */
PDF::PDF(std::string LHAPDFName, int LHAPDFsubset, ParticleID beam1, ParticleID beam2):
beamtype{{to_beam(beam1_type), to_beam(beam2_type)}}
{
LHAPDF::initPDFSet(LHAPDFName, LHAPDF::LHGRID, LHAPDFsubset);
}
double PDF::pdfpt(size_t beam_idx, double x, double q, ParticleID id) const{
if(!(inRangeQ(q) && inRangeX(x))) return 0.;
if (id == pid::gluon){
return LHAPDF::xfx(x,q,0);
}
else if (abs(id) < 7){
return LHAPDF::xfx(x,q,id*beamtype[beam_idx]);
}
else {
std::cerr << "particle type unknown: "<< id <<std::endl;
return 0.0;
}
}
double PDF::Halphas(double q) const{
double as = LHAPDF::alphasPDF(q);
if (isnan(as) || as > 0.5) as = 0.5;
return as;
}
bool PDF::inRangeQ(double q) const{
// here we assume that all members actually have the same range!
static constexpr int member = 0;
return (LHAPDF::getQ2min(member) < q*q) && (q*q < LHAPDF::getQ2max(member));
}
bool PDF::inRangeX(double x) const{
// here we assume that all members actually have the same range!
static constexpr int member = 0;
return (LHAPDF::getXmin(member) < x) && (x < LHAPDF::getXmax(member));
}
#endif
}
diff --git a/src/PDG_codes.cc b/src/PDG_codes.cc
index 6dc9379..e453c57 100644
--- a/src/PDG_codes.cc
+++ b/src/PDG_codes.cc
@@ -1,48 +1,54 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/PDG_codes.hh"
#include <map>
-#include <iostream>
+
+#include "HEJ/exceptions.hh"
namespace HEJ{
ParticleID to_ParticleID(std::string const & name){
using namespace HEJ::pid;
static const std::map<std::string, ParticleID> known = {
{"d", d}, {"down", down}, {"1",static_cast<ParticleID>(1)},
{"u", u}, {"up", up}, {"2",static_cast<ParticleID>(2)},
{"s", s}, {"strange", strange}, {"3",static_cast<ParticleID>(3)},
{"c", c}, {"charm", charm}, {"4",static_cast<ParticleID>(4)},
{"b", b}, {"bottom", bottom}, {"5",static_cast<ParticleID>(5)},
{"t", t}, {"top", top}, {"6",static_cast<ParticleID>(6)},
{"e", e}, {"electron", electron}, {"e-", e}, {"11",static_cast<ParticleID>(11)},
{"nu_e", nu_e}, {"electron_neutrino", electron_neutrino}, {"12",static_cast<ParticleID>(12)},
{"mu", mu}, {"muon", muon}, {"mu-", mu}, {"13",static_cast<ParticleID>(13)},
{"nu_mu", nu_mu}, {"muon_neutrino", muon_neutrino}, {"14",static_cast<ParticleID>(14)},
{"tau", tau}, {"tau-", tau}, {"15",static_cast<ParticleID>(15)},
{"nu_tau", nu_tau}, {"tau_neutrino", tau_neutrino}, {"16",static_cast<ParticleID>(16)},
{"d_bar", d_bar}, {"-1",static_cast<ParticleID>(-1)},
{"u_bar", u_bar}, {"-2",static_cast<ParticleID>(-2)},
{"s_bar", s_bar}, {"-3",static_cast<ParticleID>(-3)},
{"c_bar", c_bar}, {"-4",static_cast<ParticleID>(-4)},
{"b_bar", b_bar}, {"-5",static_cast<ParticleID>(-5)},
{"t_bar", t_bar}, {"-6",static_cast<ParticleID>(-6)},
{"e_bar", e_bar}, {"positron", positron}, {"e+", e_bar}, {"-11",static_cast<ParticleID>(-11)},
{"nu_e_bar", nu_e_bar}, {"-12",static_cast<ParticleID>(-12)},
{"mu_bar", mu_bar}, {"mu+", mu_bar}, {"-13",static_cast<ParticleID>(-13)},
{"nu_mu_bar", nu_mu_bar}, {"-14",static_cast<ParticleID>(-14)},
{"tau_bar", tau_bar}, {"tau+", tau_bar}, {"-15",static_cast<ParticleID>(-15)},
{"nu_tau_bar", nu_tau_bar}, {"-16",static_cast<ParticleID>(-16)},
{"gluon", gluon}, {"g", g}, {"21",static_cast<ParticleID>(21)},
{"photon", photon}, {"gamma", gamma}, {"22",static_cast<ParticleID>(22)},
{"Z", Z}, {"23",static_cast<ParticleID>(23)},
{"Wp", Wp}, {"W+", Wp}, {"24",static_cast<ParticleID>(24)},
{"Wm", Wm}, {"W-", Wm}, {"-24",static_cast<ParticleID>(-24)},
{"h", h}, {"H", h}, {"Higgs", Higgs}, {"higgs", higgs}, {"25",static_cast<ParticleID>(25)},
{"p", p}, {"proton", proton}, {"p_bar", p_bar}, {"2212",static_cast<ParticleID>(2212)}
};
const auto res = known.find(name);
if(res == known.end()){
throw std::invalid_argument("Unknown particle " + name);
}
return res->second;
}
}
diff --git a/src/PhaseSpacePoint.cc b/src/PhaseSpacePoint.cc
index 6dde61a..1d581f3 100644
--- a/src/PhaseSpacePoint.cc
+++ b/src/PhaseSpacePoint.cc
@@ -1,614 +1,625 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/PhaseSpacePoint.hh"
+#include <algorithm>
+#include <assert.h>
+#include <numeric>
#include <random>
-#include <CLHEP/Random/Randomize.h>
-#include <CLHEP/Random/RanluxEngine.h>
+#include "fastjet/ClusterSequence.hh"
#include "HEJ/Constants.hh"
+#include "HEJ/Event.hh"
+#include "HEJ/JetSplitter.hh"
+#include "HEJ/kinematics.hh"
#include "HEJ/resummation_jet.hh"
#include "HEJ/utility.hh"
-#include "HEJ/kinematics.hh"
+#include "HEJ/PDG_codes.hh"
+#include "HEJ/event_types.hh"
namespace HEJ{
namespace {
constexpr int max_jet_user_idx = PhaseSpacePoint::ng_max;
bool is_nonjet_parton(fastjet::PseudoJet const & parton){
assert(parton.user_index() != -1);
return parton.user_index() > max_jet_user_idx;
}
bool is_jet_parton(fastjet::PseudoJet const & parton){
assert(parton.user_index() != -1);
return parton.user_index() <= max_jet_user_idx;
}
// user indices for partons with extremal rapidity
constexpr int qqxb_idx = -7;
constexpr int qqxf_idx = -6;
constexpr int unob_idx = -5;
constexpr int unof_idx = -4;
constexpr int backward_FKL_idx = -3;
constexpr int forward_FKL_idx = -2;
}
namespace {
double estimate_ng_mean(std::vector<fastjet::PseudoJet> const & Born_jets){
const double delta_y =
Born_jets.back().rapidity() - Born_jets.front().rapidity();
assert(delta_y > 0);
// Formula derived from fit in arXiv:1805.04446 (see Fig. 2)
return 0.975052*delta_y;
}
}
std::vector<fastjet::PseudoJet> PhaseSpacePoint::cluster_jets(
std::vector<fastjet::PseudoJet> const & partons
) const{
fastjet::ClusterSequence cs(partons, param_.jet_param.def);
return cs.inclusive_jets(param_.jet_param.min_pt);
}
bool PhaseSpacePoint::pass_resummation_cuts(
std::vector<fastjet::PseudoJet> const & jets
) const{
return cluster_jets(jets).size() == jets.size();
}
int PhaseSpacePoint::sample_ng(std::vector<fastjet::PseudoJet> const & Born_jets){
const double ng_mean = estimate_ng_mean(Born_jets);
std::poisson_distribution<int> dist(ng_mean);
const int ng = dist(ran_.get());
assert(ng >= 0);
assert(ng < ng_max);
weight_ *= std::tgamma(ng + 1)*std::exp(ng_mean)*std::pow(ng_mean, -ng);
return ng;
}
void PhaseSpacePoint::copy_AWZH_boson_from(Event const & event){
auto const & from = event.outgoing();
const auto AWZH_boson = std::find_if(
begin(from), end(from),
[](Particle const & p){ return is_AWZH_boson(p); }
);
if(AWZH_boson == end(from)) return;
auto insertion_point = std::lower_bound(
begin(outgoing_), end(outgoing_), *AWZH_boson, rapidity_less{}
);
outgoing_.insert(insertion_point, *AWZH_boson);
// copy decay products
const int idx = std::distance(begin(from), AWZH_boson);
assert(idx >= 0);
const auto decay_it = event.decays().find(idx);
if(decay_it != end(event.decays())){
const int new_idx = std::distance(begin(outgoing_), insertion_point);
assert(new_idx >= 0);
assert(outgoing_[new_idx].type == AWZH_boson->type);
decays_.emplace(new_idx, decay_it->second);
}
assert(std::is_sorted(begin(outgoing_), end(outgoing_), rapidity_less{}));
}
//! \brief relabels qqx-pair with its PDG IDs.
//*@param ev Born Event
//
// This function will label the qqx pair in a qqx event back to
// their original types from the input event.
void PhaseSpacePoint::label_qqx(Event const & event){
auto const & bornout = event.outgoing();
const auto backquark = std::find_if(
begin(bornout) + 1 - ((qqxb_)?1:0), end(bornout) - 1 + ((qqxf_)?1:0) ,
[](Particle const & s){ return (s.type != pid::gluon && is_parton(s.type)); }
);
assert(backquark->type !=pid::gluon);
if(backquark == end(bornout) || (backquark+1)->type==pid::gluon) weight_= 0;
auto partons = to_PseudoJet(filter_partons(outgoing_));
fastjet::ClusterSequence cs(partons, event.jet_def());
const auto jets = fastjet::sorted_by_rapidity(cs.inclusive_jets(event.min_jet_pt()));
const auto indices = cs.particle_jet_indices({jets});
assert(partons.size() == indices.size());
int qpart=0;
// Find Parton in res event closest to most backward qqx jet in born
for (size_t i=0; i<indices.size(); i++){
if( (indices[i] != -1) && indices[i]!=indices[i+1]
&& nearby_rap(backquark->rapidity(), partons[i].rapidity(), 0.1)){
qpart=i;
}
}
if (indices[qpart] == -1) weight_= 0;
else if (indices[qpart] == 0 && (!qqxb_)) weight_=0;
else if (indices[qpart] == signed(jets.size()-2) && (!qqxf_)) weight_=0;
// Ensure qqx in separate jets and adjacent in rapidity
if (indices[qpart] == indices[qpart+1]-1){
outgoing_.at(qpart).type = backquark->type;
outgoing_.at(qpart+1).type = (backquark+1)->type;
}
else weight_=0;
assert(std::is_sorted(begin(outgoing_), end(outgoing_), rapidity_less{}));
}
PhaseSpacePoint::PhaseSpacePoint(
Event const & ev, PhaseSpacePointConfig conf, HEJ::RNG & ran
):
unob_{ev.type() == event_type::unob},
unof_{ev.type() == event_type::unof},
qqxb_{ev.type() == event_type::qqxexb},
qqxf_{ev.type() == event_type::qqxexf},
qqxmid_{ev.type() == event_type::qqxmid},
param_{std::move(conf)},
ran_{ran}
{
weight_ = 1;
const auto Born_jets = sorted_by_rapidity(ev.jets());
const int ng = sample_ng(Born_jets);
weight_ /= std::tgamma(ng + 1);
const int ng_jets = sample_ng_jets(ng, Born_jets);
std::vector<fastjet::PseudoJet> out_partons = gen_non_jet(
ng - ng_jets, CMINPT, param_.jet_param.min_pt
);
const auto qperp = std::accumulate(
begin(out_partons), end(out_partons),
fastjet::PseudoJet{}
);
const auto jets = reshuffle(Born_jets, qperp);
if(weight_ == 0.) return;
if(! pass_resummation_cuts(jets)){
weight_ = 0.;
return;
}
std::vector<fastjet::PseudoJet> jet_partons = split(jets, ng_jets);
if(weight_ == 0.) return;
rescale_rapidities(
out_partons,
most_backward_FKL(jet_partons).rapidity(),
most_forward_FKL(jet_partons).rapidity()
);
if(! cluster_jets(out_partons).empty()){
weight_ = 0.;
return;
}
std::sort(begin(out_partons), end(out_partons), rapidity_less{});
assert(
std::is_sorted(begin(jet_partons), end(jet_partons), rapidity_less{})
);
const auto first_jet_parton = out_partons.insert(
end(out_partons), begin(jet_partons), end(jet_partons)
);
std::inplace_merge(
begin(out_partons), first_jet_parton, end(out_partons), rapidity_less{}
);
if(! jets_ok(Born_jets, out_partons)){
weight_ = 0.;
return;
}
weight_ *= phase_space_normalisation(Born_jets.size(), out_partons.size());
outgoing_.reserve(out_partons.size() + 1); // one slot for possible A, W, Z, H
for(auto & p: out_partons){
outgoing_.emplace_back(Particle{pid::gluon, std::move(p)});
}
const auto WEmit = std::find_if(
begin(ev.outgoing()), end(ev.outgoing()),
[](Particle const & s){ return abs(s.type) == pid::Wp; }
);
if (abs(WEmit->type) == pid::Wp){
outgoing_[unob_].type = filter_partons(ev.outgoing())[unob_].type;
outgoing_.rbegin()[unof_].type = filter_partons(ev.outgoing()).rbegin()[unof_].type;
}
else{
most_backward_FKL(outgoing_).type = ev.incoming().front().type;
most_forward_FKL(outgoing_).type = ev.incoming().back().type;
}
if(qqxmid_||qqxb_||qqxf_){
label_qqx(ev);
}
copy_AWZH_boson_from(ev);
assert(!outgoing_.empty());
reconstruct_incoming(ev.incoming());
}
std::vector<fastjet::PseudoJet> PhaseSpacePoint::gen_non_jet(
int count, double ptmin, double ptmax
){
// heuristic parameters for pt sampling
const double ptpar = 1.3 + count/5.;
const double temp1 = atan((ptmax - ptmin)/ptpar);
std::vector<fastjet::PseudoJet> partons(count);
for(size_t i = 0; i < (size_t) count; ++i){
const double r1 = ran_.get().flat();
const double pt = ptmin + ptpar*tan(r1*temp1);
const double temp2 = cos(r1*temp1);
const double phi = 2*M_PI*ran_.get().flat();
weight_ *= 2.0*M_PI*pt*ptpar*temp1/(temp2*temp2);
// we don't know the allowed rapidity span yet,
// set a random value to be rescaled later on
const double y = ran_.get().flat();
partons[i].reset_PtYPhiM(pt, y, phi);
// Set user index higher than any jet-parton index
// in order to assert that these are not inside jets
partons[i].set_user_index(i + 1 + ng_max);
assert(ptmin-1e-5 <= partons[i].pt() && partons[i].pt() <= ptmax+1e-5);
}
assert(std::all_of(partons.cbegin(), partons.cend(), is_nonjet_parton));
return partons;
}
void PhaseSpacePoint::rescale_rapidities(
std::vector<fastjet::PseudoJet> & partons,
double ymin, double ymax
){
constexpr double ep = 1e-7;
for(auto & parton: partons){
assert(0 <= parton.rapidity() && parton.rapidity() <= 1);
const double dy = ymax - ymin - 2*ep;
const double y = ymin + ep + dy*parton.rapidity();
parton.reset_momentum_PtYPhiM(parton.pt(), y, parton.phi());
weight_ *= dy;
assert(ymin <= parton.rapidity() && parton.rapidity() <= ymax);
}
}
namespace {
template<typename T, typename... Rest>
auto min(T const & a, T const & b, Rest&&... r) {
using std::min;
return min(a, min(b, std::forward<Rest>(r)...));
}
}
double PhaseSpacePoint::probability_in_jet(
std::vector<fastjet::PseudoJet> const & Born_jets
) const{
assert(std::is_sorted(begin(Born_jets), end(Born_jets), rapidity_less{}));
assert(Born_jets.size() >= 2);
const double dy =
Born_jets.back().rapidity() - Born_jets.front().rapidity();
const double R = param_.jet_param.def.R();
const int njets = Born_jets.size();
const double p_J_y_large = (njets-1)*R*R/(2.*dy);
const double p_J_y0 = njets*R/M_PI;
return min(p_J_y_large, p_J_y0, 1.);
}
int PhaseSpacePoint::sample_ng_jets(
int ng, std::vector<fastjet::PseudoJet> const & Born_jets
){
const double p_J = probability_in_jet(Born_jets);
std::binomial_distribution<> bin_dist(ng, p_J);
const int ng_J = bin_dist(ran_.get());
weight_ *= std::pow(p_J, -ng_J)*std::pow(1 - p_J, ng_J - ng);
return ng_J;
}
std::vector<fastjet::PseudoJet> PhaseSpacePoint::reshuffle(
std::vector<fastjet::PseudoJet> const & Born_jets,
fastjet::PseudoJet const & q
){
if(q == fastjet::PseudoJet{0, 0, 0, 0}) return Born_jets;
const auto jets = resummation_jet_momenta(Born_jets, q);
if(jets.empty()){
weight_ = 0;
return {};
}
// additional Jacobian to ensure Born integration over delta gives 1
weight_ *= resummation_jet_weight(Born_jets, q);
return jets;
}
std::vector<int> PhaseSpacePoint::distribute_jet_partons(
int ng_jets, std::vector<fastjet::PseudoJet> const & jets
){
size_t first_valid_jet = 0;
size_t num_valid_jets = jets.size();
const double R_eff = 5./3.*param_.jet_param.def.R();
// if there is an unordered jet too far away from the FKL jets
// then extra gluon constituents of the unordered jet would
// violate the FKL rapidity ordering
if((unob_||qqxb_) && jets[0].delta_R(jets[1]) > R_eff){
++first_valid_jet;
--num_valid_jets;
}
else if((unof_||qqxf_) && jets[jets.size()-1].delta_R(jets[jets.size()-2]) > R_eff){
--num_valid_jets;
}
std::vector<int> np(jets.size(), 1);
for(int i = 0; i < ng_jets; ++i){
++np[first_valid_jet + ran_.get().flat() * num_valid_jets];
}
weight_ *= std::pow(num_valid_jets, ng_jets);
return np;
}
#ifndef NDEBUG
namespace{
bool tagged_FKL_backward(
std::vector<fastjet::PseudoJet> const & jet_partons
){
return std::find_if(
begin(jet_partons), end(jet_partons),
[](fastjet::PseudoJet const & p){
return p.user_index() == backward_FKL_idx;
}
) != end(jet_partons);
}
bool tagged_FKL_forward(
std::vector<fastjet::PseudoJet> const & jet_partons
){
// the most forward FKL parton is most likely near the end of jet_partons;
// start search from there
return std::find_if(
jet_partons.rbegin(), jet_partons.rend(),
[](fastjet::PseudoJet const & p){
return p.user_index() == forward_FKL_idx;
}
) != jet_partons.rend();
}
bool tagged_FKL_extremal(
std::vector<fastjet::PseudoJet> const & jet_partons
){
return tagged_FKL_backward(jet_partons) && tagged_FKL_forward(jet_partons);
}
} // namespace anonymous
#endif
std::vector<fastjet::PseudoJet> PhaseSpacePoint::split(
std::vector<fastjet::PseudoJet> const & jets,
int ng_jets
){
return split(jets, distribute_jet_partons(ng_jets, jets));
}
bool PhaseSpacePoint::pass_extremal_cuts(
fastjet::PseudoJet const & ext_parton,
fastjet::PseudoJet const & jet
) const{
if(ext_parton.pt() < param_.min_extparton_pt) return false;
return (ext_parton - jet).pt()/jet.pt() < param_.max_ext_soft_pt_fraction;
}
std::vector<fastjet::PseudoJet> PhaseSpacePoint::split(
std::vector<fastjet::PseudoJet> const & jets,
std::vector<int> const & np
){
assert(! jets.empty());
assert(jets.size() == np.size());
assert(pass_resummation_cuts(jets));
const size_t most_backward_FKL_idx = 0 + unob_ + qqxb_;
const size_t most_forward_FKL_idx = jets.size() - 1 - unof_ - qqxf_;
const auto & jet = param_.jet_param;
const JetSplitter jet_splitter{jet.def, jet.min_pt, ran_};
std::vector<fastjet::PseudoJet> jet_partons;
// randomly distribute jet gluons among jets
for(size_t i = 0; i < jets.size(); ++i){
auto split_res = jet_splitter.split(jets[i], np[i]);
weight_ *= split_res.weight;
if(weight_ == 0) return {};
assert(
std::all_of(
begin(split_res.constituents), end(split_res.constituents),
is_jet_parton
)
);
const auto first_new_parton = jet_partons.insert(
end(jet_partons),
begin(split_res.constituents), end(split_res.constituents)
);
// mark uno and extremal FKL emissions here so we can check
// their position once all emissions are generated
auto extremal = end(jet_partons);
if (i == most_backward_FKL_idx){ //FKL backward emission
extremal = std::min_element(
first_new_parton, end(jet_partons), rapidity_less{}
);
extremal->set_user_index(backward_FKL_idx);
}
else if(((unob_ || qqxb_) && i == 0)){
// unordered/qqxb
extremal = std::min_element(
first_new_parton, end(jet_partons), rapidity_less{}
);
extremal->set_user_index((unob_)?unob_idx:qqxb_idx);
}
else if (i == most_forward_FKL_idx){
extremal = std::max_element(
first_new_parton, end(jet_partons), rapidity_less{}
);
extremal->set_user_index(forward_FKL_idx);
}
else if(((unof_ || qqxf_) && i == jets.size() - 1)){
// unordered/qqxf
extremal = std::max_element(
first_new_parton, end(jet_partons), rapidity_less{}
);
extremal->set_user_index((unof_)?unof_idx:qqxf_idx);
}
if(
extremal != end(jet_partons)
&& !pass_extremal_cuts(*extremal, jets[i])
){
weight_ = 0;
return {};
}
}
assert(tagged_FKL_extremal(jet_partons));
std::sort(begin(jet_partons), end(jet_partons), rapidity_less{});
if(
!extremal_ok(jet_partons)
|| !split_preserved_jets(jets, jet_partons)
){
weight_ = 0.;
return {};
}
return jet_partons;
}
bool PhaseSpacePoint::extremal_ok(
std::vector<fastjet::PseudoJet> const & partons
) const{
assert(std::is_sorted(begin(partons), end(partons), rapidity_less{}));
if(unob_ && partons.front().user_index() != unob_idx) return false;
if(unof_ && partons.back().user_index() != unof_idx) return false;
if(qqxb_ && partons.front().user_index() != qqxb_idx) return false;
if(qqxf_ && partons.back().user_index() != qqxf_idx) return false;
return
most_backward_FKL(partons).user_index() == backward_FKL_idx
&& most_forward_FKL(partons).user_index() == forward_FKL_idx;
}
bool PhaseSpacePoint::split_preserved_jets(
std::vector<fastjet::PseudoJet> const & jets,
std::vector<fastjet::PseudoJet> const & jet_partons
) const{
assert(std::is_sorted(begin(jets), end(jets), rapidity_less{}));
const auto split_jets = sorted_by_rapidity(cluster_jets(jet_partons));
// this can happen if two overlapping jets
// are both split into more than one parton
if(split_jets.size() != jets.size()) return false;
for(size_t i = 0; i < split_jets.size(); ++i){
// this can happen if there are two overlapping jets
// and a parton is assigned to the "wrong" jet
if(!nearby_ep(jets[i].rapidity(), split_jets[i].rapidity(), 1e-2)){
return false;
}
}
return true;
}
template<class Particle>
Particle const & PhaseSpacePoint::most_backward_FKL(
std::vector<Particle> const & partons
) const{
return partons[0 + unob_ + qqxb_];
}
template<class Particle>
Particle const & PhaseSpacePoint::most_forward_FKL(
std::vector<Particle> const & partons
) const{
const size_t idx = partons.size() - 1 - unof_ - qqxf_;
assert(idx < partons.size());
return partons[idx];
}
template<class Particle>
Particle & PhaseSpacePoint::most_backward_FKL(
std::vector<Particle> & partons
) const{
return partons[0 + unob_ + qqxb_];
}
template<class Particle>
Particle & PhaseSpacePoint::most_forward_FKL(
std::vector<Particle> & partons
) const{
const size_t idx = partons.size() - 1 - unof_ - qqxf_;
assert(idx < partons.size());
return partons[idx];
}
namespace {
bool contains_idx(
fastjet::PseudoJet const & jet, fastjet::PseudoJet const & parton
){
auto const & constituents = jet.constituents();
const int idx = parton.user_index();
return std::find_if(
begin(constituents), end(constituents),
[idx](fastjet::PseudoJet const & con){return con.user_index() == idx;}
) != end(constituents);
}
}
/**
* final jet test:
* - number of jets must match Born kinematics
* - no partons designated as nonjet may end up inside jets
* - all other outgoing partons *must* end up inside jets
* - the extremal (in rapidity) partons must be inside the extremal jets
* - rapidities must be the same (by construction)
*/
bool PhaseSpacePoint::jets_ok(
std::vector<fastjet::PseudoJet> const & Born_jets,
std::vector<fastjet::PseudoJet> const & partons
) const{
fastjet::ClusterSequence cs(partons, param_.jet_param.def);
const auto jets = sorted_by_rapidity(cs.inclusive_jets(param_.jet_param.min_pt));
if(jets.size() != Born_jets.size()) return false;
int in_jet = 0;
for(size_t i = 0; i < jets.size(); ++i){
assert(jets[i].has_constituents());
for(auto && parton: jets[i].constituents()){
if(is_nonjet_parton(parton)) return false;
}
in_jet += jets[i].constituents().size();
}
const int expect_in_jet = std::count_if(
partons.cbegin(), partons.cend(), is_jet_parton
);
if(in_jet != expect_in_jet) return false;
// note that PseudoJet::contains does not work here
if(! (
contains_idx(most_backward_FKL(jets), most_backward_FKL(partons))
&& contains_idx(most_forward_FKL(jets), most_forward_FKL(partons))
)) return false;
if(unob_ && !contains_idx(jets.front(), partons.front())) return false;
if(unof_ && !contains_idx(jets.back(), partons.back())) return false;
for(size_t i = 0; i < jets.size(); ++i){
assert(nearby_ep(jets[i].rapidity(), Born_jets[i].rapidity(), 1e-2));
}
return true;
}
void PhaseSpacePoint::reconstruct_incoming(
std::array<Particle, 2> const & Born_incoming
){
std::tie(incoming_[0].p, incoming_[1].p) = incoming_momenta(outgoing_);
for(size_t i = 0; i < incoming_.size(); ++i){
incoming_[i].type = Born_incoming[i].type;
}
assert(momentum_conserved());
}
double PhaseSpacePoint::phase_space_normalisation(
int num_Born_jets, int num_out_partons
) const{
return pow(16*pow(M_PI,3), num_Born_jets - num_out_partons);
}
bool PhaseSpacePoint::momentum_conserved() const{
fastjet::PseudoJet diff;
for(auto const & in: incoming()) diff += in.p;
const double norm = diff.E();
for(auto const & out: outgoing()) diff -= out.p;
return nearby(diff, fastjet::PseudoJet{}, norm);
}
} //namespace HEJ
diff --git a/src/Ranlux64.cc b/src/Ranlux64.cc
index 2d806be..c870864 100644
--- a/src/Ranlux64.cc
+++ b/src/Ranlux64.cc
@@ -1,54 +1,61 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/Ranlux64.hh"
+#include <cstdio>
+
namespace HEJ {
namespace {
//! create Ranlux64Engine with state read from the given file
CLHEP::Ranlux64Engine make_Ranlux64Engine(std::string const & seed_file) {
CLHEP::Ranlux64Engine result;
result.restoreStatus(seed_file.c_str());
return result;
}
CLHEP::Ranlux64Engine make_Ranlux64Engine() {
/*
* some (all?) of the Ranlux64Engine constructors leave fields
* uninitialised, invoking undefined behaviour. This can be
* circumvented by restoring the state from a file
*/
static const std::string state =
"9876\n"
"0.91280703978419097666\n"
"0.41606065829518357191\n"
"0.99156342622341142601\n"
"0.030922955274050423213\n"
"0.16206278421638486975\n"
"0.76151768001958330956\n"
"0.43765760066092695979\n"
"0.42904698253748563275\n"
"0.11476317525663759511\n"
"0.026620053590963976831\n"
"0.65953715764414511114\n"
"0.30136722624439826745\n"
"3.5527136788005009294e-15 4\n"
"1 202\n";
const std::string file = std::tmpnam(nullptr);
{
std::ofstream out{file};
out << state;
}
auto result = make_Ranlux64Engine(file);
std::remove(file.c_str());
return result;
}
}
Ranlux64::Ranlux64(): ran_{make_Ranlux64Engine()} {}
Ranlux64::Ranlux64(std::string const & seed_file):
ran_{make_Ranlux64Engine(seed_file)}
{}
double Ranlux64::flat() {
return ran_.flat();
}
}
diff --git a/src/RivetAnalysis.cc b/src/RivetAnalysis.cc
index 87cd1b4..7db9b8b 100644
--- a/src/RivetAnalysis.cc
+++ b/src/RivetAnalysis.cc
@@ -1,109 +1,143 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/RivetAnalysis.hh"
#ifdef HEJ_BUILD_WITH_RIVET
#include <ostream>
-
-#include "HEJ/Event.hh"
+#include <stddef.h>
#include "yaml-cpp/yaml.h"
+
#include "Rivet/AnalysisHandler.hh"
+#include "HepMC/GenEvent.h"
+
+#include "HEJ/Event.hh"
+#include "HEJ/exceptions.hh"
+
#endif
namespace HEJ{
std::unique_ptr<Analysis> RivetAnalysis::create(YAML::Node const & config){
return std::unique_ptr<Analysis>{new RivetAnalysis{config}};
}
}
#ifdef HEJ_BUILD_WITH_RIVET
namespace HEJ {
RivetAnalysis::RivetAnalysis(YAML::Node const & config):
output_name_{config["output"].as<std::string>()},
first_event_(true)
{
// read in analyses
const auto & name_node = config["rivet"];
switch(name_node.Type()){
case YAML::NodeType::Scalar:
analyses_names_.push_back(name_node.as<std::string>());
break;
case YAML::NodeType::Sequence:
for(YAML::const_iterator it = name_node.begin(); it != name_node.end(); ++it){
analyses_names_.push_back(it->as<std::string>());
}
break;
default:
throw std::invalid_argument{
"No Analysis was provided to rivet. "
"Either give an analysis or deactivate rivet."
};
}
}
+ namespace {
+ void replace(
+ std::string & str,
+ char to_replace, std::string const & replacement
+ ) {
+ for(
+ auto pos = str.find(to_replace);
+ pos != str.npos;
+ pos = str.find(to_replace, pos)
+ ) {
+ str.replace(pos, 1, replacement);
+ pos += replacement.size();
+ }
+ }
+
+ // remove "special" characters from scale name
+ // so that we can more easily use it as part of a file name
+ std::string sanitise_scalename(std::string scalename) {
+ replace(scalename, '/', "_over_");
+ replace(scalename, '*', "_times_");
+ return scalename;
+ }
+ }
+
void RivetAnalysis::init(Event const & event){
rivet_runs_.push_back(
{std::make_unique<Rivet::AnalysisHandler>(), "", HepMCInterface()}
);
rivet_runs_.back().handler->addAnalyses(analyses_names_);
if( !event.variations().empty() ){
rivet_runs_.reserve(event.variations().size()+1);
for(auto const & vari : event.variations()){
std::ostringstream name;
- name << ".Scale" << vari.description->scale_name
+ name << ".Scale" << sanitise_scalename(vari.description->scale_name)
<< "_MuR" << vari.description->mur_factor
<< "_MuF" << vari.description->muf_factor;
rivet_runs_.push_back(
{std::make_unique<Rivet::AnalysisHandler>(), name.str(), HepMCInterface()}
);
rivet_runs_.back().handler->addAnalyses(analyses_names_);
}
}
}
void RivetAnalysis::fill(Event const & event, Event const &){
if(first_event_){
first_event_=false;
init(event);
}
HepMC::GenEvent hepmc_kin(rivet_runs_[0].hepmc.init_kinematics(event));
for(size_t i = 0; i < rivet_runs_.size(); ++i){
auto & run = rivet_runs_[i];
run.hepmc.set_central(hepmc_kin, event, i-1); // -1: first = central
run.handler->analyze(hepmc_kin);
}
}
void RivetAnalysis::finalise(){
for(auto const & run: rivet_runs_){
run.handler->finalize();
run.handler->writeData(output_name_+run.name+std::string(".yoda"));
}
}
} // namespace HEJ
#else // no rivet => create empty analysis
namespace Rivet {
class AnalysisHandler {};
}
namespace HEJ {
RivetAnalysis::RivetAnalysis(YAML::Node const &)
{
throw std::invalid_argument(
"Failed to create RivetAnalysis: "
"HEJ 2 was built without rivet support"
);
}
void RivetAnalysis::init(Event const &){}
void RivetAnalysis::fill(Event const &, Event const &){}
void RivetAnalysis::finalise(){}
} // namespace HEJ
#endif
diff --git a/src/ScaleFunction.cc b/src/ScaleFunction.cc
index ce2132c..5fc7d7e 100644
--- a/src/ScaleFunction.cc
+++ b/src/ScaleFunction.cc
@@ -1,144 +1,171 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/ScaleFunction.hh"
-#include <numeric>
#include <cassert>
#include "HEJ/Event.hh"
+#include "HEJ/exceptions.hh"
namespace HEJ{
double H_T(Event const & ev){
double result = 0.;
for(size_t i = 0; i < ev.outgoing().size(); ++i){
auto const decay_products = ev.decays().find(i);
if(decay_products == end(ev.decays())){
result += ev.outgoing()[i].perp();
}
else{
for(auto const & particle: decay_products->second){
result += particle.perp();
}
}
}
return result;
}
double max_jet_pt(Event const & ev) {
return sorted_by_pt(ev.jets()).front().pt();
}
double jet_invariant_mass(Event const & ev) {
fastjet::PseudoJet sum;
for(const auto & jet: ev.jets()) sum+=jet;
return sum.m();
}
double m_j1j2(Event const & ev) {
const auto jets = sorted_by_pt(ev.jets());
assert(jets.size() >= 2);
return (jets[0] + jets[1]).m();
}
ScaleFunction operator*(double factor, ScaleFunction base_scale) {
base_scale.name_.insert(0, std::to_string(factor) + '*');
auto new_fun =
[factor,fun{std::move(base_scale.fun_)}](HEJ::Event const & ev) {
return factor*fun(ev);
};
base_scale.fun_ = std::move(new_fun);
return base_scale;
}
+ ScaleFunction operator*(ScaleFunction factor, ScaleFunction base_scale) {
+ base_scale.name_.insert(0, factor.name_ + '*');
+ auto new_fun =
+ [fun1{std::move(factor.fun_)}, fun2{std::move(base_scale.fun_)}, name{base_scale.name_}]
+ (HEJ::Event const & ev) {
+ return fun1(ev)*fun2(ev);
+ };
+ base_scale.fun_ = std::move(new_fun);
+ return base_scale;
+ }
+
ScaleFunction operator/(ScaleFunction base_scale, double denom) {
base_scale.name_.append('/' + std::to_string(denom));
auto new_fun =
[denom,fun{std::move(base_scale.fun_)}](HEJ::Event const & ev) {
return fun(ev)/denom;
};
base_scale.fun_ = std::move(new_fun);
return base_scale;
}
+ ScaleFunction operator/(ScaleFunction base_scale, ScaleFunction denom) {
+ base_scale.name_.append('/' + denom.name_);
+ auto new_fun =
+ [fun2{std::move(denom.fun_)}, fun1{std::move(base_scale.fun_)}]
+ (HEJ::Event const & ev) {
+ return fun1(ev)/fun2(ev);
+ };
+ base_scale.fun_ = std::move(new_fun);
+ return base_scale;
+ }
+
// TODO: significant logic duplication with operator()
void ScaleGenerator::gen_descriptions() {
if(scales_.empty()) {
throw std::logic_error{"Need at least one scale"};
}
descriptions_.emplace_back(
std::make_shared<ParameterDescription>(scales_.front().name(), 1., 1.)
);
for(auto & base_scale: scales_){
const auto base_name = base_scale.name();
descriptions_.emplace_back(
std::make_shared<ParameterDescription>(base_name, 1., 1.)
);
//multiplicative scale variation
for(double mur_factor: scale_factors_){
for(double muf_factor: scale_factors_){
if(muf_factor == 1. && mur_factor == 1.) continue;
if(
mur_factor/muf_factor < 1/max_scale_ratio_
|| mur_factor/muf_factor > max_scale_ratio_
) continue;
descriptions_.emplace_back(
std::make_shared<ParameterDescription>(
base_name, mur_factor, muf_factor
)
);
}
}
}
}
Event ScaleGenerator::operator()(Event ev) const {
if(! ev.variations().empty()) {
throw std::invalid_argument{"Input event already has scale variation"};
}
assert(!scales_.empty());
assert(!descriptions_.empty());
size_t descr_idx = 0;
const double mu_central = (scales_.front())(ev);
ev.central().mur = mu_central;
ev.central().muf = mu_central;
assert(descr_idx < descriptions_.size());
assert(descriptions_[descr_idx]);
ev.central().description = descriptions_[descr_idx++];
// check if we are doing scale variation at all
if(scales_.size() == 1 && scale_factors_.empty()) return ev;
for(auto & base_scale: scales_){
const double mu_base = base_scale(ev);
assert(descr_idx < descriptions_.size());
assert(descriptions_[descr_idx]);
ev.variations().emplace_back(
EventParameters{
mu_base, mu_base, ev.central().weight, descriptions_[descr_idx++]
}
);
//multiplicative scale variation
for(double mur_factor: scale_factors_){
const double mur = mu_base*mur_factor;
for(double muf_factor: scale_factors_){
if(muf_factor == 1. && mur_factor == 1.) continue;
const double muf = mu_base*muf_factor;
if(
mur/muf < 1/max_scale_ratio_
|| mur/muf > max_scale_ratio_
) continue;
assert(descr_idx < descriptions_.size());
assert(descriptions_[descr_idx]);
ev.variations().emplace_back(
EventParameters{
mur, muf, ev.central().weight, descriptions_[descr_idx++]
}
);
}
}
};
return ev;
}
}
diff --git a/src/Weights.cc b/src/Weights.cc
index 9e0ee9c..de2d561 100644
--- a/src/Weights.cc
+++ b/src/Weights.cc
@@ -1,41 +1,46 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/Weights.hh"
#include <stdexcept>
namespace HEJ {
Weights& Weights::operator*=(Weights const & other) {
if(other.variations.size() != variations.size()) {
throw std::invalid_argument{"Wrong number of weights"};
}
central *= other.central;
for(std::size_t i = 0; i < variations.size(); ++i) {
variations[i] *= other.variations[i];
}
return *this;
}
Weights& Weights::operator*=(double factor) {
central *= factor;
for(auto & wt: variations) wt *= factor;
return *this;
}
Weights& Weights::operator/=(Weights const & other) {
if(other.variations.size() != variations.size()) {
throw std::invalid_argument{"Wrong number of weights"};
}
central /= other.central;
for(std::size_t i = 0; i < variations.size(); ++i) {
variations[i] /= other.variations[i];
}
return *this;
}
Weights& Weights::operator/=(double factor) {
central /= factor;
for(auto & wt: variations) wt /= factor;
return *this;
}
}
diff --git a/src/YAMLreader.cc b/src/YAMLreader.cc
index 5af5866..72919e4 100644
--- a/src/YAMLreader.cc
+++ b/src/YAMLreader.cc
@@ -1,464 +1,471 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/YAMLreader.hh"
-#include <set>
+#include <algorithm>
+#include <iostream>
+#include <limits>
+#include <map>
#include <string>
+#include <unordered_map>
#include <vector>
-#include <iostream>
-#include <stdexcept>
#include <dlfcn.h>
+#include "HEJ/ScaleFunction.hh"
+#include "HEJ/event_types.hh"
+#include "HEJ/output_formats.hh"
+
namespace HEJ{
+ class Event;
namespace{
//! Get YAML tree of supported options
/**
* The configuration file is checked against this tree of options
* in assert_all_options_known.
*/
YAML::Node const & get_supported_options(){
const static YAML::Node supported = [](){
YAML::Node supported;
static const auto opts = {
"trials", "min extparton pt", "max ext soft pt fraction",
"FKL", "unordered", "qqx", "non-HEJ",
"scales", "scale factors", "max scale ratio", "import scales",
- "log correction", "unweight", "event output", "analysis"
+ "log correction", "event output", "analysis"
};
// add subnodes to "supported" - the assigned value is irrelevant
for(auto && opt: opts) supported[opt] = "";
for(auto && jet_opt: {"min pt", "algorithm", "R"}){
supported["resummation jets"][jet_opt] = "";
supported["fixed order jets"][jet_opt] = "";
}
for(auto && opt: {"mt", "use impact factors", "include bottom", "mb"}){
supported["Higgs coupling"][opt] = "";
}
for(auto && opt: {"name", "seed"}){
supported["random generator"][opt] = "";
}
return supported;
}();
return supported;
}
fastjet::JetAlgorithm to_JetAlgorithm(std::string const & algo){
using namespace fastjet;
static const std::map<std::string, fastjet::JetAlgorithm> known = {
{"kt", kt_algorithm},
{"cambridge", cambridge_algorithm},
{"antikt", antikt_algorithm},
{"cambridge for passive", cambridge_for_passive_algorithm},
{"plugin", plugin_algorithm}
};
const auto res = known.find(algo);
if(res == known.end()){
throw std::invalid_argument("Unknown jet algorithm " + algo);
}
return res->second;
}
EventTreatment to_EventTreatment(std::string const & name){
static const std::map<std::string, EventTreatment> known = {
{"reweight", EventTreatment::reweight},
{"keep", EventTreatment::keep},
{"discard", EventTreatment::discard}
};
const auto res = known.find(name);
if(res == known.end()){
throw std::invalid_argument("Unknown event treatment " + name);
}
return res->second;
}
} // namespace anonymous
namespace detail{
void set_from_yaml(fastjet::JetAlgorithm & setting, YAML::Node const & yaml){
setting = to_JetAlgorithm(yaml.as<std::string>());
}
void set_from_yaml(EventTreatment & setting, YAML::Node const & yaml){
setting = to_EventTreatment(yaml.as<std::string>());
}
void set_from_yaml(ParticleID & setting, YAML::Node const & yaml){
setting = to_ParticleID(yaml.as<std::string>());
}
} // namespace detail
JetParameters get_jet_parameters(
YAML::Node const & node,
std::string const & entry
){
assert(node);
JetParameters result;
fastjet::JetAlgorithm jet_algo = fastjet::antikt_algorithm;
double R;
set_from_yaml_if_defined(jet_algo, node, entry, "algorithm");
set_from_yaml(R, node, entry, "R");
result.def = fastjet::JetDefinition{jet_algo, R};
set_from_yaml(result.min_pt, node, entry, "min pt");
return result;
}
RNGConfig to_RNGConfig(
YAML::Node const & node,
std::string const & entry
){
assert(node);
RNGConfig result;
set_from_yaml(result.name, node, entry, "name");
set_from_yaml_if_defined(result.seed, node, entry, "seed");
return result;
}
HiggsCouplingSettings get_Higgs_coupling(
YAML::Node const & node,
std::string const & entry
){
assert(node);
static constexpr double mt_max = 2e4;
#ifndef HEJ_BUILD_WITH_QCDLOOP
if(node[entry]){
throw std::invalid_argument{
"Higgs coupling settings require building HEJ 2 "
"with QCDloop support"
};
}
#endif
HiggsCouplingSettings settings;
set_from_yaml_if_defined(settings.mt, node, entry, "mt");
set_from_yaml_if_defined(settings.mb, node, entry, "mb");
set_from_yaml_if_defined(settings.include_bottom, node, entry, "include bottom");
set_from_yaml_if_defined(settings.use_impact_factors, node, entry, "use impact factors");
if(settings.use_impact_factors){
if(settings.mt != std::numeric_limits<double>::infinity()){
throw std::invalid_argument{
"Conflicting settings: "
"impact factors may only be used in the infinite top mass limit"
};
}
}
else{
// huge values of the top mass are numerically unstable
settings.mt = std::min(settings.mt, mt_max);
}
return settings;
}
FileFormat to_FileFormat(std::string const & name){
static const std::map<std::string, FileFormat> known = {
{"Les Houches", FileFormat::Les_Houches},
{"HepMC", FileFormat::HepMC}
};
const auto res = known.find(name);
if(res == known.end()){
throw std::invalid_argument("Unknown file format " + name);
}
return res->second;
}
std::string extract_suffix(std::string const & filename){
size_t separator = filename.rfind('.');
if(separator == filename.npos) return {};
return filename.substr(separator + 1);
}
FileFormat format_from_suffix(std::string const & filename){
const std::string suffix = extract_suffix(filename);
if(suffix == "lhe") return FileFormat::Les_Houches;
if(suffix == "hepmc") return FileFormat::HepMC;
throw std::invalid_argument{
"Can't determine format for output file " + filename
};
}
void assert_all_options_known(
YAML::Node const & conf, YAML::Node const & supported
){
if(!conf.IsMap()) return;
if(!supported.IsMap()) throw invalid_type{"must not have sub-entries"};
for(auto const & entry: conf){
const auto name = entry.first.as<std::string>();
if(! supported[name]) throw unknown_option{name};
/* check sub-options, e.g. 'resummation jets: min pt'
* we don't check analysis sub-options
* those depend on the analysis being used and should be checked there
* similar for "import scales"
*/
if(name != "analysis" && name != "import scales"){
try{
assert_all_options_known(conf[name], supported[name]);
}
catch(unknown_option const & ex){
throw unknown_option{name + ": " + ex.what()};
}
catch(invalid_type const & ex){
throw invalid_type{name + ": " + ex.what()};
}
}
}
}
} // namespace HEJ
namespace YAML {
Node convert<HEJ::OutputFile>::encode(HEJ::OutputFile const & outfile) {
Node node;
node[to_string(outfile.format)] = outfile.name;
return node;
};
bool convert<HEJ::OutputFile>::decode(Node const & node, HEJ::OutputFile & out) {
switch(node.Type()){
case NodeType::Map: {
YAML::const_iterator it = node.begin();
out.format = HEJ::to_FileFormat(it->first.as<std::string>());
out.name = it->second.as<std::string>();
return true;
}
case NodeType::Scalar:
out.name = node.as<std::string>();
out.format = HEJ::format_from_suffix(out.name);
return true;
default:
return false;
}
}
} // namespace YAML
namespace HEJ{
namespace detail{
void set_from_yaml(OutputFile & setting, YAML::Node const & yaml){
setting = yaml.as<OutputFile>();
}
}
namespace{
void update_fixed_order_jet_parameters(
JetParameters & fixed_order_jets, YAML::Node const & yaml
){
if(!yaml["fixed order jets"]) return;
set_from_yaml_if_defined(
fixed_order_jets.min_pt, yaml, "fixed order jets", "min pt"
);
fastjet::JetAlgorithm algo = fixed_order_jets.def.jet_algorithm();
set_from_yaml_if_defined(algo, yaml, "fixed order jets", "algorithm");
double R = fixed_order_jets.def.R();
set_from_yaml_if_defined(R, yaml, "fixed order jets", "R");
fixed_order_jets.def = fastjet::JetDefinition{algo, R};
}
// like std::stod, but throw if not the whole string can be converted
double to_double(std::string const & str){
std::size_t pos;
const double result = std::stod(str, &pos);
if(pos < str.size()){
throw std::invalid_argument(str + " is not a valid double value");
}
return result;
}
using EventScale = double (*)(Event const &);
void import_scale_functions(
std::string const & file,
std::vector<std::string> const & scale_names,
std::unordered_map<std::string, EventScale> & known
) {
auto handle = dlopen(file.c_str(), RTLD_NOW);
char * error = dlerror();
if(error != nullptr) throw std::runtime_error{error};
for(auto const & scale: scale_names) {
void * sym = dlsym(handle, scale.c_str());
error = dlerror();
if(error != nullptr) throw std::runtime_error{error};
known.emplace(scale, reinterpret_cast<EventScale>(sym));
}
}
auto get_scale_map(
YAML::Node const & yaml
) {
std::unordered_map<std::string, EventScale> scale_map;
scale_map.emplace("H_T", H_T);
scale_map.emplace("max jet pperp", max_jet_pt);
scale_map.emplace("jet invariant mass", jet_invariant_mass);
scale_map.emplace("m_j1j2", m_j1j2);
if(yaml["import scales"]) {
if(! yaml["import scales"].IsMap()) {
throw invalid_type{"Entry 'import scales' is not a map"};
}
for(auto const & import: yaml["import scales"]) {
const auto file = import.first.as<std::string>();
const auto scale_names =
import.second.IsSequence()
?import.second.as<std::vector<std::string>>()
:std::vector<std::string>{import.second.as<std::string>()};
import_scale_functions(file, scale_names, scale_map);
}
}
return scale_map;
}
// simple (as in non-composite) scale functions
/**
* An example for a simple scale function would be H_T,
* H_T/2 is then composite (take H_T and then divide by 2)
*/
ScaleFunction parse_simple_ScaleFunction(
std::string const & scale_fun,
std::unordered_map<std::string, EventScale> const & known
) {
assert(
scale_fun.empty() ||
(!std::isspace(scale_fun.front()) && !std::isspace(scale_fun.back()))
);
const auto it = known.find(scale_fun);
if(it != end(known)) return {it->first, it->second};
try{
const double scale = to_double(scale_fun);
return {scale_fun, FixedScale{scale}};
} catch(std::invalid_argument const &){}
throw std::invalid_argument{"Unknown scale choice: " + scale_fun};
}
std::string trim_front(std::string const & str){
const auto new_begin = std::find_if(
begin(str), end(str), [](char c){ return ! std::isspace(c); }
);
return std::string(new_begin, end(str));
}
std::string trim_back(std::string str){
size_t pos = str.size() - 1;
// use guaranteed wrap-around behaviour to check whether we have
// traversed the whole string
for(; pos < str.size() && std::isspace(str[pos]); --pos) {}
str.resize(pos + 1); // note that pos + 1 can be 0
return str;
}
ScaleFunction parse_ScaleFunction(
std::string const & scale_fun,
std::unordered_map<std::string, EventScale> const & known
){
assert(
scale_fun.empty() ||
(!std::isspace(scale_fun.front()) && !std::isspace(scale_fun.back()))
);
- const size_t delim = scale_fun.find_first_of("*/");
+ // parse from right to left => a/b/c gives (a/b)/c
+ const size_t delim = scale_fun.find_last_of("*/");
if(delim == scale_fun.npos){
return parse_simple_ScaleFunction(scale_fun, known);
}
const std::string first = trim_back(std::string{scale_fun, 0, delim});
const std::string second = trim_front(std::string{scale_fun, delim+1});
if(scale_fun[delim] == '/'){
- return parse_simple_ScaleFunction(first, known)/to_double(second);
+ return parse_ScaleFunction(first, known)
+ / parse_ScaleFunction(second, known);
}
else{
assert(scale_fun[delim] == '*');
- try{
- const double factor = to_double(second);
- return factor*parse_simple_ScaleFunction(first, known);
- }
- catch(std::invalid_argument const &){
- const double factor = to_double(first);
- return factor*parse_simple_ScaleFunction(first, known);
- }
+ return parse_ScaleFunction(first, known)
+ * parse_ScaleFunction(second, known);
}
}
EventTreatMap get_event_treatment(
YAML::Node const & yaml
){
using namespace event_type;
EventTreatMap treat {
{no_2_jets, EventTreatment::discard},
{bad_final_state, EventTreatment::discard},
{FKL, EventTreatment::reweight},
{unob, EventTreatment::keep},
{unof, EventTreatment::keep},
{qqxexb, EventTreatment::keep},
{qqxexf, EventTreatment::keep},
{qqxmid, EventTreatment::keep},
{nonHEJ, EventTreatment::keep}
};
set_from_yaml(treat.at(FKL), yaml, "FKL");
set_from_yaml(treat.at(unob), yaml, "unordered");
treat.at(unof) = treat.at(unob);
set_from_yaml(treat.at(qqxexb), yaml, "qqx");
set_from_yaml(treat.at(qqxexf), yaml, "qqx");
set_from_yaml(treat.at(qqxmid), yaml, "qqx");
set_from_yaml(treat.at(nonHEJ), yaml, "non-HEJ");
if(treat[nonHEJ] == EventTreatment::reweight){
throw std::invalid_argument{"Cannot reweight non-HEJ events"};
}
return treat;
}
Config to_Config(YAML::Node const & yaml){
try{
assert_all_options_known(yaml, get_supported_options());
}
catch(unknown_option const & ex){
throw unknown_option{std::string{"Unknown option '"} + ex.what() + "'"};
}
Config config;
config.resummation_jets = get_jet_parameters(yaml, "resummation jets");
config.fixed_order_jets = config.resummation_jets;
update_fixed_order_jet_parameters(config.fixed_order_jets, yaml);
set_from_yaml(config.min_extparton_pt, yaml, "min extparton pt");
config.max_ext_soft_pt_fraction = std::numeric_limits<double>::infinity();
set_from_yaml_if_defined(
config.max_ext_soft_pt_fraction, yaml, "max ext soft pt fraction"
);
set_from_yaml(config.trials, yaml, "trials");
set_from_yaml(config.log_correction, yaml, "log correction");
- set_from_yaml(config.unweight, yaml, "unweight");
config.treat = get_event_treatment(yaml);
set_from_yaml_if_defined(config.output, yaml, "event output");
config.rng = to_RNGConfig(yaml, "random generator");
set_from_yaml_if_defined(config.analysis_parameters, yaml, "analysis");
config.scales = to_ScaleConfig(yaml);
config.Higgs_coupling = get_Higgs_coupling(yaml, "Higgs coupling");
return config;
}
} // namespace anonymous
ScaleConfig to_ScaleConfig(YAML::Node const & yaml){
ScaleConfig config;
auto scale_funs = get_scale_map(yaml);
std::vector<std::string> scales;
set_from_yaml(scales, yaml, "scales");
config.base.reserve(scales.size());
std::transform(
begin(scales), end(scales), std::back_inserter(config.base),
[scale_funs](auto const & entry){
return parse_ScaleFunction(entry, scale_funs);
}
);
set_from_yaml_if_defined(config.factors, yaml, "scale factors");
config.max_ratio = std::numeric_limits<double>::infinity();
set_from_yaml_if_defined(config.max_ratio, yaml, "max scale ratio");
return config;
}
Config load_config(std::string const & config_file){
try{
return to_Config(YAML::LoadFile(config_file));
}
catch(...){
std::cerr << "Error reading " << config_file << ":\n ";
throw;
}
}
} // namespace HEJ
diff --git a/src/bin/HEJ.cc b/src/bin/HEJ.cc
index 2f70bf1..ca81ec7 100644
--- a/src/bin/HEJ.cc
+++ b/src/bin/HEJ.cc
@@ -1,178 +1,185 @@
/**
- * Name: main.cc
- * Authors: Tuomas Hapola, Andreas Maier <andreas.maier@durham.ac.uk>
- *
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
*/
-#include <fstream>
-#include <numeric>
-#include <memory>
+#include <array>
#include <chrono>
#include <iostream>
+#include <limits>
+#include <memory>
+#include <numeric>
#include "yaml-cpp/yaml.h"
+#include "LHEF/LHEF.h"
+
+#include "fastjet/ClusterSequence.hh"
+
#include "HEJ/CombinedEventWriter.hh"
#include "HEJ/config.hh"
+#include "HEJ/Event.hh"
#include "HEJ/EventReweighter.hh"
#include "HEJ/get_analysis.hh"
-#include "LHEF/LHEF.h"
-#include "HEJ/utility.hh"
-#include "HEJ/Version.hh"
+#include "HEJ/make_RNG.hh"
+#include "HEJ/ProgressBar.hh"
#include "HEJ/stream.hh"
+#include "HEJ/Version.hh"
#include "HEJ/YAMLreader.hh"
-#include "HEJ/ProgressBar.hh"
-#include "HEJ/make_RNG.hh"
int event_number(std::string const & record){
size_t start = record.rfind("Number of Events");
start = record.find_first_of("123456789", start);
if(start == std::string::npos) {
throw std::invalid_argument("no event number record found");
}
const size_t end = record.find_first_not_of("0123456789", start);
return std::stoi(record.substr(start, end - start));
}
HEJ::Config load_config(char const * filename){
try{
return HEJ::load_config(filename);
}
catch(std::exception const & exc){
std::cerr << "Error: " << exc.what() << '\n';
std::exit(EXIT_FAILURE);
}
}
std::unique_ptr<HEJ::Analysis> get_analysis(
YAML::Node const & parameters
){
try{
return HEJ::get_analysis(parameters);
}
catch(std::exception const & exc){
std::cerr << "Failed to load analysis: " << exc.what() << '\n';
std::exit(EXIT_FAILURE);
}
}
// unique_ptr is a workaround:
// HEJ::optional is a better fit, but gives spurious errors with g++ 7.3.0
std::unique_ptr<HEJ::ProgressBar<double>> make_progress_bar(
std::vector<double> const & xs
) {
if(xs.empty()) return {};
const double Born_xs = std::accumulate(begin(xs), end(xs), 0.);
return std::make_unique<HEJ::ProgressBar<double>>(std::cout, Born_xs);
}
std::string time_to_string(const time_t time){
char s[30];
struct tm * p = localtime(&time);
strftime(s, 30, "%a %b %d %Y %H:%M:%S", p);
return s;
}
int main(int argn, char** argv) {
using clock = std::chrono::system_clock;
if (argn < 3) {
std::cerr << "\n# Usage:\n."<< argv[0] <<" config_file input_file\n\n";
return EXIT_FAILURE;
}
+
const auto start_time = clock::now();
{
std::cout << "Starting " << HEJ::Version::package_name_full()
<< ", revision " << HEJ::Version::revision() << " ("
<< time_to_string(clock::to_time_t(start_time)) << ")" << std::endl;
}
+ std::cout << HEJ::Version::logo() << "\n" << std::endl;
+
fastjet::ClusterSequence::print_banner();
// read configuration
const HEJ::Config config = load_config(argv[1]);
HEJ::istream in{argv[2]};
std::unique_ptr<HEJ::Analysis> analysis = get_analysis(
config.analysis_parameters
);
assert(analysis != nullptr);
LHEF::Reader reader{in};
auto heprup = reader.heprup;
heprup.generators.emplace_back(LHEF::XMLTag{});
heprup.generators.back().name = HEJ::Version::package_name();
heprup.generators.back().version = HEJ::Version::String();
HEJ::CombinedEventWriter writer{config.output, std::move(heprup)};
double global_reweight = 1.;
int max_events = std::numeric_limits<int>::max();
if(argn > 3){
max_events = std::stoi(argv[3]);
const int input_events = event_number(reader.headerBlock);
global_reweight = input_events/static_cast<double>(max_events);
std::cout << "Processing " << max_events
<< " out of " << input_events << " events\n";
}
HEJ::ScaleGenerator scale_gen{
config.scales.base,
config.scales.factors,
config.scales.max_ratio
};
auto ran = HEJ::make_RNG(config.rng.name, config.rng.seed);
assert(ran != nullptr);
HEJ::EventReweighter hej{
reader.heprup,
std::move(scale_gen),
to_EventReweighterConfig(config),
*ran
};
int nevent = 0;
std::array<int, HEJ::event_type::last_type + 1>
nevent_type{0}, nfailed_type{0};
auto progress = make_progress_bar(reader.heprup.XSECUP);
// Loop over the events in the inputfile
while(reader.readEvent()){
// reweight events so that the total cross section is conserved
reader.hepeup.setWeight(0, global_reweight * reader.hepeup.weight());
if(nevent == max_events) break;
++nevent;
// calculate HEJ weight
HEJ::Event FO_event{
HEJ::UnclusteredEvent{reader.hepeup},
config.fixed_order_jets.def, config.fixed_order_jets.min_pt,
};
auto resummed_events = hej.reweight(FO_event, config.trials);
++nevent_type[FO_event.type()];
if(resummed_events.empty()) ++nfailed_type[FO_event.type()];
for(auto const & ev: resummed_events){
//TODO: move pass_cuts to after phase space point generation
if(analysis->pass_cuts(ev, FO_event)){
analysis->fill(ev, FO_event);
writer.write(ev);
}
}
if(progress) progress->increment(FO_event.central().weight);
} // main event loop
std::cout << '\n';
analysis->finalise();
using namespace HEJ::event_type;
std::cout<< "Events processed: " << nevent << '\n';
for(size_t ev_type = first_type; ev_type <= last_type; ++ev_type){
std::cout << '\t' << names[ev_type] << ": " << nevent_type[ev_type]
<< ", failed to reconstruct " << nfailed_type[ev_type]
<< '\n';
}
std::chrono::duration<double> run_time = (clock::now() - start_time);
std::cout << "Finished " << HEJ::Version::package_name() << " at "
<< time_to_string(clock::to_time_t(clock::now()))
<< "\n=> Runtime: " << run_time.count() << " sec ("
<< nevent/run_time.count() << " Events/sec).\n";
}
diff --git a/src/currents.cc b/src/currents.cc
index d348f0e..de692eb 100644
--- a/src/currents.cc
+++ b/src/currents.cc
@@ -1,3210 +1,3210 @@
//////////////////////////////////////////////////
//////////////////////////////////////////////////
// This source code is Copyright (2012) of //
// Jeppe R. Andersen and Jennifer M. Smillie //
// and is distributed under the //
// Gnu Public License version 2 //
// http://www.gnu.org/licenses/gpl-2.0.html //
// You are allowed to distribute and alter the //
// source under the conditions of the GPLv2 //
// as long as this copyright notice //
// is unaltered and distributed with the source //
// Any use should comply with the //
// MCNET GUIDELINES //
// for Event Generator Authors and Users //
// as distributed with this source code //
//////////////////////////////////////////////////
//////////////////////////////////////////////////
#include "HEJ/currents.hh"
+#include <iostream>
#include <limits>
+#include <utility>
+#include <vector>
+
+#ifdef HEJ_BUILD_WITH_QCDLOOP
+#include "qcdloop/qcdloop.h"
+#endif
#include "HEJ/Constants.hh"
-#include "HEJ/utility.hh"
+#include "HEJ/exceptions.hh"
#include "HEJ/PDG_codes.hh"
const COM looprwfactor = (COM(0.,1.)*M_PI*M_PI)/pow((2.*M_PI),4);
constexpr double infinity = std::numeric_limits<double>::infinity();
-#ifdef HEJ_BUILD_WITH_QCDLOOP
-#include "qcdloop/qcdloop.h"
-#endif
-
-#include <iostream>
-#include <utility>
-
namespace {
// Loop integrals
#ifdef HEJ_BUILD_WITH_QCDLOOP
COM B0DD(CLHEP::HepLorentzVector q, double mq)
{
static std::vector<std::complex<double>> result(3);
static auto ql_B0 = [](){
ql::Bubble<std::complex<double>,double,double> ql_B0;
ql_B0.setCacheSize(100);
return ql_B0;
}();
static std::vector<double> masses(2);
static std::vector<double> momenta(1);
for(auto & m: masses) m = mq*mq;
momenta.front() = q.m2();
ql_B0.integral(result, 1, masses, momenta);
return result[0];
}
COM C0DD(CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mq)
{
static std::vector<std::complex<double>> result(3);
static auto ql_C0 = [](){
ql::Triangle<std::complex<double>,double,double> ql_C0;
ql_C0.setCacheSize(100);
return ql_C0;
}();
static std::vector<double> masses(3);
static std::vector<double> momenta(3);
for(auto & m: masses) m = mq*mq;
momenta[0] = q1.m2();
momenta[1] = q2.m2();
momenta[2] = (q1+q2).m2();
ql_C0.integral(result, 1, masses, momenta);
return result[0];
}
COM D0DD(CLHEP::HepLorentzVector q1,CLHEP::HepLorentzVector q2, CLHEP::HepLorentzVector q3, double mq)
{
static std::vector<std::complex<double>> result(3);
static auto ql_D0 = [](){
ql::Box<std::complex<double>,double,double> ql_D0;
ql_D0.setCacheSize(100);
return ql_D0;
}();
static std::vector<double> masses(4);
static std::vector<double> momenta(6);
for(auto & m: masses) m = mq*mq;
momenta[0] = q1.m2();
momenta[1] = q2.m2();
momenta[2] = q3.m2();
momenta[3] = (q1+q2+q3).m2();
momenta[4] = (q1+q2).m2();
momenta[5] = (q2+q3).m2();
ql_D0.integral(result, 1, masses, momenta);
return result[0];
}
COM A1(CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt)
// As given in Eq. (B.2) of VDD
{
double q12,q22,Q2;
CLHEP::HepLorentzVector Q;
double Delta3,mt2;
COM ans(COM(0.,0.));
q12=q1.m2();
q22=q2.m2();
Q=-q1-q2; // Define all momenta ingoing as in appendix of VDD
Q2=Q.m2();
Delta3=q12*q12+q22*q22+Q2*Q2-2*q12*q22-2*q12*Q2-2*q22*Q2;
if (mt < 0.)
std::cerr<<"Problem in A1! mt = "<<mt<<std::endl;
mt2=mt*mt;
ans=looprwfactor*COM(0,-1)*C0DD(q1,q2,mt)*( 4.*mt2/Delta3*(Q2-q12-q22)
-1.-4.*q12*q22/Delta3-12.*q12*q22*Q2/Delta3/Delta3*(q12+q22-Q2) )
- looprwfactor*COM(0,-1)*( B0DD(q2,mt)-B0DD(Q,mt) )
* ( 2.*q22/Delta3+12.*q12*q22/Delta3/Delta3*(q22-q12+Q2) )
- looprwfactor*COM(0,-1)*( B0DD(q1,mt)-B0DD(Q,mt) )
* ( 2.*q12/Delta3+12.*q12*q22/Delta3/Delta3*(q12-q22+Q2) )
- 2./Delta3/16/M_PI/M_PI*(q12+q22-Q2);
return ans;
}
COM A2(CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt)
// As given in Eq. (B.2) of VDD, but with high energy limit
// of invariants taken.
{
double q12,q22,Q2;
CLHEP::HepLorentzVector Q;
double Delta3,mt2;
COM ans(COM(0.,0.));
if (mt < 0.)
std::cerr<<"Problem in A2! mt = "<<mt<<std::endl;
mt2=mt*mt;
q12=q1.m2();
q22=q2.m2();
Q=-q1-q2; // Define all momenta ingoing as in appendix of VDD
Q2=Q.m2();
Delta3=q12*q12+q22*q22+Q2*Q2-2*q12*q22-2*q12*Q2-2*q22*Q2;
ans=looprwfactor*COM(0,-1)*C0DD(q1,q2,mt)*( 2.*mt2+1./2.*(q12+q22-Q2)
+2.*q12*q22*Q2/Delta3 )
+looprwfactor*COM(0,-1)*(B0DD(q2,mt)-B0DD(Q,mt))
*q22*(q22-q12-Q2)/Delta3
+looprwfactor*COM(0,-1)*(B0DD(q1,mt)-B0DD(Q,mt))
*q12*(q12-q22-Q2)/Delta3+1./16/M_PI/M_PI;
return ans;
}
#else // no QCDloop
COM A1(CLHEP::HepLorentzVector, CLHEP::HepLorentzVector, double) {
throw std::logic_error{"A1 called without QCDloop support"};
}
COM A2(CLHEP::HepLorentzVector, CLHEP::HepLorentzVector, double) {
throw std::logic_error{"A2 called without QCDloop support"};
}
#endif
void to_current(const CLHEP::HepLorentzVector & q, current & ret){
ret[0]=q.e();
ret[1]=q.x();
ret[2]=q.y();
ret[3]=q.z();
}
constexpr double C_A = 3.;
constexpr double C_F = 4./3.;
// using ParticleID = HEJ::pid::ParticleID;
} // namespace anonymous
// Colour acceleration multiplier for gluons see eq. (7) in arXiv:0910.5113
// @TODO: this is not a current and should be moved somewhere else
double K_g(double p1minus, double paminus) {
return 1./2.*(p1minus/paminus + paminus/p1minus)*(HEJ::C_A - 1./HEJ::C_A) + 1./HEJ::C_A;
}
double K_g(
CLHEP::HepLorentzVector const & pout,
CLHEP::HepLorentzVector const & pin
) {
if(pin.z() > 0) return K_g(pout.plus(), pin.plus());
return K_g(pout.minus(), pin.minus());
}
CCurrent CCurrent::operator+(const CCurrent& other)
{
COM result_c0=c0 + other.c0;
COM result_c1=c1 + other.c1;
COM result_c2=c2 + other.c2;
COM result_c3=c3 + other.c3;
return CCurrent(result_c0,result_c1,result_c2,result_c3);
}
CCurrent CCurrent::operator-(const CCurrent& other)
{
COM result_c0=c0 - other.c0;
COM result_c1=c1 - other.c1;
COM result_c2=c2 - other.c2;
COM result_c3=c3 - other.c3;
return CCurrent(result_c0,result_c1,result_c2,result_c3);
}
CCurrent CCurrent::operator*(const double x)
{
COM result_c0=x*CCurrent::c0;
COM result_c1=x*CCurrent::c1;
COM result_c2=x*CCurrent::c2;
COM result_c3=x*CCurrent::c3;
return CCurrent(result_c0,result_c1,result_c2,result_c3);
}
CCurrent CCurrent::operator/(const double x)
{
COM result_c0=CCurrent::c0/x;
COM result_c1=CCurrent::c1/x;
COM result_c2=CCurrent::c2/x;
COM result_c3=CCurrent::c3/x;
return CCurrent(result_c0,result_c1,result_c2,result_c3);
}
CCurrent CCurrent::operator*(const COM x)
{
COM result_c0=x*CCurrent::c0;
COM result_c1=x*CCurrent::c1;
COM result_c2=x*CCurrent::c2;
COM result_c3=x*CCurrent::c3;
return CCurrent(result_c0,result_c1,result_c2,result_c3);
}
CCurrent CCurrent::operator/(const COM x)
{
COM result_c0=(CCurrent::c0)/x;
COM result_c1=(CCurrent::c1)/x;
COM result_c2=(CCurrent::c2)/x;
COM result_c3=(CCurrent::c3)/x;
return CCurrent(result_c0,result_c1,result_c2,result_c3);
}
std::ostream& operator <<(std::ostream& os, const CCurrent& cur)
{
os << "("<<cur.c0<< " ; "<<cur.c1<<" , "<<cur.c2<<" , "<<cur.c3<<")";
return os;
}
CCurrent operator * ( double x, CCurrent& m)
{
return m*x;
}
CCurrent operator * ( COM x, CCurrent& m)
{
return m*x;
}
CCurrent operator / ( double x, CCurrent& m)
{
return m/x;
}
CCurrent operator / ( COM x, CCurrent& m)
{
return m/x;
}
COM CCurrent::dot(CLHEP::HepLorentzVector p1)
{
// Current goes (E,px,py,pz)
// std::cout<<"current = ("<<c0<<","<<c1<<","<<c2<<","<<c3<<")\n";
// Vector goes (px,py,pz,E)
// std::cout<<"vector = ("<<p1[0]<<","<<p1[1]<<","<<p1[2]<<","<<p1[3]<<")\n";
return p1[3]*c0-p1[0]*c1-p1[1]*c2-p1[2]*c3;
}
COM CCurrent::dot(CCurrent p1)
{
return p1.c0*c0-p1.c1*c1-p1.c2*c2-p1.c3*c3;
}
//Current Functions
// Current for <outgoing state | mu | incoming state>
/// @TODO always use this instead of "j"
/// @TODO isn't this jio with flipt helicities?
void joi(HLV pout, bool helout, HLV pin, bool helin, current &cur) {
cur[0]=0.;
cur[1]=0.;
cur[2]=0.;
cur[3]=0.;
const double sqpop = sqrt(pout.plus());
const double sqpom = sqrt(pout.minus());
const COM poperp = pout.x() + COM(0, 1) * pout.y();
if (helout != helin) {
throw std::invalid_argument{"Non-matching helicities"};
} else if (helout == false) { // negative helicity
if (pin.plus() > pin.minus()) { // if forward
const double sqpip = sqrt(pin.plus());
cur[0] = sqpop * sqpip;
cur[1] = sqpom * sqpip * poperp / abs(poperp);
cur[2] = -COM(0,1) * cur[1];
cur[3] = cur[0];
} else { // if backward
const double sqpim = sqrt(pin.minus());
cur[0] = -sqpom * sqpim * poperp / abs(poperp);
cur[1] = -sqpim * sqpop;
cur[2] = COM(0,1) * cur[1];
cur[3] = -cur[0];
}
} else { // positive helicity
if (pin.plus() > pin.minus()) { // if forward
const double sqpip = sqrt(pin.plus());
cur[0] = sqpop * sqpip;
cur[1] = sqpom * sqpip * conj(poperp) / abs(poperp);
cur[2] = COM(0,1) * cur[1];
cur[3] = cur[0];
} else { // if backward
const double sqpim = sqrt(pin.minus());
cur[0] = -sqpom * sqpim * conj(poperp) / abs(poperp);
cur[1] = -sqpim * sqpop;
cur[2] = -COM(0,1) * cur[1];
cur[3] = -cur[0];
}
}
}
CCurrent joi (HLV pout, bool helout, HLV pin, bool helin)
{
current cur;
joi(pout, helout, pin, helin, cur);
return CCurrent(cur[0],cur[1],cur[2],cur[3]);
}
/// @TODO remove this
void j (HLV pout, bool helout, HLV pin, bool helin,current &cur) {
joi(pout, helout, pin, helin, cur);
}
/// @TODO remove this
CCurrent j (HLV pout, bool helout, HLV pin, bool helin)
{
return joi(pout, helout, pin, helin);
}
// Current for <incoming state | mu | outgoing state>
void jio(HLV pin, bool helin, HLV pout, bool helout, current &cur) {
cur[0] = 0.0;
cur[1] = 0.0;
cur[2] = 0.0;
cur[3] = 0.0;
const double sqpop = sqrt(pout.plus());
const double sqpom = sqrt(pout.minus());
const COM poperp = pout.x() + COM(0, 1) * pout.y();
if (helout != helin) {
throw std::invalid_argument{"Non-matching helicities"};
} else if (helout == false) { // negative helicity
if (pin.plus() > pin.minus()) { // if forward
const double sqpip = sqrt(pin.plus());
cur[0] = sqpop * sqpip;
cur[1] = sqpom * sqpip * conj(poperp) / abs(poperp);
cur[2] = COM(0,1) * cur[1];
cur[3] = cur[0];
} else { // if backward
const double sqpim = sqrt(pin.minus());
cur[0] = -sqpom * sqpim * conj(poperp) / abs(poperp);
cur[1] = -sqpim * sqpop;
cur[2] = -COM(0,1) * cur[1];
cur[3] = -cur[0];
}
} else { // positive helicity
if (pin.plus() > pin.minus()) { // if forward
const double sqpip = sqrt(pin.plus());
cur[0] = sqpop * sqpip;
cur[1] = sqpom * sqpip * poperp / abs(poperp);
cur[2] = -COM(0,1) * cur[1];
cur[3] = cur[0];
} else { // if backward
const double sqpim = sqrt(pin.minus());
cur[0] = -sqpom * sqpim * poperp / abs(poperp);
cur[1] = -sqpim * sqpop;
cur[2] = COM(0,1) * cur[1];
cur[3] = -cur[0];
}
}
}
CCurrent jio (HLV pin, bool helin, HLV pout, bool helout)
{
current cur;
jio(pin, helin, pout, helout, cur);
return CCurrent(cur[0],cur[1],cur[2],cur[3]);
}
// Current for <outgoing state | mu | outgoing state>
void joo(HLV pi, bool heli, HLV pj, bool helj, current &cur) {
// Zero our current
cur[0] = 0.0;
cur[1] = 0.0;
cur[2] = 0.0;
cur[3] = 0.0;
if (heli!=helj) {
throw std::invalid_argument{"Non-matching helicities"};
} else if ( heli == true ) { // If positive helicity swap momenta
std::swap(pi,pj);
}
const double sqpjp = sqrt(pj.plus());
const double sqpjm = sqrt(pj.minus());
const double sqpip = sqrt(pi.plus());
const double sqpim = sqrt(pi.minus());
const COM piperp = pi.x() + COM(0,1) * pi.y();
const COM pjperp = pj.x() + COM(0,1) * pj.y();
const COM phasei = piperp / abs(piperp);
const COM phasej = pjperp / abs(pjperp);
cur[0] = sqpim * sqpjm * phasei * conj(phasej) + sqpip * sqpjp;
cur[1] = sqpim * sqpjp * phasei + sqpip * sqpjm * conj(phasej);
cur[2] = -COM(0, 1) * (sqpim * sqpjp * phasei - sqpip * sqpjm * conj(phasej));
cur[3] = -sqpim * sqpjm * phasei * conj(phasej) + sqpip * sqpjp;
}
CCurrent joo (HLV pi, bool heli, HLV pj, bool helj)
{
current cur;
joo(pi, heli, pj, helj, cur);
return CCurrent(cur[0],cur[1],cur[2],cur[3]);
}
namespace {
/// @TODO unused function
// double jM2 (CLHEP::HepLorentzVector p1out, bool hel1out, CLHEP::HepLorentzVector p1in, bool hel1in, CLHEP::HepLorentzVector p2out, bool hel2out, CLHEP::HepLorentzVector p2in, bool hel2in)
// {
// CLHEP::HepLorentzVector q1=p1in-p1out;
// CLHEP::HepLorentzVector q2=-(p2in-p2out);
// current C1,C2;
// j (p1out,hel1out,p1in,hel1in, C1);
// j (p2out,hel2out,p2in,hel2in, C2);
// std::cout << "# From Currents, C1 : ("<<C1[0]<<","<<C1[1]<<","<<C1[2]<<","<<C1[3]<<"\n";
// std::cout << "# From Currents, C2 : ("<<C2[0]<<","<<C2[1]<<","<<C2[2]<<","<<C2[3]<<"\n";
// COM M=cdot(C1,C2);
// return (M*conj(M)).real()/(q1.m2()*q2.m2());
// }
} // namespace anonymous
double jM2qQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in)
{
// std::cerr<<"Current: "<<p1out<<" "<<p1in<<" "<<p2out<<" "<<p2in<<std::endl;
CLHEP::HepLorentzVector q1=p1in-p1out;
CLHEP::HepLorentzVector q2=-(p2in-p2out);
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
current mj1m,mj1p,mj2m,mj2p;
joi(p1out,true,p1in,true,mj1p);
joi(p1out,false,p1in,false,mj1m);
joi(p2out,true,p2in,true,mj2p);
joi(p2out,false,p2in,false,mj2m);
COM Mmp=cdot(mj1m,mj2p);
COM Mmm=cdot(mj1m,mj2m);
COM Mpp=cdot(mj1p,mj2p);
COM Mpm=cdot(mj1p,mj2m);
double sst=abs2(Mmm)+abs2(Mmp)+abs2(Mpp)+abs2(Mpm);
// Multiply by Cf^2
return HEJ::C_F*HEJ::C_F*(sst)/(q1.m2()*q2.m2());
}
double jM2qQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in)
{
CLHEP::HepLorentzVector q1=p1in-p1out;
CLHEP::HepLorentzVector q2=-(p2in-p2out);
current mj1m,mj1p,mj2m,mj2p;
joi(p1out,true,p1in,true,mj1p);
joi(p1out,false,p1in,false,mj1m);
jio(p2in,true,p2out,true,mj2p);
jio(p2in,false,p2out,false,mj2m);
COM Mmp=cdot(mj1m,mj2p);
COM Mmm=cdot(mj1m,mj2m);
COM Mpp=cdot(mj1p,mj2p);
COM Mpm=cdot(mj1p,mj2m);
double sumsq=abs2(Mmm)+abs2(Mmp)+abs2(Mpp)+abs2(Mpm);
// Multiply by Cf^2
return C_F*C_F*(sumsq)/(q1.m2()*q2.m2());
}
double jM2qbarQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in)
{
CLHEP::HepLorentzVector q1=p1in-p1out;
CLHEP::HepLorentzVector q2=-(p2in-p2out);
current mj1m,mj1p,mj2m,mj2p;
jio(p1in,true,p1out,true,mj1p);
jio(p1in,false,p1out,false,mj1m);
jio(p2in,true,p2out,true,mj2p);
jio(p2in,false,p2out,false,mj2m);
COM Mmp=cdot(mj1m,mj2p);
COM Mmm=cdot(mj1m,mj2m);
COM Mpp=cdot(mj1p,mj2p);
COM Mpm=cdot(mj1p,mj2m);
double sumsq=abs2(Mmm)+abs2(Mmp)+abs2(Mpp)+abs2(Mpm);
// Multiply by Cf^2
return C_F*C_F*(sumsq)/(q1.m2()*q2.m2());
}
double jM2qg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in)
// Calculates the square of the current contractions for qg scattering
// p1: quark
// p2: gluon
{
CLHEP::HepLorentzVector q1=p1in-p1out;
CLHEP::HepLorentzVector q2=-(p2in-p2out);
current mj1m,mj1p,mj2m,mj2p;
joi(p1out,true,p1in,true,mj1p);
joi(p1out,false,p1in,false,mj1m);
joi(p2out,true,p2in,true,mj2p);
joi(p2out,false,p2in,false,mj2m);
COM Mmp=cdot(mj1m,mj2p);
COM Mmm=cdot(mj1m,mj2m);
COM Mpp=cdot(mj1p,mj2p);
COM Mpm=cdot(mj1p,mj2m);
const double K = K_g(p2out, p2in);
// sum of spinor strings ||^2
double a2Mmp=abs2(Mmp);
double a2Mmm=abs2(Mmm);
double a2Mpp=abs2(Mpp);
double a2Mpm=abs2(Mpm);
double sst = K/C_A*(a2Mpp+a2Mpm+a2Mmp+a2Mmm);
// Cf*Ca=4
return C_F*C_A*sst/(q1.m2()*q2.m2());
}
double jM2qbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in)
// Calculates the square of the current contractions for qg scattering
// p1: quark
// p2: gluon
{
CLHEP::HepLorentzVector q1=p1in-p1out;
CLHEP::HepLorentzVector q2=-(p2in-p2out);
current mj1m,mj1p,mj2m,mj2p;
jio(p1in,true,p1out,true,mj1p);
jio(p1in,false,p1out,false,mj1m);
joi(p2out,true,p2in,true,mj2p);
joi(p2out,false,p2in,false,mj2m);
COM Mmp=cdot(mj1m,mj2p);
COM Mmm=cdot(mj1m,mj2m);
COM Mpp=cdot(mj1p,mj2p);
COM Mpm=cdot(mj1p,mj2m);
const double K = K_g(p2out, p2in);
// sum of spinor strings ||^2
double a2Mmp=abs2(Mmp);
double a2Mmm=abs2(Mmm);
double a2Mpp=abs2(Mpp);
double a2Mpm=abs2(Mpm);
double sst = K/C_A*(a2Mpp+a2Mpm+a2Mmp+a2Mmm);
// Cf*Ca=4
return C_F*C_A*sst/(q1.m2()*q2.m2());
}
double jM2gg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in)
// Calculates the square of the current contractions for gg scattering
// p1: gluon
// p2: gluon
{
CLHEP::HepLorentzVector q1=p1in-p1out;
CLHEP::HepLorentzVector q2=-(p2in-p2out);
current mj1m,mj1p,mj2m,mj2p;
joi(p1out,true,p1in,true,mj1p);
joi(p1out,false,p1in,false,mj1m);
joi(p2out,true,p2in,true,mj2p);
joi(p2out,false,p2in,false,mj2m);
COM Mmp=cdot(mj1m,mj2p);
COM Mmm=cdot(mj1m,mj2m);
COM Mpp=cdot(mj1p,mj2p);
COM Mpm=cdot(mj1p,mj2m);
const double K_g1 = K_g(p1out, p1in);
const double K_g2 = K_g(p2out, p2in);
// sum of spinor strings ||^2
double a2Mmp=abs2(Mmp);
double a2Mmm=abs2(Mmm);
double a2Mpp=abs2(Mpp);
double a2Mpm=abs2(Mpm);
double sst = K_g1/C_A*K_g2/C_A*(a2Mpp+a2Mpm+a2Mmp+a2Mmm);
// Ca*Ca=9
return C_A*C_A*sst/(q1.m2()*q2.m2());
}
namespace {
/**
* @brief Higgs vertex contracted with current @param C1 and @param C2
*/
COM cHdot(const current & C1, const current & C2, const current & q1,
const current & q2, double mt, bool incBot, double mb)
{
if (mt == infinity) {
return (cdot(C1,C2)*cdot(q1,q2)-cdot(C1,q2)*cdot(C2,q1))/(6*M_PI*HEJ::vev);
}
else {
CLHEP::HepLorentzVector vq1,vq2;
vq1.set(q1[1].real(),q1[2].real(),q1[3].real(),q1[0].real());
vq2.set(q2[1].real(),q2[2].real(),q2[3].real(),q2[0].real());
// first minus sign obtained because of q1-difference to VDD
// std::cout<<"A1 : " << A1(-vq1,vq2)<<std::endl;
// std::cout<<"A2 : " << A2(-vq1,vq2)<<std::endl;
if(!(incBot))
// Factor is because 4 mt^2 g^2/HEJ::vev A1 -> 16 pi mt^2/HEJ::vev alphas,
// and we divide by a factor 4 at the amp sqaured level later
// which I absorb here (i.e. I divide by 2)
/// @TODO move factor 1/2 from S to |ME|^2 => consistent with general notation
return 8.*M_PI*mt*mt/HEJ::vev*(-cdot(C1,q2)*cdot(C2,q1)*A1(-vq1,vq2,mt)-cdot(C1,C2)*A2(-vq1,vq2,mt));
else
return 8.*M_PI*mt*mt/HEJ::vev*(-cdot(C1,q2)*cdot(C2,q1)*A1(-vq1,vq2,mt)-cdot(C1,C2)*A2(-vq1,vq2,mt))
+ 8.*M_PI*mb*mb/HEJ::vev*(-cdot(C1,q2)*cdot(C2,q1)*A1(-vq1,vq2,mb)-cdot(C1,C2)*A2(-vq1,vq2,mb));
}
}
} // namespace anonymous
double MH2qQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in,
CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in,
CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2,
double mt, bool incBot, double mb)
{
// CLHEP::HepLorentzVector q1=p1in-p1out;
// CLHEP::HepLorentzVector q2=-(p2in-p2out);
current j1p,j1m,j2p,j2m, q1v, q2v;
joi (p1out,true,p1in,true,j1p);
joi (p1out,false,p1in,false,j1m);
joi (p2out,true,p2in,true,j2p);
joi (p2out,false,p2in,false,j2m);
to_current(q1, q1v);
to_current(q2, q2v);
COM Mmp=cHdot(j1m,j2p,q1v,q2v,mt, incBot, mb);
COM Mmm=cHdot(j1m,j2m,q1v,q2v,mt, incBot, mb);
COM Mpp=cHdot(j1p,j2p,q1v,q2v,mt, incBot, mb);
COM Mpm=cHdot(j1p,j2m,q1v,q2v,mt, incBot, mb);
double sst=abs2(Mmp)+abs2(Mmm)+abs2(Mpp)+abs2(Mpm);
// return (4./3.)*(4./3.)*sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
return sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
}
double MH2qQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt, bool incBot, double mb)
{
// CLHEP::HepLorentzVector q1=p1in-p1out;
// CLHEP::HepLorentzVector q2=-(p2in-p2out);
current j1p,j1m,j2p,j2m,q1v,q2v;
joi (p1out,true,p1in,true,j1p);
joi (p1out,false,p1in,false,j1m);
jio (p2in,true,p2out,true,j2p);
jio (p2in,false,p2out,false,j2m);
to_current(q1, q1v);
to_current(q2, q2v);
COM Mmp=cHdot(j1m,j2p,q1v,q2v,mt, incBot, mb);
COM Mmm=cHdot(j1m,j2m,q1v,q2v,mt, incBot, mb);
COM Mpp=cHdot(j1p,j2p,q1v,q2v,mt, incBot, mb);
COM Mpm=cHdot(j1p,j2m,q1v,q2v,mt, incBot, mb);
double sst=abs2(Mmp)+abs2(Mmm)+abs2(Mpp)+abs2(Mpm);
// return (4./3.)*(4./3.)*sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
return sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
}
double MH2qbarQ (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt, bool incBot, double mb)
{
// CLHEP::HepLorentzVector q1=p1in-p1out;
// CLHEP::HepLorentzVector q2=-(p2in-p2out);
current j1p,j1m,j2p,j2m,q1v,q2v;
jio (p1in,true,p1out,true,j1p);
jio (p1in,false,p1out,false,j1m);
joi (p2out,true,p2in,true,j2p);
joi (p2out,false,p2in,false,j2m);
to_current(q1, q1v);
to_current(q2, q2v);
COM Mmp=cHdot(j1m,j2p,q1v,q2v,mt, incBot, mb);
COM Mmm=cHdot(j1m,j2m,q1v,q2v,mt, incBot, mb);
COM Mpp=cHdot(j1p,j2p,q1v,q2v,mt, incBot, mb);
COM Mpm=cHdot(j1p,j2m,q1v,q2v,mt, incBot, mb);
double sst=abs2(Mmp)+abs2(Mmm)+abs2(Mpp)+abs2(Mpm);
// return (4./3.)*(4./3.)*sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
return sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
}
double MH2qbarQbar (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt, bool incBot, double mb)
{
// CLHEP::HepLorentzVector q1=p1in-p1out;
// CLHEP::HepLorentzVector q2=-(p2in-p2out);
current j1p,j1m,j2p,j2m,q1v,q2v;
jio (p1in,true,p1out,true,j1p);
jio (p1in,false,p1out,false,j1m);
jio (p2in,true,p2out,true,j2p);
jio (p2in,false,p2out,false,j2m);
to_current(q1, q1v);
to_current(q2, q2v);
COM Mmp=cHdot(j1m,j2p,q1v,q2v,mt, incBot, mb);
COM Mmm=cHdot(j1m,j2m,q1v,q2v,mt, incBot, mb);
COM Mpp=cHdot(j1p,j2p,q1v,q2v,mt, incBot, mb);
COM Mpm=cHdot(j1p,j2m,q1v,q2v,mt, incBot, mb);
double sst=abs2(Mmp)+abs2(Mmm)+abs2(Mpp)+abs2(Mpm);
// return (4./3.)*(4./3.)*sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
return sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
}
double MH2qg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt, bool incBot, double mb)
// q~p1 g~p2 (i.e. ALWAYS p1 for quark, p2 for gluon)
// should be called with q1 meant to be contracted with p2 in first part of vertex
// (i.e. if g is backward, q1 is forward)
{
current j1p,j1m,j2p,j2m,q1v,q2v;
joi (p1out,true,p1in,true,j1p);
joi (p1out,false,p1in,false,j1m);
joi (p2out,true,p2in,true,j2p);
joi (p2out,false,p2in,false,j2m);
to_current(q1, q1v);
to_current(q2, q2v);
// First, calculate the non-flipping amplitudes:
COM Mpp=cHdot(j1p,j2p,q1v,q2v,mt, incBot, mb);
COM Mpm=cHdot(j1p,j2m,q1v,q2v,mt, incBot, mb);
COM Mmp=cHdot(j1m,j2p,q1v,q2v,mt, incBot, mb);
COM Mmm=cHdot(j1m,j2m,q1v,q2v,mt, incBot, mb);
//cout << "Bits in MH2qg: " << Mpp << " " << Mpm << " " << Mmp << " " << Mmm << endl;
const double K = K_g(p2out, p2in);
double sst=K/C_A*(abs2(Mmp)+abs2(Mmm)+abs2(Mpp)+abs2(Mpm));
// Cf*Ca=4
// return 4.*sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
return sst/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
}
double MH2qbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt, bool incBot, double mb)
// qbar~p1 g~p2 (i.e. ALWAYS p1 for anti-quark, p2 for gluon)
// should be called with q1 meant to be contracted with p2 in first part of vertex
// (i.e. if g is backward, q1 is forward)
{
current j1p,j1m,j2p,j2m,q1v,q2v;
jio (p1in,true,p1out,true,j1p);
jio (p1in,false,p1out,false,j1m);
joi (p2out,true,p2in,true,j2p);
joi (p2out,false,p2in,false,j2m);
to_current(q1, q1v);
to_current(q2, q2v);
// First, calculate the non-flipping amplitudes:
COM amp,amm,apm,app;
app=cHdot(j1p,j2p,q1v,q2v,mt, incBot, mb);
apm=cHdot(j1p,j2m,q1v,q2v,mt, incBot, mb);
amp=cHdot(j1m,j2p,q1v,q2v,mt, incBot, mb);
amm=cHdot(j1m,j2m,q1v,q2v,mt, incBot, mb);
double MH2sum = abs2(app)+abs2(amm)+abs2(apm)+abs2(amp);
const double K = K_g(p2out, p2in);
MH2sum*=K/C_A;
// Cf*Ca=4
// return 4.*MH2sum/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
return MH2sum/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
}
double MH2gg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mt, bool incBot, double mb)
// g~p1 g~p2
// should be called with q1 meant to be contracted with p2 in first part of vertex
// (i.e. if g is backward, q1 is forward)
{
current j1p,j1m,j2p,j2m,q1v,q2v;
joi (p1out,true,p1in,true,j1p);
joi (p1out,false,p1in,false,j1m);
joi (p2out,true,p2in,true,j2p);
joi (p2out,false,p2in,false,j2m);
to_current(q1, q1v);
to_current(q2, q2v);
// First, calculate the non-flipping amplitudes:
COM amp,amm,apm,app;
app=cHdot(j1p,j2p,q1v,q2v,mt, incBot, mb);
apm=cHdot(j1p,j2m,q1v,q2v,mt, incBot, mb);
amp=cHdot(j1m,j2p,q1v,q2v,mt, incBot, mb);
amm=cHdot(j1m,j2m,q1v,q2v,mt, incBot, mb);
double MH2sum = abs2(app)+abs2(amm)+abs2(apm)+abs2(amp);
const double K_g1 = K_g(p1out, p1in);
const double K_g2 = K_g(p2out, p2in);
MH2sum*=K_g1/C_A*K_g2/C_A;
// Ca*Ca=9
// return 9.*MH2sum/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
return MH2sum/((p1in-p1out).m2()*(p2in-p2out).m2()*q1.m2()*q2.m2());
}
// // Z's stuff
// void jZ(HLV pin, HLV pout, HLV pem, HLV pep, bool HelPartons, bool HelLeptons, current cur) {
// // Init current to zero
// cur[0] = 0.0;
// cur[1] = 0.0;
// cur[2] = 0.0;
// cur[3] = 0.0;
// // Temporary variables
// COM temp;
// current Term_1, Term_2, Term_3, Term_4, J_temp, TempCur1, TempCur2;
// // Momentum of virtual gluons aroun weak boson emission site
// HLV qa = pout + pep + pem;
// HLV qb = pin - pep - pem;
// double ta = qa.m2();
// double tb = qb.m2();
// // Out-Out currents:
// current Em_Ep, Out_Em, Out_Ep;
// // Other currents:
// current Out_In, Em_In, Ep_In;
// joi(pout, HelPartons, pin, HelPartons, Out_In);
// joi(pem, HelLeptons, pin, HelPartons, Em_In);
// joi(pep, HelLeptons, pin, HelPartons, Ep_In);
// joo(pem, HelLeptons, pep, HelLeptons, Em_Ep);
// joo(pout, HelPartons, pem, HelLeptons, Out_Em);
// joo(pout, HelPartons, pep, HelLeptons, Out_Ep);
// if (HelLeptons == HelPartons) {
// temp = 2.0 * cdot(pout, Em_Ep);
// cmult(temp / ta, Out_In, Term_1);
// temp = cdot(Out_Em, Em_Ep);
// cmult(temp / ta , Em_In, Term_2);
// temp = 2.0 * cdot(pin, Em_Ep);
// cmult(temp / tb, Out_In, Term_3);
// temp = -cdot(Ep_In, Em_Ep);
// cmult(temp / tb, Out_Ep, Term_4);
// cadd(Term_1, Term_2, Term_3, Term_4, J_temp);
// cur[0] = J_temp[0];
// cur[1] = J_temp[1];
// cur[2] = J_temp[2];
// cur[3] = J_temp[3];
// }
// else {
// if (HelPartons == true) {
// temp = 2.0 * cdot(pout, Em_Ep);
// cmult(temp / ta, Out_In, Term_1);
// joo(pout, true, pep, true, TempCur1);
// joi(pep, true, pin, true, TempCur2);
// temp = cdot(TempCur1, Em_Ep);
// cmult(temp / ta , TempCur2, Term_2);
// temp = 2.0 * cdot(pin, Em_Ep);
// cmult(temp / tb, Out_In, Term_3);
// joo(pout, true, pem, true, TempCur1);
// joi(pem, true, pin, true, TempCur2);
// temp = -cdot(TempCur2, Em_Ep);
// cmult(temp / tb, TempCur1, Term_4);
// cadd(Term_1, Term_2, Term_3, Term_4, J_temp);
// cur[0] = J_temp[0];
// cur[1] = J_temp[1];
// cur[2] = J_temp[2];
// cur[3] = J_temp[3];
// }
// else {
// temp = 2.0 * cdot(pout, Em_Ep);
// cmult(temp / ta, Out_In, Term_1);
// joo(pout, false, pep, false, TempCur1);
// joi(pep, false, pin, false, TempCur2);
// temp = cdot(TempCur1, Em_Ep);
// cmult(temp / ta, TempCur2, Term_2);
// temp = 2.0 * cdot(pin, Em_Ep);
// cmult(temp / tb, Out_In, Term_3);
// joo(pout, false, pem, false, TempCur1);
// joi(pem, false, pin, false, TempCur2);
// temp = -cdot(TempCur2, Em_Ep);
// cmult(temp / tb, TempCur1, Term_4);
// cadd(Term_1, Term_2, Term_3, Term_4, J_temp);
// cur[0] = J_temp[0];
// cur[1] = J_temp[1];
// cur[2] = J_temp[2];
// cur[3] = J_temp[3];
// }
// }
// }
// void jZbar(HLV pin, HLV pout, HLV pem, HLV pep, bool HelPartons, bool HelLeptons, current cur) {
// // Init current to zero
// cur[0] = 0.0;
// cur[1] = 0.0;
// cur[2] = 0.0;
// cur[3] = 0.0;
// // Temporary variables
// COM temp;
// current Term_1, Term_2, Term_3, Term_4, J_temp, TempCur1, TempCur2;
// // Transfered 4-momenta
// HLV qa = pout + pep + pem;
// HLV qb = pin - pep - pem;
// // The square of the transfered 4-momenta
// double ta = qa.m2();
// double tb = qb.m2();
// // Out-Out currents:
// current Em_Ep, Em_Out, Ep_Out;
// // In-Out currents:
// current In_Out, In_Em, In_Ep;
// // Safe to use the currents since helicity structure is ok
// if (HelPartons == HelLeptons) {
// jio(pin, HelPartons, pout, HelPartons, In_Out);
// joo(pem, HelLeptons, pep, HelLeptons, Em_Ep);
// jio(pin, HelPartons, pem, HelLeptons, In_Em);
// jio(pin, HelPartons, pep, HelLeptons, In_Ep);
// joo(pem, HelLeptons, pout, HelPartons, Em_Out);
// joo(pep, HelLeptons, pout, HelPartons, Ep_Out);
// }
// else {
// jio(pin, HelPartons, pout, HelPartons, In_Out);
// joo(pem, HelLeptons, pep, HelLeptons, Em_Ep);
// In_Em[0] = 0.0;
// In_Em[1] = 0.0;
// In_Em[2] = 0.0;
// In_Em[3] = 0.0;
// In_Ep[0] = 0.0;
// In_Ep[1] = 0.0;
// In_Ep[2] = 0.0;
// In_Ep[3] = 0.0;
// Em_Out[0] = 0.0;
// Em_Out[1] = 0.0;
// Em_Out[2] = 0.0;
// Em_Out[3] = 0.0;
// Ep_Out[0] = 0.0;
// Ep_Out[1] = 0.0;
// Ep_Out[2] = 0.0;
// Ep_Out[3] = 0.0;
// }
// if (HelLeptons == HelPartons) {
// temp = 2.0 * cdot(pout, Em_Ep);
// cmult(temp / ta, In_Out, Term_1);
// temp = cdot(Ep_Out, Em_Ep);
// cmult(temp / ta, In_Ep, Term_2);
// temp = 2.0 * cdot(pin, Em_Ep);
// cmult(temp / tb, In_Out, Term_3);
// temp = - cdot(In_Em, Em_Ep);
// cmult(temp / tb, Em_Out, Term_4);
// cadd(Term_1, Term_2, Term_3, Term_4, J_temp);
// cur[0] = J_temp[0];
// cur[1] = J_temp[1];
// cur[2] = J_temp[2];
// cur[3] = J_temp[3];
// }
// else {
// if (HelPartons == true) {
// temp = 2.0 * cdot(pout, Em_Ep);
// cmult(temp / ta, In_Out, Term_1);
// joo(pem, true, pout, true, TempCur1);
// jio(pin, true, pem, true, TempCur2);
// temp = cdot(TempCur1, Em_Ep);
// cmult(temp / ta , TempCur2, Term_2);
// temp = 2.0 * cdot(pin, Em_Ep);
// cmult(temp / tb, In_Out, Term_3);
// joo(pep, true, pout, true, TempCur1);
// jio(pin, true, pep, true, TempCur2);
// temp = - cdot(TempCur2, Em_Ep);
// cmult(temp / tb, TempCur1, Term_4);
// cadd(Term_1, Term_2, Term_3, Term_4, J_temp);
// cur[0] = J_temp[0];
// cur[1] = J_temp[1];
// cur[2] = J_temp[2];
// cur[3] = J_temp[3];
// }
// else {
// temp = 2.0 * cdot(pout, Em_Ep);
// cmult(temp / ta, In_Out, Term_1);
// joo(pem, false, pout, false, TempCur1);
// jio(pin, false, pem, false, TempCur2);
// temp = cdot(TempCur1, Em_Ep);
// cmult(temp / ta , TempCur2, Term_2);
// temp = 2.0 * cdot(pin, Em_Ep);
// cmult(temp / tb, In_Out, Term_3);
// joo(pep, false, pout, false, TempCur1);
// jio(pin, false, pep, false, TempCur2);
// temp = - cdot(TempCur2, Em_Ep);
// cmult(temp / tb, TempCur1, Term_4);
// cadd(Term_1, Term_2, Term_3, Term_4, J_temp);
// cur[0] = J_temp[0];
// cur[1] = J_temp[1];
// cur[2] = J_temp[2];
// cur[3] = J_temp[3];
// }
// }
// }
// // Progagators
// COM PZ(double s) {
// double MZ, GammaZ;
// MZ = 9.118800e+01; // Mass of the mediating gauge boson
// GammaZ = 2.441404e+00; // Z peak width
// // Return Z Prop value
// return 1.0 / (s - MZ * MZ + COM(0.0, 1.0) * GammaZ * MZ);
// }
// COM PG(double s) {
// return 1.0 / s;
// }
// // Non-gluonic with pa emitting
// std::vector <double> jMZqQ (HLV pa, HLV pb, HLV p1, HLV p2, HLV pep, HLV pem, std::vector <double> VProducts, std::vector < std::vector <double> > Virtuals, int aptype, int bptype, bool UseVirtuals, bool BottomLineEmit) {
// std::vector <double> ScaledWeights;
// double Sum;
// // Propagator factors
// COM PZs = PZ((pep + pem).m2());
// COM PGs = PG((pep + pem).m2());
// // Emitting current initialisation
// current j1pptop, j1pmtop; // Emission from top line
// current j1ppbot, j1pmbot; // Emission from bottom line
// // Non-emitting current initialisation
// current j2ptop, j2mtop; // Emission from top line
// current j2pbot, j2mbot; // Emission from bottom line
// // Currents for top emission
// // Upper current calculations
// // if a is a quark
// if (aptype > 0) {
// jZ(pa, p1, pem, pep, true, true, j1pptop);
// jZ(pa, p1, pem, pep, true, false, j1pmtop);
// }
// // if a is an antiquark
// else {
// jZbar(pa, p1, pem, pep, true, true, j1pptop);
// jZbar(pa, p1, pem, pep, true, false, j1pmtop);
// }
// // Lower current calculations
// // if b is a quark
// if (bptype > 0) {
// joi(p2, true, pb, true, j2ptop);
// joi(p2, false, pb, false, j2mtop);
// }
// // if b is an antiquark
// else {
// jio(pb, true, p2, true, j2ptop);
// jio(pb, false, p2, false, j2mtop);
// }
// // Currents for bottom emission
// // Lower current calculations
// if (bptype > 0) {
// jZ(pb, p2, pem, pep, true, true, j1ppbot);
// jZ(pb, p2, pem, pep, true, false, j1pmbot);
// }
// else {
// jZbar(pb, p2, pem, pep, true, true, j1ppbot);
// jZbar(pb, p2, pem, pep, true, false, j1pmbot);
// }
// // Upper current calculations
// if (aptype > 0) {
// joi(p1, true, pa, true, j2pbot);
// joi(p1, false, pa, false, j2mbot);
// }
// else {
// jio(pa, true, p1, true, j2pbot);
// jio(pa, false, p1, false, j2mbot);
// }
// COM Coeff[2][8];
// if (!Interference) {
// double ZCharge_a_P = Zq(aptype, true);
// double ZCharge_a_M = Zq(aptype, false);
// double ZCharge_b_P = Zq(bptype, true);
// double ZCharge_b_M = Zq(bptype, false);
// if (BottomLineEmit) {
// // Emission from top-line quark (pa/p1 line)
// Coeff[0][0] = (ZCharge_a_P * Zep * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pptop, j2ptop);
// Coeff[0][1] = (ZCharge_a_P * Zep * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pptop, j2mtop);
// Coeff[0][2] = (ZCharge_a_P * Zem * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pmtop, j2ptop);
// Coeff[0][3] = (ZCharge_a_P * Zem * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pmtop, j2mtop);
// Coeff[0][4] = (ZCharge_a_M * Zem * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pptop, j2ptop));
// Coeff[0][5] = (ZCharge_a_M * Zem * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pptop, j2mtop));
// Coeff[0][6] = (ZCharge_a_M * Zep * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pmtop, j2ptop));
// Coeff[0][7] = (ZCharge_a_M * Zep * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pmtop, j2mtop));
// }
// else {
// // Emission from bottom-line quark (pb/p2 line)
// Coeff[1][0] = (ZCharge_b_P * Zep * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1ppbot, j2pbot);
// Coeff[1][7] = (ZCharge_b_P * Zep * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1ppbot, j2mbot);
// Coeff[1][2] = (ZCharge_b_P * Zem * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1pmbot, j2pbot);
// Coeff[1][5] = (ZCharge_b_P * Zem * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1pmbot, j2mbot);
// Coeff[1][4] = (ZCharge_b_M * Zem * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1ppbot, j2pbot));
// Coeff[1][3] = (ZCharge_b_M * Zem * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1ppbot, j2mbot));
// Coeff[1][6] = (ZCharge_b_M * Zep * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1pmbot, j2pbot));
// Coeff[1][1] = (ZCharge_b_M * Zep * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1pmbot, j2mbot));
// }
// }
// // Else calculate all the possiblities
// else {
// double ZCharge_a_P = Zq(aptype, true);
// double ZCharge_a_M = Zq(aptype, false);
// double ZCharge_b_P = Zq(bptype, true);
// double ZCharge_b_M = Zq(bptype, false);
// // Emission from top-line quark (pa/p1 line)
// Coeff[0][0] = (ZCharge_a_P * Zep * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pptop, j2ptop);
// Coeff[0][1] = (ZCharge_a_P * Zep * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pptop, j2mtop);
// Coeff[0][2] = (ZCharge_a_P * Zem * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pmtop, j2ptop);
// Coeff[0][3] = (ZCharge_a_P * Zem * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pmtop, j2mtop);
// Coeff[0][4] = (ZCharge_a_M * Zem * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pptop, j2ptop));
// Coeff[0][5] = (ZCharge_a_M * Zem * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pptop, j2mtop));
// Coeff[0][6] = (ZCharge_a_M * Zep * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pmtop, j2ptop));
// Coeff[0][7] = (ZCharge_a_M * Zep * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pmtop, j2mtop));
// // Emission from bottom-line quark (pb/p2 line)
// Coeff[1][0] = (ZCharge_b_P * Zep * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1ppbot, j2pbot);
// Coeff[1][7] = (ZCharge_b_P * Zep * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1ppbot, j2mbot);
// Coeff[1][2] = (ZCharge_b_P * Zem * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1pmbot, j2pbot);
// Coeff[1][5] = (ZCharge_b_P * Zem * PZs * RWeak + Gq(bptype) * PGs) * cdot(j1pmbot, j2mbot);
// Coeff[1][4] = (ZCharge_b_M * Zem * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1ppbot, j2pbot));
// Coeff[1][3] = (ZCharge_b_M * Zem * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1ppbot, j2mbot));
// Coeff[1][6] = (ZCharge_b_M * Zep * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1pmbot, j2pbot));
// Coeff[1][1] = (ZCharge_b_M * Zep * PZs * RWeak + Gq(bptype) * PGs) * conj(cdot(j1pmbot, j2mbot));
// }
// // Find the numbers of scales
// int ScaleCount;
// #if calcscaleunc
// ScaleCount = 20;
// #else
// ScaleCount = 1;
// #endif
// // For each scale...
// for (int j = 0; j < ScaleCount; j++) {
// Sum = 0.0;
// // If we want to compare back to the W's code only emit from one quark and only couple to left handed particles
// // virtuals arent here since they are calculated and included in weight() call.
// if (!Interference) {
// if (BottomLineEmit) for (int i = 0; i < 8; i++) Sum += abs2(Coeff[1][i]) * VProducts.at(1);
// else for (int i = 0; i < 8; i++) Sum += abs2(Coeff[0][i]) * VProducts.at(0);
// }
// // Else work out the full interference
// else {
// // For the full calculation...
// if (UseVirtuals) {
// for (int i = 0; i < 8; i++) {
// Sum += abs2(Coeff[0][i]) * VProducts.at(0) * Virtuals.at(j).at(0)
// + abs2(Coeff[1][i]) * VProducts.at(1) * Virtuals.at(j).at(1)
// + 2.0 * real(Coeff[0][i] * conj(Coeff[1][i])) * VProducts.at(2) * Virtuals.at(j).at(2);
// }
// }
// // For the tree level calculation...
// else {
// for (int i = 0; i < 8; i++) {
// Sum += abs2(Coeff[0][i]) * VProducts.at(0)
// + abs2(Coeff[1][i]) * VProducts.at(1)
// + 2.0 * real(Coeff[0][i] * conj(Coeff[1][i])) * VProducts.at(2);
// }
// }
// }
// // Add this to the vector to be returned with the other factors of C_A and the helicity sum/average factors.
// ScaledWeights.push_back(Sum / 18.0);
// }
// // Return all the scale values
// return ScaledWeights;
// }
// // Semi-gluonic with pa emitting
// std::vector <double> jMZqg (HLV pa, HLV pb, HLV p1, HLV p2, HLV pep, HLV pem, std::vector <double> VProducts, std::vector < std::vector <double> > Virtuals, int aptype, int bptype, bool UseVirtuals, bool BottomLineEmit) {
// COM Coeff[8];
// double Sum;
// std::vector <double> ScaledWeights;
// COM PZs = PZ((pep + pem).m2());
// COM PGs = PG((pep + pem).m2());
// // Emitting current initialisation - Emission from top line
// current j1pptop, j1pmtop;
// // Non-emitting current initialisation - Emission from top line
// current j2ptop, j2mtop;
// // Currents for top emission
// // Upper current calculations
// if (aptype > 0) {
// jZ (pa, p1, pem, pep, true, true, j1pptop);
// jZ (pa, p1, pem, pep, true, false, j1pmtop);
// }
// else {
// jZbar(pa, p1, pem, pep, true, true, j1pptop);
// jZbar(pa, p1, pem, pep, true, false, j1pmtop);
// }
// // Lower current calculations
// joi(p2, true, pb, true, j2ptop);
// joi(p2, false, pb, false, j2mtop);
// // Calculate all the possiblities
// double ZCharge_a_P = Zq(aptype, true);
// double ZCharge_a_M = Zq(aptype, false);
// // Emission from top-line quark (pa/p1 line)
// Coeff[0] = (ZCharge_a_P * Zep * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pptop, j2ptop);
// Coeff[1] = (ZCharge_a_P * Zep * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pptop, j2mtop);
// Coeff[2] = (ZCharge_a_P * Zem * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pmtop, j2ptop);
// Coeff[3] = (ZCharge_a_P * Zem * PZs * RWeak + Gq(aptype) * PGs) * cdot(j1pmtop, j2mtop);
// Coeff[4] = (ZCharge_a_M * Zem * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pptop, j2ptop));
// Coeff[5] = (ZCharge_a_M * Zem * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pptop, j2mtop));
// Coeff[6] = (ZCharge_a_M * Zep * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pmtop, j2ptop));
// Coeff[7] = (ZCharge_a_M * Zep * PZs * RWeak + Gq(aptype) * PGs) * conj(cdot(j1pmtop, j2mtop));
// // Calculate gluon colour accelerated factor
// double CAMFactor, z;
// // If b is a forward moving gluon define z (C.F. multiple jets papers)
// if (pb.pz() > 0) z = p2.plus() / pb.plus();
// else z = p2.minus() / pb.minus();
// CAMFactor = (1.0 - 1.0 / 9.0) / 2.0 * (z + 1.0 / z) + 1.0 / 9.0;
// // Find the numbers of scales
// int ScaleCount;
// #if calcscaleunc
// ScaleCount = 20;
// #else
// ScaleCount = 1;
// #endif
// // For each scale...
// for (int j = 0; j < ScaleCount; j++) {
// Sum = 0.0;
// // If we dont want the interference
// if (!Interference) for (int i = 0; i < 8; i++) Sum += abs2(Coeff[i]) * VProducts.at(0);
// // Else work out the full interference
// else {
// if (UseVirtuals) {
// for (int i = 0; i < 8; i++) Sum += abs2(Coeff[i]) * VProducts.at(0) * Virtuals.at(j).at(0);
// }
// else {
// for (int i = 0; i < 8; i++) Sum += abs2(Coeff[i]) * VProducts.at(0);
// }
// }
// // Add this to the vector to be returned with the other factors of C_A, the colour accelerated factor and the helicity sum/average factors.: (4/3)*3/32
// ScaledWeights.push_back(CAMFactor * Sum / 8.0);
// }
// return ScaledWeights;
// }
// // Electroweak Charge Functions
// double Zq (int PID, bool Helcitiy) {
// double temp;
// // Positive Spin
// if (Helcitiy == true) {
// if (PID == 1 || PID == 3 || PID == 5) temp = (+ 1.0 * stw2 / 3.0) / ctw;
// if (PID == 2 || PID == 4) temp = (- 2.0 * stw2 / 3.0) / ctw;
// if (PID == -1 || PID == -3 || PID == -5) temp = (- 1.0 * stw2 / 3.0) / ctw;
// if (PID == -2 || PID == -4) temp = (+ 2.0 * stw2 / 3.0) / ctw;
// // If electron or positron
// if (PID == 7 || PID == -7) temp = Zep;
// }
// // Negative Spin
// else {
// if (PID == 1 || PID == 3 || PID == 5) temp = (-0.5 + 1.0 * stw2 / 3.0) / ctw;
// if (PID == 2 || PID == 4) temp = ( 0.5 - 2.0 * stw2 / 3.0) / ctw;
// if (PID == -1 || PID == -3 || PID == -5) temp = ( 0.5 - 1.0 * stw2 / 3.0) / ctw;
// if (PID == -2 || PID == -4) temp = (-0.5 + 2.0 * stw2 / 3.0) / ctw;
// // If electron or positron
// if (PID == 7 || PID == -7) temp = Zem;
// }
// return temp;
// }
// double Gq (int PID) {
// if (!VirtualPhoton) return 0.0;
// if (PID == -1) return 1.0 * ee / 3.0;
// if (PID == -2) return -2.0 * ee / 3.0;
// if (PID == -3) return 1.0 * ee / 3.0;
// if (PID == -4) return -2.0 * ee / 3.0;
// if (PID == -5) return 1.0 * ee / 3.0;
// if (PID == 1) return -1.0 * ee / 3.0;
// if (PID == 2) return 2.0 * ee / 3.0;
// if (PID == 3) return -1.0 * ee / 3.0;
// if (PID == 4) return 2.0 * ee / 3.0;
// if (PID == 5) return -1.0 * ee / 3.0;
// std::cout << "ERROR! No Electroweak Charge Found at line " << __LINE__ << "..." << std::endl;
// return 0.0;
// }
namespace {
//@{
/// @brief Higgs vertex contracted with one current
CCurrent jH (CLHEP::HepLorentzVector pout, bool helout, CLHEP::HepLorentzVector pin,
bool helin, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2,
double mt, bool incBot, double mb)
{
CCurrent j2 = joi(pout,helout,pin,helin);
CCurrent jq2(q2.e(),q2.px(),q2.py(),q2.pz());
if(mt == infinity)
return ((q1.dot(q2))*j2 - j2.dot(q1)*jq2)/(3*M_PI*HEJ::vev);
else
{
if(incBot)
return (-16.*M_PI*mb*mb/HEJ::vev*j2.dot(q1)*jq2*A1(-q1,q2,mb)-16.*M_PI*mb*mb/HEJ::vev*j2*A2(-q1,q2,mb))
+ (-16.*M_PI*mt*mt/HEJ::vev*j2.dot(q1)*jq2*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j2*A2(-q1,q2,mt));
else
return (-16.*M_PI*mt*mt/HEJ::vev*j2.dot(q1)*jq2*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j2*A2(-q1,q2,mt));
}
}
CCurrent jioH (CLHEP::HepLorentzVector pin, bool helin, CLHEP::HepLorentzVector pout,
bool helout, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2,
double mt, bool incBot, double mb)
{
CCurrent j2 = jio(pin,helin,pout,helout);
CCurrent jq2(q2.e(),q2.px(),q2.py(),q2.pz());
if(mt == infinity)
return ((q1.dot(q2))*j2 - j2.dot(q1)*jq2)/(3*M_PI*HEJ::vev);
else
{
if(incBot)
return (-16.*M_PI*mb*mb/HEJ::vev*j2.dot(q1)*jq2*A1(-q1,q2,mb)-16.*M_PI*mb*mb/HEJ::vev*j2*A2(-q1,q2,mb))
+ (-16.*M_PI*mt*mt/HEJ::vev*j2.dot(q1)*jq2*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j2*A2(-q1,q2,mt));
else
return (-16.*M_PI*mt*mt/HEJ::vev*j2.dot(q1)*jq2*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j2*A2(-q1,q2,mt));
}
}
CCurrent jHtop (CLHEP::HepLorentzVector pout, bool helout, CLHEP::HepLorentzVector pin,
bool helin, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2,
double mt, bool incBot, double mb)
{
CCurrent j1 = joi(pout,helout,pin,helin);
CCurrent jq1(q1.e(),q1.px(),q1.py(),q1.pz());
if(mt == infinity)
return ((q1.dot(q2))*j1 - j1.dot(q2)*jq1)/(3*M_PI*HEJ::vev);
else
{
if(incBot)
return (-16.*M_PI*mb*mb/HEJ::vev*j1.dot(q2)*jq1*A1(-q1,q2,mb)-16.*M_PI*mb*mb/HEJ::vev*j1*A2(-q1,q2,mb))
+ (-16.*M_PI*mt*mt/HEJ::vev*j1.dot(q2)*jq1*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j1*A2(-q1,q2,mt));
else
return (-16.*M_PI*mt*mt/HEJ::vev*j1.dot(q2)*jq1*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j1*A2(-q1,q2,mt));
}
}
CCurrent jioHtop (CLHEP::HepLorentzVector pin, bool helin, CLHEP::HepLorentzVector pout,
bool helout, CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2,
double mt, bool incBot, double mb)
{
CCurrent j1 = jio(pin,helin,pout,helout);
CCurrent jq1(q1.e(),q1.px(),q1.py(),q1.pz());
if(mt == infinity)
return ((q1.dot(q2))*j1 - j1.dot(q2)*jq1)/(3*M_PI*HEJ::vev);
else
{
if(incBot)
return (-16.*M_PI*mb*mb/HEJ::vev*j1.dot(q2)*jq1*A1(-q1,q2,mb)-16.*M_PI*mb*mb/HEJ::vev*j1*A2(-q1,q2,mb))
+ (-16.*M_PI*mt*mt/HEJ::vev*j1.dot(q2)*jq1*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j1*A2(-q1,q2,mt));
else
return (-16.*M_PI*mt*mt/HEJ::vev*j1.dot(q2)*jq1*A1(-q1,q2,mt)-16.*M_PI*mt*mt/HEJ::vev*j1*A2(-q1,q2,mt));
}
}
//@}
} // namespace anonymous
double jM2unogqHQ (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// This construction is taking rapidity order: pg > p1out >> p2out
// std::cerr<<"This Uno Current: "<<p1out<<" "<<p1in<<" "<<p2out<<" "<<p2in<<" "<<pg<<std::endl;
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out); // Bottom End
CLHEP::HepLorentzVector qg=p1in-p1out-pg; // Extra bit post-gluon
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mj1m,mj1p,mj2m,mj2p,mjH2m,mjH2p;
mj1p=joi(p1out,true,p1in,true);
mj1m=joi(p1out,false,p1in,false);
mjH2p=jH(p2out,true,p2in,true,qH1,qH2, mt, incBot, mb);
mjH2m=jH(p2out,false,p2in,false,qH1,qH2, mt, incBot, mb);
// Dot products of these which occur again and again
COM MHmp=mj1m.dot(mjH2p); // And now for the Higgs ones
COM MHmm=mj1m.dot(mjH2m);
COM MHpp=mj1p.dot(mjH2p);
COM MHpm=mj1p.dot(mjH2m);
// std::cout<< p1out.rapidity() << " " << p2out.rapidity()<< " " << qH1 << " " << qH2 << "\n" <<MHmm << " " << MHmp << " " << MHpm << " " << MHpp << std::endl;
// Currents with pg
CCurrent jgam,jgap,j2gm,j2gp;
j2gp=joo(p1out,true,pg,true);
j2gm=joo(p1out,false,pg,false);
jgap=joi(pg,true,p1in,true);
jgam=joi(pg,false,p1in,false);
CCurrent qsum(q1+qg);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p2o(p2out),p2i(p2in);
CCurrent p1o(p1out);
CCurrent p1i(p1in);
Lmm=(qsum*(MHmm) + (-2.*mjH2m.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmm/2.))/q1.m2();
Lmp=(qsum*(MHmp) + (-2.*mjH2p.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmp/2.))/q1.m2();
Lpm=(qsum*(MHpm) + (-2.*mjH2m.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpm/2.))/q1.m2();
Lpp=(qsum*(MHpp) + (-2.*mjH2p.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpp/2.))/q1.m2();
U1mm=(jgam.dot(mjH2m)*j2gm+2.*p1o*MHmm)/(p1out+pg).m2();
U1mp=(jgam.dot(mjH2p)*j2gm+2.*p1o*MHmp)/(p1out+pg).m2();
U1pm=(jgap.dot(mjH2m)*j2gp+2.*p1o*MHpm)/(p1out+pg).m2();
U1pp=(jgap.dot(mjH2p)*j2gp+2.*p1o*MHpp)/(p1out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH2m)*jgam+2.*p1i*MHmm)/(p1in-pg).m2();
U2mp=((-1.)*j2gm.dot(mjH2p)*jgam+2.*p1i*MHmp)/(p1in-pg).m2();
U2pm=((-1.)*j2gp.dot(mjH2m)*jgap+2.*p1i*MHpm)/(p1in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH2p)*jgap+2.*p1i*MHpp)/(p1in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q2.m2()*qH2.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH1.m2()*qg.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=HEJ::C_F*HEJ::C_F/HEJ::C_A/HEJ::C_A; // Factor of (Cf/Ca) for each quark to match MH2qQ.
//Higgs coupling is included in Hjets.C
return ampsq;
}
double jM2unogqbarHQ (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// This construction is taking rapidity order: pg > p1out >> p2out
// std::cerr<<"This Uno Current: "<<p1out<<" "<<p1in<<" "<<p2out<<" "<<p2in<<" "<<pg<<std::endl;
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out); // Bottom End
CLHEP::HepLorentzVector qg=p1in-p1out-pg; // Extra bit post-gluon
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mj1m,mj1p,mj2m,mj2p,mjH2m,mjH2p;
mj1p=jio(p1in,true,p1out,true);
mj1m=jio(p1in,false,p1out,false);
mjH2p=jH(p2out,true,p2in,true,qH1,qH2, mt, incBot, mb);
mjH2m=jH(p2out,false,p2in,false,qH1,qH2, mt, incBot, mb);
// Dot products of these which occur again and again
COM MHmp=mj1m.dot(mjH2p); // And now for the Higgs ones
COM MHmm=mj1m.dot(mjH2m);
COM MHpp=mj1p.dot(mjH2p);
COM MHpm=mj1p.dot(mjH2m);
// Currents with pg
CCurrent jgam,jgap,j2gm,j2gp;
j2gp=joo(pg,true,p1out,true);
j2gm=joo(pg,false,p1out,false);
jgap=jio(p1in,true,pg,true);
jgam=jio(p1in,false,pg,false);
CCurrent qsum(q1+qg);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p2o(p2out),p2i(p2in);
CCurrent p1o(p1out);
CCurrent p1i(p1in);
Lmm=(qsum*(MHmm) + (-2.*mjH2m.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmm/2.))/q1.m2();
Lmp=(qsum*(MHmp) + (-2.*mjH2p.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmp/2.))/q1.m2();
Lpm=(qsum*(MHpm) + (-2.*mjH2m.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpm/2.))/q1.m2();
Lpp=(qsum*(MHpp) + (-2.*mjH2p.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpp/2.))/q1.m2();
U1mm=(jgam.dot(mjH2m)*j2gm+2.*p1o*MHmm)/(p1out+pg).m2();
U1mp=(jgam.dot(mjH2p)*j2gm+2.*p1o*MHmp)/(p1out+pg).m2();
U1pm=(jgap.dot(mjH2m)*j2gp+2.*p1o*MHpm)/(p1out+pg).m2();
U1pp=(jgap.dot(mjH2p)*j2gp+2.*p1o*MHpp)/(p1out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH2m)*jgam+2.*p1i*MHmm)/(p1in-pg).m2();
U2mp=((-1.)*j2gm.dot(mjH2p)*jgam+2.*p1i*MHmp)/(p1in-pg).m2();
U2pm=((-1.)*j2gp.dot(mjH2m)*jgap+2.*p1i*MHpm)/(p1in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH2p)*jgap+2.*p1i*MHpp)/(p1in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q2.m2()*qH2.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH1.m2()*qg.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4.*4./(9.*9.); // Factor of (Cf/Ca) for each quark to match MH2qQ.
//Higgs coupling is included in Hjets.C
return ampsq;
}
double jM2unogqHQbar (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// This construction is taking rapidity order: pg > p1out >> p2out
// std::cerr<<"This Uno Current: "<<p1out<<" "<<p1in<<" "<<p2out<<" "<<p2in<<" "<<pg<<std::endl;
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out); // Bottom End
CLHEP::HepLorentzVector qg=p1in-p1out-pg; // Extra bit post-gluon
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mj1m,mj1p,mj2m,mj2p,mjH2m,mjH2p;
mj1p=joi(p1out,true,p1in,true);
mj1m=joi(p1out,false,p1in,false);
mjH2p=jioH(p2in,true,p2out,true,qH1,qH2, mt, incBot, mb);
mjH2m=jioH(p2in,false,p2out,false,qH1,qH2, mt, incBot, mb);
// Dot products of these which occur again and again
COM MHmp=mj1m.dot(mjH2p); // And now for the Higgs ones
COM MHmm=mj1m.dot(mjH2m);
COM MHpp=mj1p.dot(mjH2p);
COM MHpm=mj1p.dot(mjH2m);
// Currents with pg
CCurrent jgam,jgap,j2gm,j2gp;
j2gp=joo(p1out,true,pg,true);
j2gm=joo(p1out,false,pg,false);
jgap=joi(pg,true,p1in,true);
jgam=joi(pg,false,p1in,false);
CCurrent qsum(q1+qg);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p2o(p2out),p2i(p2in);
CCurrent p1o(p1out);
CCurrent p1i(p1in);
Lmm=(qsum*(MHmm) + (-2.*mjH2m.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmm/2.))/q1.m2();
Lmp=(qsum*(MHmp) + (-2.*mjH2p.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmp/2.))/q1.m2();
Lpm=(qsum*(MHpm) + (-2.*mjH2m.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpm/2.))/q1.m2();
Lpp=(qsum*(MHpp) + (-2.*mjH2p.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpp/2.))/q1.m2();
U1mm=(jgam.dot(mjH2m)*j2gm+2.*p1o*MHmm)/(p1out+pg).m2();
U1mp=(jgam.dot(mjH2p)*j2gm+2.*p1o*MHmp)/(p1out+pg).m2();
U1pm=(jgap.dot(mjH2m)*j2gp+2.*p1o*MHpm)/(p1out+pg).m2();
U1pp=(jgap.dot(mjH2p)*j2gp+2.*p1o*MHpp)/(p1out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH2m)*jgam+2.*p1i*MHmm)/(p1in-pg).m2();
U2mp=((-1.)*j2gm.dot(mjH2p)*jgam+2.*p1i*MHmp)/(p1in-pg).m2();
U2pm=((-1.)*j2gp.dot(mjH2m)*jgap+2.*p1i*MHpm)/(p1in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH2p)*jgap+2.*p1i*MHpp)/(p1in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q2.m2()*qH2.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH1.m2()*qg.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4.*4./(9.*9.); // Factor of (Cf/Ca) for each quark to match MH2qQ.
//Higgs coupling is included in Hjets.C
return ampsq;
}
double jM2unogqbarHQbar (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// This construction is taking rapidity order: pg > p1out >> p2out
// std::cerr<<"This Uno Current: "<<p1out<<" "<<p1in<<" "<<p2out<<" "<<p2in<<" "<<pg<<std::endl;
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out); // Bottom End
CLHEP::HepLorentzVector qg=p1in-p1out-pg; // Extra bit post-gluon
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mj1m,mj1p,mj2m,mj2p,mjH2m,mjH2p;
mj1p=jio(p1in,true,p1out,true);
mj1m=jio(p1in,false,p1out,false);
mjH2p=jioH(p2in,true,p2out,true,qH1,qH2, mt, incBot, mb);
mjH2m=jioH(p2in,false,p2out,false,qH1,qH2, mt, incBot, mb);
// Dot products of these which occur again and again
COM MHmp=mj1m.dot(mjH2p); // And now for the Higgs ones
COM MHmm=mj1m.dot(mjH2m);
COM MHpp=mj1p.dot(mjH2p);
COM MHpm=mj1p.dot(mjH2m);
// Currents with pg
CCurrent jgam,jgap,j2gm,j2gp;
j2gp=joo(pg,true,p1out,true);
j2gm=joo(pg,false,p1out,false);
jgap=jio(p1in,true,pg,true);
jgam=jio(p1in,false,pg,false);
CCurrent qsum(q1+qg);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p2o(p2out),p2i(p2in);
CCurrent p1o(p1out);
CCurrent p1i(p1in);
Lmm=(qsum*(MHmm) + (-2.*mjH2m.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmm/2.))/q1.m2();
Lmp=(qsum*(MHmp) + (-2.*mjH2p.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmp/2.))/q1.m2();
Lpm=(qsum*(MHpm) + (-2.*mjH2m.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpm/2.))/q1.m2();
Lpp=(qsum*(MHpp) + (-2.*mjH2p.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpp/2.))/q1.m2();
U1mm=(jgam.dot(mjH2m)*j2gm+2.*p1o*MHmm)/(p1out+pg).m2();
U1mp=(jgam.dot(mjH2p)*j2gm+2.*p1o*MHmp)/(p1out+pg).m2();
U1pm=(jgap.dot(mjH2m)*j2gp+2.*p1o*MHpm)/(p1out+pg).m2();
U1pp=(jgap.dot(mjH2p)*j2gp+2.*p1o*MHpp)/(p1out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH2m)*jgam+2.*p1i*MHmm)/(p1in-pg).m2();
U2mp=((-1.)*j2gm.dot(mjH2p)*jgam+2.*p1i*MHmp)/(p1in-pg).m2();
U2pm=((-1.)*j2gp.dot(mjH2m)*jgap+2.*p1i*MHpm)/(p1in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH2p)*jgap+2.*p1i*MHpp)/(p1in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q2.m2()*qH2.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH1.m2()*qg.m2();
ampsq/=th;
ampsq/=16.;
//Higgs coupling is included in Hjets.C
ampsq*=4.*4./(9.*9.); // Factor of (Cf/Ca) for each quark to match MH2qQ.
return ampsq;
}
double jM2unogqHg (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// This construction is taking rapidity order: pg > p1out >> p2out
// std::cerr<<"This Uno Current: "<<p1out<<" "<<p1in<<" "<<p2out<<" "<<p2in<<" "<<pg<<std::endl;
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out); // Bottom End
CLHEP::HepLorentzVector qg=p1in-p1out-pg; // Extra bit post-gluon
CCurrent mj1m,mj1p,mj2m,mj2p,mjH2m,mjH2p;
mj1p=joi(p1out,true,p1in,true);
mj1m=joi(p1out,false,p1in,false);
mjH2p=jH(p2out,true,p2in,true,qH1,qH2, mt, incBot, mb);
mjH2m=jH(p2out,false,p2in,false,qH1,qH2, mt, incBot, mb);
// Dot products of these which occur again and again
COM MHmp=mj1m.dot(mjH2p); // And now for the Higgs ones
COM MHmm=mj1m.dot(mjH2m);
COM MHpp=mj1p.dot(mjH2p);
COM MHpm=mj1p.dot(mjH2m);
// Currents with pg
CCurrent jgam,jgap,j2gm,j2gp;
j2gp=joo(p1out,true,pg,true);
j2gm=joo(p1out,false,pg,false);
jgap=joi(pg,true,p1in,true);
jgam=joi(pg,false,p1in,false);
CCurrent qsum(q1+qg);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p2o(p2out),p2i(p2in);
CCurrent p1o(p1out);
CCurrent p1i(p1in);
Lmm=(qsum*(MHmm) + (-2.*mjH2m.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmm/2.))/q1.m2();
Lmp=(qsum*(MHmp) + (-2.*mjH2p.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmp/2.))/q1.m2();
Lpm=(qsum*(MHpm) + (-2.*mjH2m.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpm/2.))/q1.m2();
Lpp=(qsum*(MHpp) + (-2.*mjH2p.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpp/2.))/q1.m2();
U1mm=(jgam.dot(mjH2m)*j2gm+2.*p1o*MHmm)/(p1out+pg).m2();
U1mp=(jgam.dot(mjH2p)*j2gm+2.*p1o*MHmp)/(p1out+pg).m2();
U1pm=(jgap.dot(mjH2m)*j2gp+2.*p1o*MHpm)/(p1out+pg).m2();
U1pp=(jgap.dot(mjH2p)*j2gp+2.*p1o*MHpp)/(p1out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH2m)*jgam+2.*p1i*MHmm)/(p1in-pg).m2();
U2mp=((-1.)*j2gm.dot(mjH2p)*jgam+2.*p1i*MHmp)/(p1in-pg).m2();
U2pm=((-1.)*j2gp.dot(mjH2m)*jgap+2.*p1i*MHpm)/(p1in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH2p)*jgap+2.*p1i*MHpp)/(p1in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q2.m2()*qH2.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH1.m2()*qg.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4./9.*4./9.; // Factor of (Cf/Ca) for each quark to match MH2qQ.
// here we need 2 to match with the normalization
// gq is 9./4. times the qQ
//Higgs coupling is included in Hjets.C
const double K = K_g(p2out, p2in);
return ampsq*K/C_A*9./4.; //ca/cf = 9/4
}
double jM2unogqbarHg (CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// This construction is taking rapidity order: pg > p1out >> p2out
// std::cerr<<"This Uno Current: "<<p1out<<" "<<p1in<<" "<<p2out<<" "<<p2in<<" "<<pg<<std::endl;
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out); // Bottom End
CLHEP::HepLorentzVector qg=p1in-p1out-pg; // Extra bit post-gluon
CCurrent mj1m,mj1p,mj2m,mj2p,mjH2m,mjH2p;
mj1p=jio(p1in,true,p1out,true);
mj1m=jio(p1in,false,p1out,false);
mjH2p=jH(p2out,true,p2in,true,qH1,qH2, mt, incBot, mb);
mjH2m=jH(p2out,false,p2in,false,qH1,qH2, mt, incBot, mb);
// Dot products of these which occur again and again
COM MHmp=mj1m.dot(mjH2p); // And now for the Higgs ones
COM MHmm=mj1m.dot(mjH2m);
COM MHpp=mj1p.dot(mjH2p);
COM MHpm=mj1p.dot(mjH2m);
// Currents with pg
CCurrent jgam,jgap,j2gm,j2gp;
j2gp=joo(pg,true,p1out,true);
j2gm=joo(pg,false,p1out,false);
jgap=jio(p1in,true,pg,true);
jgam=jio(p1in,false,pg,false);
CCurrent qsum(q1+qg);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p2o(p2out),p2i(p2in);
CCurrent p1o(p1out);
CCurrent p1i(p1in);
Lmm=(qsum*(MHmm) + (-2.*mjH2m.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmm/2.))/q1.m2();
Lmp=(qsum*(MHmp) + (-2.*mjH2p.dot(pg))*mj1m+2.*mj1m.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHmp/2.))/q1.m2();
Lpm=(qsum*(MHpm) + (-2.*mjH2m.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2m+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpm/2.))/q1.m2();
Lpp=(qsum*(MHpp) + (-2.*mjH2p.dot(pg))*mj1p+2.*mj1p.dot(pg)*mjH2p+(p2o/pg.dot(p2out) + p2i/pg.dot(p2in))*(qg.m2()*MHpp/2.))/q1.m2();
U1mm=(jgam.dot(mjH2m)*j2gm+2.*p1o*MHmm)/(p1out+pg).m2();
U1mp=(jgam.dot(mjH2p)*j2gm+2.*p1o*MHmp)/(p1out+pg).m2();
U1pm=(jgap.dot(mjH2m)*j2gp+2.*p1o*MHpm)/(p1out+pg).m2();
U1pp=(jgap.dot(mjH2p)*j2gp+2.*p1o*MHpp)/(p1out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH2m)*jgam+2.*p1i*MHmm)/(p1in-pg).m2();
U2mp=((-1.)*j2gm.dot(mjH2p)*jgam+2.*p1i*MHmp)/(p1in-pg).m2();
U2pm=((-1.)*j2gp.dot(mjH2m)*jgap+2.*p1i*MHpm)/(p1in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH2p)*jgap+2.*p1i*MHpp)/(p1in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q2.m2()*qH2.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH1.m2()*qg.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4./9.*4./9.; // Factor of (Cf/Ca) for each quark to match MH2qQ.
// here we need 2 to match with the normalization
// gq is 9./4. times the qQ
//Higgs coupling is included in Hjets.C
const double K = K_g(p2out, p2in);
return ampsq*K/C_F;
}
double jM2unobqHQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// std::cout << "####################\n";
// std::cout << "# p1in : "<<p1in<< " "<<p1in.plus()<<" "<<p1in.minus()<<std::endl;
// std::cout << "# p2in : "<<p2in<< " "<<p2in.plus()<<" "<<p2in.minus()<<std::endl;
// std::cout << "# p1out : "<<p1out<< " "<<p1out.rapidity()<<std::endl;
// std::cout << "# (qH1-qH2) : "<<(qH1-qH2)<< " "<<(qH1-qH2).rapidity()<<std::endl;
// std::cout << "# pg : "<<pg<< " "<<pg.rapidity()<<std::endl;
// std::cout << "# p2out : "<<p2out<< " "<<p2out.rapidity()<<std::endl;
// std::cout << "####################\n";
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out-pg); // Extra bit pre-gluon
CLHEP::HepLorentzVector q3=-(p2in-p2out); // Bottom End
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mjH1m,mjH1p,mj2m,mj2p;
mjH1p=jHtop(p1out,true,p1in,true,qH1,qH2, mt, incBot, mb);
mjH1m=jHtop(p1out,false,p1in,false,qH1,qH2, mt, incBot, mb);
mj2p=joi(p2out,true,p2in,true);
mj2m=joi(p2out,false,p2in,false);
// Dot products of these which occur again and again
COM MHmp=mjH1m.dot(mj2p); // And now for the Higgs ones
COM MHmm=mjH1m.dot(mj2m);
COM MHpp=mjH1p.dot(mj2p);
COM MHpm=mjH1p.dot(mj2m);
// Currents with pg
CCurrent jgbm,jgbp,j2gm,j2gp;
j2gp=joo(p2out,true,pg,true);
j2gm=joo(p2out,false,pg,false);
jgbp=joi(pg,true,p2in,true);
jgbm=joi(pg,false,p2in,false);
CCurrent qsum(q2+q3);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p1o(p1out),p1i(p1in);
CCurrent p2o(p2out);
CCurrent p2i(p2in);
CCurrent pplus((p1in+p1out)/2.);
CCurrent pminus((p2in+p2out)/2.);
// COM test=pminus.dot(p1in);
Lmm=((-1.)*qsum*(MHmm) + (-2.*mjH1m.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1m
+ (p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmm/2.))/q3.m2();
Lmp=((-1.)*qsum*(MHmp) + (-2.*mjH1m.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1m
+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmp/2.))/q3.m2();
Lpm=((-1.)*qsum*(MHpm) + (-2.*mjH1p.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1p
+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpm/2.))/q3.m2();
Lpp=((-1.)*qsum*(MHpp) + (-2.*mjH1p.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1p
+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpp/2.))/q3.m2();
U1mm=(jgbm.dot(mjH1m)*j2gm+2.*p2o*MHmm)/(p2out+pg).m2();
U1mp=(jgbp.dot(mjH1m)*j2gp+2.*p2o*MHmp)/(p2out+pg).m2();
U1pm=(jgbm.dot(mjH1p)*j2gm+2.*p2o*MHpm)/(p2out+pg).m2();
U1pp=(jgbp.dot(mjH1p)*j2gp+2.*p2o*MHpp)/(p2out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH1m)*jgbm+2.*p2i*MHmm)/(p2in-pg).m2();
U2mp=((-1.)*j2gp.dot(mjH1m)*jgbp+2.*p2i*MHmp)/(p2in-pg).m2();
U2pm=((-1.)*j2gm.dot(mjH1p)*jgbm+2.*p2i*MHpm)/(p2in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH1p)*jgbp+2.*p2i*MHpp)/(p2in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
// 1/3. = 1/C_A ?
double ampsq=-(amm+amp+apm+app)/(q1.m2()*qH1.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
const double th=qH2.m2()*q2.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=HEJ::C_F*HEJ::C_F/(HEJ::C_A*HEJ::C_A); // Factor of (Cf/Ca) for each quark to match MH2qQ.
return ampsq;
}
double jM2unobqbarHQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out-pg); // Extra bit pre-gluon
CLHEP::HepLorentzVector q3=-(p2in-p2out); // Bottom End
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mjH1m,mjH1p,mj2m,mj2p;
mjH1p=jioHtop(p1in,true,p1out,true,qH1,qH2, mt, incBot, mb);
mjH1m=jioHtop(p1in,false,p1out,false,qH1,qH2, mt, incBot, mb);
mj2p=joi(p2out,true,p2in,true);
mj2m=joi(p2out,false,p2in,false);
// Dot products of these which occur again and again
COM MHmp=mjH1m.dot(mj2p); // And now for the Higgs ones
COM MHmm=mjH1m.dot(mj2m);
COM MHpp=mjH1p.dot(mj2p);
COM MHpm=mjH1p.dot(mj2m);
// Currents with pg
CCurrent jgbm,jgbp,j2gm,j2gp;
j2gp=joo(p2out,true,pg,true);
j2gm=joo(p2out,false,pg,false);
jgbp=joi(pg,true,p2in,true);
jgbm=joi(pg,false,p2in,false);
CCurrent qsum(q2+q3);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p1o(p1out),p1i(p1in);
CCurrent p2o(p2out);
CCurrent p2i(p2in);
CCurrent pplus((p1in+p1out)/2.);
CCurrent pminus((p2in+p2out)/2.);
// COM test=pminus.dot(p1in);
Lmm=((-1.)*qsum*(MHmm) + (-2.*mjH1m.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmm/2.))/q3.m2();
Lmp=((-1.)*qsum*(MHmp) + (-2.*mjH1m.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmp/2.))/q3.m2();
Lpm=((-1.)*qsum*(MHpm) + (-2.*mjH1p.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpm/2.))/q3.m2();
Lpp=((-1.)*qsum*(MHpp) + (-2.*mjH1p.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpp/2.))/q3.m2();
U1mm=(jgbm.dot(mjH1m)*j2gm+2.*p2o*MHmm)/(p2out+pg).m2();
U1mp=(jgbp.dot(mjH1m)*j2gp+2.*p2o*MHmp)/(p2out+pg).m2();
U1pm=(jgbm.dot(mjH1p)*j2gm+2.*p2o*MHpm)/(p2out+pg).m2();
U1pp=(jgbp.dot(mjH1p)*j2gp+2.*p2o*MHpp)/(p2out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH1m)*jgbm+2.*p2i*MHmm)/(p2in-pg).m2();
U2mp=((-1.)*j2gp.dot(mjH1m)*jgbp+2.*p2i*MHmp)/(p2in-pg).m2();
U2pm=((-1.)*j2gm.dot(mjH1p)*jgbm+2.*p2i*MHpm)/(p2in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH1p)*jgbp+2.*p2i*MHpp)/(p2in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q1.m2()*qH1.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH2.m2()*q2.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4.*4./(9.*9.); // Factor of (Cf/Ca) for each quark to match MH2qQ.
//Higgs coupling is included in Hjets.C
return ampsq;
}
double jM2unobqHQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out-pg); // Extra bit pre-gluon
CLHEP::HepLorentzVector q3=-(p2in-p2out); // Bottom End
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mjH1m,mjH1p,mj2m,mj2p;
mjH1p=jHtop(p1out,true,p1in,true,qH1,qH2,mt, incBot, mb);
mjH1m=jHtop(p1out,false,p1in,false,qH1,qH2,mt, incBot, mb);
mj2p=jio(p2in,true,p2out,true);
mj2m=jio(p2in,false,p2out,false);
// Dot products of these which occur again and again
COM MHmp=mjH1m.dot(mj2p); // And now for the Higgs ones
COM MHmm=mjH1m.dot(mj2m);
COM MHpp=mjH1p.dot(mj2p);
COM MHpm=mjH1p.dot(mj2m);
// Currents with pg
CCurrent jgbm,jgbp,j2gm,j2gp;
j2gp=joo(pg,true,p2out,true);
j2gm=joo(pg,false,p2out,false);
jgbp=jio(p2in,true,pg,true);
jgbm=jio(p2in,false,pg,false);
CCurrent qsum(q2+q3);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p1o(p1out),p1i(p1in);
CCurrent p2o(p2out);
CCurrent p2i(p2in);
CCurrent pplus((p1in+p1out)/2.);
CCurrent pminus((p2in+p2out)/2.);
// COM test=pminus.dot(p1in);
Lmm=((-1.)*qsum*(MHmm) + (-2.*mjH1m.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmm/2.))/q3.m2();
Lmp=((-1.)*qsum*(MHmp) + (-2.*mjH1m.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmp/2.))/q3.m2();
Lpm=((-1.)*qsum*(MHpm) + (-2.*mjH1p.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpm/2.))/q3.m2();
Lpp=((-1.)*qsum*(MHpp) + (-2.*mjH1p.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpp/2.))/q3.m2();
U1mm=(jgbm.dot(mjH1m)*j2gm+2.*p2o*MHmm)/(p2out+pg).m2();
U1mp=(jgbp.dot(mjH1m)*j2gp+2.*p2o*MHmp)/(p2out+pg).m2();
U1pm=(jgbm.dot(mjH1p)*j2gm+2.*p2o*MHpm)/(p2out+pg).m2();
U1pp=(jgbp.dot(mjH1p)*j2gp+2.*p2o*MHpp)/(p2out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH1m)*jgbm+2.*p2i*MHmm)/(p2in-pg).m2();
U2mp=((-1.)*j2gp.dot(mjH1m)*jgbp+2.*p2i*MHmp)/(p2in-pg).m2();
U2pm=((-1.)*j2gm.dot(mjH1p)*jgbm+2.*p2i*MHpm)/(p2in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH1p)*jgbp+2.*p2i*MHpp)/(p2in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q1.m2()*qH1.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH2.m2()*q2.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4.*4./(9.*9.); // Factor of (Cf/Ca) for each quark to match MH2qQ.
//Higgs coupling is included in Hjets.C
return ampsq;
}
double jM2unobqbarHQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out-pg); // Extra bit pre-gluon
CLHEP::HepLorentzVector q3=-(p2in-p2out); // Bottom End
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mjH1m,mjH1p,mj2m,mj2p;
mjH1p=jioHtop(p1in,true,p1out,true,qH1,qH2,mt, incBot, mb);
mjH1m=jioHtop(p1in,false,p1out,false,qH1,qH2,mt, incBot, mb);
mj2p=jio(p2in,true,p2out,true);
mj2m=jio(p2in,false,p2out,false);
// Dot products of these which occur again and again
COM MHmp=mjH1m.dot(mj2p); // And now for the Higgs ones
COM MHmm=mjH1m.dot(mj2m);
COM MHpp=mjH1p.dot(mj2p);
COM MHpm=mjH1p.dot(mj2m);
// Currents with pg
CCurrent jgbm,jgbp,j2gm,j2gp;
j2gp=joo(pg,true,p2out,true);
j2gm=joo(pg,false,p2out,false);
jgbp=jio(p2in,true,pg,true);
jgbm=jio(p2in,false,pg,false);
CCurrent qsum(q2+q3);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p1o(p1out),p1i(p1in);
CCurrent p2o(p2out);
CCurrent p2i(p2in);
CCurrent pplus((p1in+p1out)/2.);
CCurrent pminus((p2in+p2out)/2.);
// COM test=pminus.dot(p1in);
Lmm=((-1.)*qsum*(MHmm) + (-2.*mjH1m.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmm/2.))/q3.m2();
Lmp=((-1.)*qsum*(MHmp) + (-2.*mjH1m.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmp/2.))/q3.m2();
Lpm=((-1.)*qsum*(MHpm) + (-2.*mjH1p.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpm/2.))/q3.m2();
Lpp=((-1.)*qsum*(MHpp) + (-2.*mjH1p.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpp/2.))/q3.m2();
U1mm=(jgbm.dot(mjH1m)*j2gm+2.*p2o*MHmm)/(p2out+pg).m2();
U1mp=(jgbp.dot(mjH1m)*j2gp+2.*p2o*MHmp)/(p2out+pg).m2();
U1pm=(jgbm.dot(mjH1p)*j2gm+2.*p2o*MHpm)/(p2out+pg).m2();
U1pp=(jgbp.dot(mjH1p)*j2gp+2.*p2o*MHpp)/(p2out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH1m)*jgbm+2.*p2i*MHmm)/(p2in-pg).m2();
U2mp=((-1.)*j2gp.dot(mjH1m)*jgbp+2.*p2i*MHmp)/(p2in-pg).m2();
U2pm=((-1.)*j2gm.dot(mjH1p)*jgbm+2.*p2i*MHpm)/(p2in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH1p)*jgbp+2.*p2i*MHpp)/(p2in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q1.m2()*qH1.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH2.m2()*q2.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4.*4./(9.*9.); // Factor of (Cf/Ca) for each quark to match MH2qQ.
//Higgs coupling is included in Hjets.C
return ampsq;
}
double jM2unobgHQg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
// std::cout << "####################\n";
// std::cout << "# p1in : "<<p1in<< " "<<p1in.plus()<<" "<<p1in.minus()<<std::endl;
// std::cout << "# p2in : "<<p2in<< " "<<p2in.plus()<<" "<<p2in.minus()<<std::endl;
// std::cout << "# p1out : "<<p1out<< " "<<p1out.rapidity()<<std::endl;
// std::cout << "# (qH1-qH2) : "<<(qH1-qH2)<< " "<<(qH1-qH2).rapidity()<<std::endl;
// std::cout << "# pg : "<<pg<< " "<<pg.rapidity()<<std::endl;
// std::cout << "# p2out : "<<p2out<< " "<<p2out.rapidity()<<std::endl;
// std::cout << "####################\n";
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out-pg); // Extra bit pre-gluon
CLHEP::HepLorentzVector q3=-(p2in-p2out); // Bottom End
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mjH1m,mjH1p,mj2m,mj2p;
mjH1p=jHtop(p1out,true,p1in,true,qH1,qH2,mt, incBot, mb);
mjH1m=jHtop(p1out,false,p1in,false,qH1,qH2,mt, incBot, mb);
mj2p=joi(p2out,true,p2in,true);
mj2m=joi(p2out,false,p2in,false);
// Dot products of these which occur again and again
COM MHmp=mjH1m.dot(mj2p); // And now for the Higgs ones
COM MHmm=mjH1m.dot(mj2m);
COM MHpp=mjH1p.dot(mj2p);
COM MHpm=mjH1p.dot(mj2m);
// Currents with pg
CCurrent jgbm,jgbp,j2gm,j2gp;
j2gp=joo(p2out,true,pg,true);
j2gm=joo(p2out,false,pg,false);
jgbp=joi(pg,true,p2in,true);
jgbm=joi(pg,false,p2in,false);
CCurrent qsum(q2+q3);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p1o(p1out),p1i(p1in);
CCurrent p2o(p2out);
CCurrent p2i(p2in);
CCurrent pplus((p1in+p1out)/2.);
CCurrent pminus((p2in+p2out)/2.);
// COM test=pminus.dot(p1in);
Lmm=((-1.)*qsum*(MHmm) + (-2.*mjH1m.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmm/2.))/q3.m2();
Lmp=((-1.)*qsum*(MHmp) + (-2.*mjH1m.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmp/2.))/q3.m2();
Lpm=((-1.)*qsum*(MHpm) + (-2.*mjH1p.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpm/2.))/q3.m2();
Lpp=((-1.)*qsum*(MHpp) + (-2.*mjH1p.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpp/2.))/q3.m2();
U1mm=(jgbm.dot(mjH1m)*j2gm+2.*p2o*MHmm)/(p2out+pg).m2();
U1mp=(jgbp.dot(mjH1m)*j2gp+2.*p2o*MHmp)/(p2out+pg).m2();
U1pm=(jgbm.dot(mjH1p)*j2gm+2.*p2o*MHpm)/(p2out+pg).m2();
U1pp=(jgbp.dot(mjH1p)*j2gp+2.*p2o*MHpp)/(p2out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH1m)*jgbm+2.*p2i*MHmm)/(p2in-pg).m2();
U2mp=((-1.)*j2gp.dot(mjH1m)*jgbp+2.*p2i*MHmp)/(p2in-pg).m2();
U2pm=((-1.)*j2gm.dot(mjH1p)*jgbm+2.*p2i*MHpm)/(p2in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH1p)*jgbp+2.*p2i*MHpp)/(p2in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q1.m2()*qH1.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH2.m2()*q2.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4./9.*4./9.; // Factor of (Cf/Ca) for each quark to match MH2qQ.
// need twice to match the normalization
//Higgs coupling is included in Hjets.C
const double K = K_g(p1out, p1in);
return ampsq*K/C_F;
}
double jM2unobgHQbarg (CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector pg, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector qH1, CLHEP::HepLorentzVector qH2, double mt, bool incBot, double mb)
{
CLHEP::HepLorentzVector q1=p1in-p1out; // Top End
CLHEP::HepLorentzVector q2=-(p2in-p2out-pg); // Extra bit pre-gluon
CLHEP::HepLorentzVector q3=-(p2in-p2out); // Bottom End
// std::cerr<<"Current: "<<q1.m2()<<" "<<q2.m2()<<std::endl;
CCurrent mjH1m,mjH1p,mj2m,mj2p;
mjH1p=jHtop(p1out,true,p1in,true,qH1,qH2,mt, incBot, mb);
mjH1m=jHtop(p1out,false,p1in,false,qH1,qH2,mt, incBot, mb);
mj2p=jio(p2in,true,p2out,true);
mj2m=jio(p2in,false,p2out,false);
// Dot products of these which occur again and again
COM MHmp=mjH1m.dot(mj2p); // And now for the Higgs ones
COM MHmm=mjH1m.dot(mj2m);
COM MHpp=mjH1p.dot(mj2p);
COM MHpm=mjH1p.dot(mj2m);
// Currents with pg
CCurrent jgbm,jgbp,j2gm,j2gp;
j2gp=joo(pg,true,p2out,true);
j2gm=joo(pg,false,p2out,false);
jgbp=jio(p2in,true,pg,true);
jgbm=jio(p2in,false,pg,false);
CCurrent qsum(q2+q3);
CCurrent Lmp,Lmm,Lpp,Lpm,U1mp,U1mm,U1pp,U1pm,U2mp,U2mm,U2pp,U2pm,p1o(p1out),p1i(p1in);
CCurrent p2o(p2out);
CCurrent p2i(p2in);
CCurrent pplus((p1in+p1out)/2.);
CCurrent pminus((p2in+p2out)/2.);
// COM test=pminus.dot(p1in);
Lmm=((-1.)*qsum*(MHmm) + (-2.*mjH1m.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmm/2.))/q3.m2();
Lmp=((-1.)*qsum*(MHmp) + (-2.*mjH1m.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1m+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHmp/2.))/q3.m2();
Lpm=((-1.)*qsum*(MHpm) + (-2.*mjH1p.dot(pg))*mj2m+2.*mj2m.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpm/2.))/q3.m2();
Lpp=((-1.)*qsum*(MHpp) + (-2.*mjH1p.dot(pg))*mj2p+2.*mj2p.dot(pg)*mjH1p+(p1o/pg.dot(p1out) + p1i/pg.dot(p1in))*(q2.m2()*MHpp/2.))/q3.m2();
U1mm=(jgbm.dot(mjH1m)*j2gm+2.*p2o*MHmm)/(p2out+pg).m2();
U1mp=(jgbp.dot(mjH1m)*j2gp+2.*p2o*MHmp)/(p2out+pg).m2();
U1pm=(jgbm.dot(mjH1p)*j2gm+2.*p2o*MHpm)/(p2out+pg).m2();
U1pp=(jgbp.dot(mjH1p)*j2gp+2.*p2o*MHpp)/(p2out+pg).m2();
U2mm=((-1.)*j2gm.dot(mjH1m)*jgbm+2.*p2i*MHmm)/(p2in-pg).m2();
U2mp=((-1.)*j2gp.dot(mjH1m)*jgbp+2.*p2i*MHmp)/(p2in-pg).m2();
U2pm=((-1.)*j2gm.dot(mjH1p)*jgbm+2.*p2i*MHpm)/(p2in-pg).m2();
U2pp=((-1.)*j2gp.dot(mjH1p)*jgbp+2.*p2i*MHpp)/(p2in-pg).m2();
const double cf=HEJ::C_F;
double amm,amp,apm,app;
amm=cf*(2.*vre(Lmm-U1mm,Lmm+U2mm))+2.*cf*cf/3.*vabs2(U1mm+U2mm);
amp=cf*(2.*vre(Lmp-U1mp,Lmp+U2mp))+2.*cf*cf/3.*vabs2(U1mp+U2mp);
apm=cf*(2.*vre(Lpm-U1pm,Lpm+U2pm))+2.*cf*cf/3.*vabs2(U1pm+U2pm);
app=cf*(2.*vre(Lpp-U1pp,Lpp+U2pp))+2.*cf*cf/3.*vabs2(U1pp+U2pp);
double ampsq=-(amm+amp+apm+app)/(q1.m2()*qH1.m2());
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) > 1.0000001)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// if ((vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm))/(2*vre(Lmm-U1mm,Lmm+U2mm)) < 0.9999999)
// std::cout << " Big Problem!! " << vabs2(Lmm-U1mm+U2mm)+vabs2(Lmm)-vabs2(U1mm)-vabs2(U2mm) << " " << 2*vre(Lmm-U1mm,Lmm+U2mm) << std::endl;
// Now add the t-channels for the Higgs
double th=qH2.m2()*q2.m2();
ampsq/=th;
ampsq/=16.;
ampsq*=4./9.*4./9.; // Factor of (Cf/Ca) for each quark to match MH2qQ.
//Higgs coupling is included in Hjets.C
const double K = K_g(p1out, p1in);
return ampsq*K/C_F; //ca/cf = 9/4
}
// Begin finite mass stuff
#ifdef HEJ_BUILD_WITH_QCDLOOP
namespace {
// All the stuff needed for the box functions in qg->qgH now...
//COM E1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM E1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2=-(k1+k2+kh);
double Delta, Sigma, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
Sigma = 4.*s12*s34 - pow(S1+S2,2);
return looprwfactor*(-s12*D0DD(k2, k1, q2, mq)*(1 - 8.*mq*mq/s12 + S2/(2.*s12) +
S2*(s12 - 8.*mq*mq)*(s34 + S1)/(2.*s12*Delta) +
2.*(s34 + S1)*(s34 + S1)/Delta +
S2*pow((s34 + S1),3)/Delta/Delta) - ((s12 + S2)*C0DD(k2,
k1 + q2, mq) -
s12*C0DD(k1, k2, mq) + (S1 - S2)*C0DD(k1 + k2, q2, mq) -
S1*C0DD(k1, q2,
mq))*(S2*(s12 - 4.*mq*mq)/(2.*s12*Delta) +
2.*(s34 + S1)/Delta +
S2*pow((s34 + S1),2)/Delta/Delta) + (C0DD(k1, q2, mq) -
C0DD(k1 + k2, q2, mq))*(1. - 4.*mq*mq/s12) -
C0DD(k1 + k2, q2, mq)*2.*s34/
S1 - (B0DD(k1 + q2, mq) -
B0DD(k1 + k2 + q2, mq))*2.*s34*(s34 +
S1)/(S1*Delta) + (B0DD(q2, mq) -
B0DD(k1 + k2 + q2, mq) +
s12*C0DD(k1 + k2, q2,
mq))*(2.*s34*(s34 +
S1)*(S1 - S2)/(Delta*Sigma) +
2.*s34*(s34 + S1)/(S1*Delta)) + (B0DD(k1 + k2, mq) -
B0DD(k1 + k2 + q2,
mq) - (s34 + S1 + S2)*C0DD(k1 + k2, q2, mq))*2.*(s34 +
S1)*(2.*s12*s34 -
S2*(S1 + S2))/(Delta*Sigma));
}
//COM F1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM F1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, Sigma, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
Sigma = 4.*s12*s34 - pow(S1+S2,2);
return looprwfactor*(-S2*D0DD(k1, k2, q2,
mq)*(0.5 - (s12 - 8.*mq*mq)*(s34 + S2)/(2.*Delta) -
s12*pow((s34 + S2),3)/Delta/Delta) + ((s12 + S1)*C0DD(k1,
k2 + q2, mq) -
s12*C0DD(k1, k2, mq) - (S1 - S2)*C0DD(k1 + k2, q2, mq) -
S2*C0DD(k2, q2,
mq))*(S2*(s12 - 4.*mq*mq)/(2.*s12*Delta) +
S2*pow((s34 + S2),2)/Delta/Delta) - (C0DD(k1 + k2, q2, mq) - C0DD(k1, k2 + q2, mq))*(1. - 4.*mq*mq/s12) -
C0DD(k1, k2 + q2, mq) + (B0DD(k2 + q2, mq) -
B0DD(k1 + k2 + q2,
mq))*2.*pow((s34 + S2),2)/((s12 + S1)*Delta) - (B0DD(
q2, mq) - B0DD(k1 + k2 + q2, mq) +
s12*C0DD(k1 + k2, q2, mq))*2.*s34*(s34 +
S2)*(S2 - S1)/(Delta*Sigma) + (B0DD(
k1 + k2, mq) -
B0DD(k1 + k2 + q2,
mq) - (s34 + S1 + S2)*C0DD(k1 + k2, q2, mq))*2.*(s34 +
S2)*(2.*s12*s34 -
S2*(S1 + S2))/(Delta*Sigma));
}
//COM G1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM G1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
return looprwfactor*(S2*D0DD(k1, q2, k2,
mq)*(Delta/s12/s12 - 4.*mq*mq/s12) -
S2*((s12 + S1)*C0DD(k1, k2 + q2, mq) -
S1*C0DD(k1, q2, mq))*(1./
s12/s12 - (s12 - 4.*mq*mq)/(2.*s12*Delta)) -
S2*((s12 + S2)*C0DD(k1 + q2, k2, mq) -
S2*C0DD(k2, q2, mq))*(1./
s12/s12 + (s12 - 4.*mq*mq)/(2.*s12*Delta)) -
C0DD(k1, q2, mq) - (C0DD(k1, k2 + q2, mq) -
C0DD(k1, q2, mq))*4.*mq*mq/
s12 + (B0DD(k1 + q2, mq) - B0DD(k1 + k2 + q2, mq))*2./
s12 + (B0DD(k1 + q2, mq) -
B0DD(q2, mq))*2.*s34/(s12*S1) + (B0DD(k2 + q2, mq) -
B0DD(k1 + k2 + q2, mq))*2.*(s34 + S2)/(s12*(s12 + S1)));
}
//COM E4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM E4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, Sigma, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
Sigma = 4.*s12*s34 - pow(S1+S2,2);
return looprwfactor* (-s12*D0DD(k2, k1, q2,
mq)*(0.5 - (S1 - 8.*mq*mq)*(s34 + S1)/(2.*Delta) -
s12*pow((s34 + S1),3)/Delta/Delta) + ((s12 + S2)*C0DD(k2,
k1 + q2, mq) -
s12*C0DD(k1, k2, mq) + (S1 - S2)*C0DD(k1 + k2, q2, mq) -
S1*C0DD(k1, q2, mq))*((S1 - 4.*mq*mq)/(2.*Delta) +
s12*pow((s34 + S1),2)/Delta/Delta) -
C0DD(k1 + k2, q2, mq) + (B0DD(k1 + q2, mq) -
B0DD(k1 + k2 + q2, mq))*(2.*s34/Delta +
2.*s12*(s34 + S1)/((s12 + S2)*Delta)) - (B0DD(
q2, mq) - B0DD(k1 + k2 + q2, mq) +
s12*C0DD(k1 + k2, q2,
mq))*((2.*s34*(2.*s12*s34 - S2*(S1 + S2) +
s12*(S1 -
S2)))/(Delta*Sigma)) + (B0DD(k1 + k2, mq) -
B0DD(k1 + k2 + q2, mq) - (s34 + S1 + S2)*C0DD(k1 + k2, q2, mq))*((2.*s12*(2.*s12*s34 - S1*(S1 + S2) +
s34*(S2 - S1)))/(Delta*Sigma)));
}
//COM F4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM F4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, Sigma, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
Sigma = 4.*s12*s34 - pow(S1+S2,2);
return looprwfactor* (-s12*D0DD(k1, k2, q2,
mq)*(0.5 + (S1 - 8.*mq*mq)*(s34 + S2)/(2.*Delta) +
s12*pow((s34 + S2),3)/Delta/Delta) - ((s12 + S1)*C0DD(k1,
k2 + q2, mq) -
s12*C0DD(k1, k2, mq) - (S1 - S2)*C0DD(k1 + k2, q2, mq) -
S2*C0DD(k2, q2, mq))*((S1 - 4.*mq*mq)/(2.*Delta) +
s12*pow((s34 + S2),2)/Delta/Delta) -
C0DD(k1 + k2, q2, mq) - (B0DD(k2 + q2, mq) -
B0DD(k1 + k2 + q2, mq))*2.*(s34 +
S2)/Delta + (B0DD(q2, mq) -
B0DD(k1 + k2 + q2, mq) +
s12*C0DD(k1 + k2, q2, mq))*2.*s34*(2.*s12*s34 -
S1*(S1 + S2) +
s12*(S2 - S1))/(Delta*Sigma) - (B0DD(k1 + k2, mq) -
B0DD(k1 + k2 + q2, mq) - (s34 + S1 + S2)*C0DD(k1 + k2, q2, mq))*(2.*s12*(2.*s12*s34 - S2*(S1 + S2) +
s34*(S1 - S2))/(Delta*Sigma)));
}
//COM G4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM G4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
return looprwfactor* (-D0DD(k1, q2, k2,
mq)*(Delta/s12 + (s12 + S1)/2. -
4.*mq*mq) + ((s12 + S1)*C0DD(k1, k2 + q2, mq) -
S1*C0DD(k1, q2, mq))*(1./
s12 - (S1 - 4.*mq*mq)/(2.*Delta)) + ((s12 + S2)*C0DD(
k1 + q2, k2, mq) -
S2*C0DD(k2, q2, mq))*(1./
s12 + (S1 - 4.*mq*mq)/(2.*Delta)) + (B0DD(
k1 + k2 + q2, mq) -
B0DD(k1 + q2, mq))*2./(s12 + S2));
}
//COM E10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM E10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, Sigma, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
Sigma = 4.*s12*s34 - pow(S1+S2,2);
return looprwfactor*(-s12*D0DD(k2, k1, q2, mq)*((s34 + S1)/Delta +
12.*mq*mq*S1*(s34 + S1)/Delta/Delta -
4.*s12*S1*pow((s34 + S1),3)/Delta/Delta/Delta) - ((s12 + S2)*C0DD(k2, k1 + q2, mq) -
s12*C0DD(k1, k2, mq) + (S1 - S2)*C0DD(k1 + k2, q2, mq) -
S1*C0DD(k1, q2, mq))*(1./Delta +
4.*mq*mq*S1/Delta/Delta -
4.*s12*S1*pow((s34 + S1),2)/Delta/Delta/Delta) +
C0DD(k1 + k2, q2, mq)*(4.*s12*s34*(S1 - S2)/(Delta*Sigma) -
4.*(s12 -
2.*mq*mq)*(2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma)) + (B0DD(k1 + q2, mq) -
B0DD(k1 + k2 + q2, mq))*(4.*(s34 + S1)/((s12 + S2)*Delta) +
8.*S1*(s34 + S1)/Delta/Delta) + (B0DD(q2, mq) -
B0DD(k1 + k2 + q2, mq) +
s12*C0DD(k1 + k2, q2, mq))*(12.*s34*(2.*s12 + S1 +
S2)*(2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma*Sigma) -
4.*s34*(4.*s12 + 3.*S1 +
S2)/(Delta*Sigma) +
8.*s12*s34*(s34*(s12 + S2) -
S1*(s34 +
S1))/(Delta*Delta*Sigma)) + (B0DD(k1 + k2, mq) -
B0DD(k1 + k2 + q2, mq) - (s34 + S1 + S2)*C0DD(k1 + k2, q2,
mq))*(12.*s12*(2.*s34 + S1 +
S2)*(2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma*Sigma) +
8.*s12*S1*(s34*(s12 + S2) -
S1*(s34 +
S1))/(Delta*Delta*Sigma))) + (COM(0.,1.)/(4.*M_PI*M_PI))*((2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma));
}
//COM F10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM F10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, Sigma, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
Sigma = 4.*s12*s34 - pow(S1+S2,2);
return looprwfactor* (s12*D0DD(k1, k2, q2,
mq)*((s34 + S2)/Delta - 4.*mq*mq/Delta +
12.*mq*mq*s34*(s12 + S1)/Delta/Delta -
4.*s12*pow((s34 + S2),2)/Delta/Delta -
4.*s12*S1*pow((s34 + S2),3)/Delta/Delta/Delta) + ((s12 + S1)*C0DD(k1, k2 + q2, mq) -
s12*C0DD(k1, k2, mq) - (S1 - S2)*C0DD(k1 + k2, q2, mq) -
S2*C0DD(k2, q2, mq))*(1./Delta +
4.*mq*mq*S1/Delta/Delta -
4.*s12*(s34 + S2)/Delta/Delta -
4.*s12*S1*pow((s34 + S2),2)/Delta/Delta/Delta) -
C0DD(k1 + k2, q2, mq)*(4.*s12*s34/(S2*Delta) +
4.*s12*s34*(S2 - S1)/(Delta*Sigma) +
4.*(s12 -
2.*mq*mq)*(2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma)) - (B0DD(
k2 + q2, mq) -
B0DD(k1 + k2 + q2, mq))*(4.*s34/(S2*Delta) +
8.*s34*(s12 + S1)/Delta/Delta) - (B0DD(q2, mq) -
B0DD(k1 + k2 + q2, mq) +
s12*C0DD(k1 + k2, q2,
mq))*(-12*s34*(2*s12 + S1 +
S2)*(2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma*Sigma) -
4.*s12*s34*s34/(S2*Delta*Delta) +
4.*s34*S1/(Delta*Sigma) -
4.*s34*(s12*s34*(2.*s12 + S2) -
S1*S1*(2.*s12 +
S1))/(Delta*Delta*Sigma)) - (B0DD(k1 + k2, mq) -
B0DD(k1 + k2 + q2, mq) - (s34 + S1 + S2)*C0DD(k1 + k2, q2, mq))*(-12.*s12*(2.*s34 + S1 +
S2)*(2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma*Sigma) +
8.*s12*(2.*s34 + S1)/(Delta*Sigma) -
8.*s12*s34*(2.*s12*s34 - S1*(S1 + S2) +
s12*(S2 -
S1))/(Delta*Delta*Sigma))) + (COM(0.,1.)/(4.*M_PI*M_PI))*((2.*s12*s34 -
S1*(S1 + S2))/(Delta*Sigma));
}
//COM G10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM G10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//CLHEP::HepLorentzVector q2=k3+k4;
CLHEP::HepLorentzVector q2 = -(k1+k2+kh);
double Delta, S1, S2, s12, s34;
S1 = 2.*k1.dot(q2);
S2 = 2.*k2.dot(q2);
s12 = 2.*k1.dot(k2);
//s34 = 2.*k3.dot(k4);
s34 = q2.m2();
Delta = s12*s34 - S1*S2;
return looprwfactor* (-D0DD(k1, q2, k2, mq)*(1. +
4.*S1*mq*mq/Delta) + ((s12 + S1)*C0DD(k1,
k2 + q2, mq) -
S1*C0DD(k1, q2, mq))*(1./Delta +
4.*S1*mq*mq/Delta/Delta) - ((s12 + S2)*C0DD(k1 + q2,
k2, mq) - S2*C0DD(k2, q2, mq))*(1./Delta +
4.*S1*mq*mq/Delta/Delta) + (B0DD(k1 + k2 + q2, mq) -
B0DD(k1 + q2, mq))*4.*(s34 +
S1)/(Delta*(s12 + S2)) + (B0DD(q2, mq) -
B0DD(k2 + q2, mq))*4.*s34/(Delta*S2));
}
//COM H1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM H1(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//return E1(k1,k2,k3,k4,mq)+F1(k1,k2,k3,k4,mq)+G1(k1,k2,k3,k4,mq);
return E1(k1,k2,kh,mq)+F1(k1,k2,kh,mq)+G1(k1,k2,kh,mq);
}
//COM H4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM H4(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//return E4(k1,k2,k3,k4,mq)+F4(k1,k2,k3,k4,mq)+G4(k1,k2,k3,k4,mq);
return E4(k1,k2,kh,mq)+F4(k1,k2,kh,mq)+G4(k1,k2,kh,mq);
}
//COM H10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM H10(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//return E10(k1,k2,k3,k4,mq)+F10(k1,k2,k3,k4,mq)+G10(k1,k2,k3,k4,mq);
return E10(k1,k2,kh,mq)+F10(k1,k2,kh,mq)+G10(k1,k2,kh,mq);
}
//COM H2(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM H2(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//return -1.*H1(k2,k1,k3,k4,mq);
return -1.*H1(k2,k1,kh,mq);
}
//COM H5(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM H5(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//return -1.*H4(k2,k1,k3,k4,mq);
return -1.*H4(k2,k1,kh,mq);
}
//COM H12(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector k3, CLHEP::HepLorentzVector k4, double mq)
COM H12(CLHEP::HepLorentzVector k1, CLHEP::HepLorentzVector k2, CLHEP::HepLorentzVector kh, double mq)
{
//return -1.*H10(k2,k1,k3,k4,mq);
return -1.*H10(k2,k1,kh,mq);
}
// FL and FT functions
COM FL(CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mq)
{
CLHEP::HepLorentzVector Q = q1 + q2;
double detQ2 = q1.m2()*q2.m2() - q1.dot(q2)*q1.dot(q2);
return -1./(2.*detQ2)*((2.-
3.*q1.m2()*q2.dot(Q)/detQ2)*(B0DD(q1, mq) -
B0DD(Q, mq)) + (2. -
3.*q2.m2()*q1.dot(Q)/detQ2)*(B0DD(q2, mq) -
B0DD(Q, mq)) - (4.*mq*mq + q1.m2() + q2.m2() +
Q.m2() - 3.*q1.m2()*q2.m2()*Q.m2()/detQ2)*C0DD(
q1, q2, mq) - 2.);
}
COM FT(CLHEP::HepLorentzVector q1, CLHEP::HepLorentzVector q2, double mq)
{
CLHEP::HepLorentzVector Q = q1 + q2;
double detQ2 = q1.m2()*q2.m2() - q1.dot(q2)*q1.dot(q2);
return -1./(2.*detQ2)*(Q.m2()*(B0DD(q1, mq) + B0DD(q2, mq) - 2.*B0DD(Q, mq) -
2.*q1.dot(q2)*C0DD(q1, q2, mq)) + (q1.m2() -
q2.m2()) *(B0DD(q1, mq) - B0DD(q2, mq))) -
q1.dot(q2)*FL(q1, q2, mq);
}
CLHEP::HepLorentzVector ParityFlip(CLHEP::HepLorentzVector p)
{
CLHEP::HepLorentzVector flippedVector;
flippedVector.setE(p.e());
flippedVector.setX(-p.x());
flippedVector.setY(-p.y());
flippedVector.setZ(-p.z());
return flippedVector;
}
/// @brief HC amp for qg->qgH with finite top (i.e. j^{++}_H)
void g_gH_HC(CLHEP::HepLorentzVector pa, CLHEP::HepLorentzVector p1,
CLHEP::HepLorentzVector pH, double mq, current &retAns)
{
current cura1,pacur,p1cur,pHcur,conjeps1,conjepsH1,epsa,epsHa,epsHapart1,
epsHapart2,conjepsH1part1,conjepsH1part2;
COM ang1a,sqa1;
const double F = 4.*mq*mq/HEJ::vev;
// Easier to have the whole thing as current object so I can use cdot functionality.
// Means I need to write pa,p1 as current objects
to_current(pa, pacur);
to_current(p1,p1cur);
to_current(pH,pHcur);
bool gluonforward = true;
if(pa.z() < 0)
gluonforward = false;
//HEJ gauge
jio(pa,false,p1,false,cura1);
if(gluonforward){
// sqrt(2pa_-/p1_-)*p1_perp/abs(p1_perp)
ang1a = sqrt(pa.plus()*p1.minus())*(p1.x()+COM(0.,1.)*p1.y())/p1.perp();
// sqrt(2pa_-/p1_-)*p1_perp*/abs(p1_perp)
sqa1 = sqrt(pa.plus()*p1.minus())*(p1.x()-COM(0.,1.)*p1.y())/p1.perp();
} else {
ang1a = sqrt(pa.minus()*p1.plus());
sqa1 = sqrt(pa.minus()*p1.plus());
}
const double prop = (pa-p1-pH).m2();
cmult(-1./sqrt(2)/ang1a,cura1,conjeps1);
cmult(1./sqrt(2)/sqa1,cura1,epsa);
const COM Fta = FT(-pa,pa-pH,mq)/(pa-pH).m2();
const COM Ft1 = FT(-p1-pH,p1,mq)/(p1+pH).m2();
const COM h4 = H4(p1,-pa,pH,mq);
const COM h5 = H5(p1,-pa,pH,mq);
const COM h10 = H10(p1,-pa,pH,mq);
const COM h12 = H12(p1,-pa,pH,mq);
cmult(Fta*pa.dot(pH), epsa, epsHapart1);
cmult(-1.*Fta*cdot(pHcur,epsa), pacur, epsHapart2);
cmult(Ft1*cdot(pHcur,conjeps1), p1cur, conjepsH1part1);
cmult(-Ft1*p1.dot(pH), conjeps1, conjepsH1part2);
cadd(epsHapart1, epsHapart2, epsHa);
cadd(conjepsH1part1, conjepsH1part2, conjepsH1);
const COM aH1 = cdot(pHcur, cura1);
current T1,T2,T3,T4,T5,T6,T7,T8,T9,T10;
if(gluonforward){
cmult(sqrt(2.)*sqrt(p1.plus()/pa.plus())*prop/sqa1, conjepsH1, T1);
cmult(-sqrt(2.)*sqrt(pa.plus()/p1.plus())*prop/ang1a, epsHa, T2);
}
else{
cmult(-sqrt(2.)*sqrt(p1.minus()/pa.minus())
*((p1.x()-COM(0.,1.)*p1.y())/p1.perp())*prop/sqa1, conjepsH1, T1);
cmult(sqrt(2.)*sqrt(pa.minus()/p1.minus())
*((p1.x()-COM(0.,1.)*p1.y())/p1.perp())*prop/ang1a, epsHa, T2);
}
cmult(sqrt(2.)/ang1a*aH1, epsHa, T3);
cmult(sqrt(2.)/sqa1*aH1, conjepsH1, T4);
cmult(-sqrt(2.)*Fta*pa.dot(p1)*aH1/sqa1, conjeps1, T5);
cmult(-sqrt(2.)*Ft1*pa.dot(p1)*aH1/ang1a, epsa, T6);
cmult(-aH1/sqrt(2.)/sqa1*h4*8.*COM(0.,1.)*M_PI*M_PI, conjeps1, T7);
cmult(aH1/sqrt(2.)/ang1a*h5*8.*COM(0.,1.)*M_PI*M_PI, epsa, T8);
cmult(aH1*aH1/2./ang1a/sqa1*h10*8.*COM(0.,1.)*M_PI*M_PI, pacur, T9);
cmult(-aH1*aH1/2./ang1a/sqa1*h12*8.*COM(0.,1.)*M_PI*M_PI, p1cur, T10);
current ans;
for(int i=0;i<4;i++)
{
ans[i] = T1[i]+T2[i]+T3[i]+T4[i]+T5[i]+T6[i]+T7[i]+T8[i]+T9[i]+T10[i];
}
retAns[0] = F/prop*ans[0];
retAns[1] = F/prop*ans[1];
retAns[2] = F/prop*ans[2];
retAns[3] = F/prop*ans[3];
}
/// @brief HNC amp for qg->qgH with finite top (i.e. j^{+-}_H)
void g_gH_HNC(CLHEP::HepLorentzVector pa, CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector pH, double mq, current &retAns)
{
const double F = 4.*mq*mq/HEJ::vev;
COM ang1a,sqa1;
current conjepsH1,epsHa,p1cur,pacur,pHcur,conjeps1,epsa,paplusp1cur,
p1minuspacur,cur1a,cura1,epsHapart1,epsHapart2,conjepsH1part1,
conjepsH1part2;
// Find here if pa, meaning the gluon, is forward or backward
bool gluonforward = true;
if(pa.z() < 0)
gluonforward = false;
jio(pa,true,p1,true,cura1);
joi(p1,true,pa,true,cur1a);
to_current(pa,pacur);
to_current(p1,p1cur);
to_current(pH,pHcur);
to_current(pa+p1,paplusp1cur);
to_current(p1-pa,p1minuspacur);
const COM aH1 = cdot(pHcur,cura1);
const COM oneHa = std::conj(aH1); // = cdot(pHcur,cur1a)
if(gluonforward){
// sqrt(2pa_-/p1_-)*p1_perp/abs(p1_perp)
ang1a = sqrt(pa.plus()*p1.minus())*(p1.x()+COM(0.,1.)*p1.y())/p1.perp();
// sqrt(2pa_-/p1_-)*p1_perp*/abs(p1_perp)
sqa1 = sqrt(pa.plus()*p1.minus())*(p1.x()-COM(0.,1.)*p1.y())/p1.perp();
}
else {
ang1a = sqrt(pa.minus()*p1.plus());
sqa1 = sqrt(pa.minus()*p1.plus());
}
const double prop = (pa-p1-pH).m2();
cmult(1./sqrt(2)/sqa1, cur1a, epsa);
cmult(-1./sqrt(2)/sqa1, cura1, conjeps1);
const COM phase = cdot(conjeps1, epsa);
const COM Fta = FT(-pa,pa-pH,mq)/(pa-pH).m2();
const COM Ft1 = FT(-p1-pH,p1,mq)/(p1+pH).m2();
const COM Falpha = FT(p1-pa,pa-p1-pH,mq);
const COM Fbeta = FL(p1-pa,pa-p1-pH,mq);
const COM h1 = H1(p1,-pa, pH, mq);
const COM h2 = H2(p1,-pa, pH, mq);
const COM h4 = H4(p1,-pa, pH, mq);
const COM h5 = H5(p1,-pa, pH, mq);
const COM h10 = H10(p1,-pa, pH, mq);
const COM h12 = H12(p1,-pa, pH, mq);
cmult(Fta*pa.dot(pH), epsa, epsHapart1);
cmult(-1.*Fta*cdot(pHcur,epsa), pacur, epsHapart2);
cmult(Ft1*cdot(pHcur,conjeps1), p1cur, conjepsH1part1);
cmult(-Ft1*p1.dot(pH), conjeps1, conjepsH1part2);
cadd(epsHapart1, epsHapart2, epsHa);
cadd(conjepsH1part1, conjepsH1part2, conjepsH1);
current T1,T2,T3,T4,T5a,T5b,T6,T7,T8a,T8b,T9,T10,T11a,
T11b,T12a,T12b,T13;
if(gluonforward){
cmult(sqrt(2.)*sqrt(p1.plus()/pa.plus())*prop/sqa1, conjepsH1, T1);
cmult(-sqrt(2.)*sqrt(pa.plus()/p1.plus())*prop/sqa1, epsHa, T2);
}
else{
cmult(-sqrt(2.)*sqrt(p1.minus()/pa.minus())*((p1.x()-COM(0.,1.)*p1.y())/p1.perp())
*prop/sqa1, conjepsH1, T1);
cmult(sqrt(2.)*sqrt(pa.minus()/p1.minus())*((p1.x()+COM(0.,1.)*p1.y())/p1.perp())
*prop/sqa1, epsHa, T2);
}
const COM boxdiagFact = 8.*COM(0.,1.)*M_PI*M_PI;
cmult(aH1*sqrt(2.)/sqa1, epsHa, T3);
cmult(oneHa*sqrt(2.)/sqa1, conjepsH1, T4);
cmult(-2.*phase*Fta*pa.dot(pH), p1cur, T5a);
cmult(2.*phase*Ft1*p1.dot(pH), pacur, T5b);
cmult(-sqrt(2.)*Fta*p1.dot(pa)*oneHa/sqa1, conjeps1, T6);
cmult(-sqrt(2.)*Ft1*pa.dot(p1)*aH1/sqa1, epsa, T7);
cmult(-boxdiagFact*phase*h2, pacur, T8a);
cmult(boxdiagFact*phase*h1, p1cur, T8b);
cmult(boxdiagFact*aH1/sqrt(2.)/sqa1*h5, epsa, T9);
cmult(-boxdiagFact*oneHa/sqrt(2.)/sqa1*h4, conjeps1, T10);
cmult(boxdiagFact*aH1*oneHa/2./sqa1/sqa1*h10, pacur, T11a);
cmult(-boxdiagFact*aH1*oneHa/2./sqa1/sqa1*h12, p1cur, T11b);
cmult(-phase/(pa-p1).m2()*Falpha*(p1-pa).dot(pa-p1-pH), paplusp1cur, T12a);
cmult(phase/(pa-p1).m2()*Falpha*(pa+p1).dot(pa-p1-pH), p1minuspacur, T12b);
cmult(-phase*Fbeta*(pa-p1-pH).m2(), paplusp1cur, T13);
current ans;
for(int i=0;i<4;i++)
{
ans[i] = T1[i]+T2[i]+T3[i]+T4[i]+T5a[i]+T5b[i]+T6[i]+T7[i]+T8a[i]+T8b[i]+T9[i]+T10[i]+T11a[i]+T11b[i]+T12a[i]+T12b[i]+T13[i];
}
retAns[0] = F/prop*ans[0];
retAns[1] = F/prop*ans[1];
retAns[2] = F/prop*ans[2];
retAns[3] = F/prop*ans[3];
}
} // namespace anonymous
// JDC - new amplitude with Higgs emitted close to gluon with full mt effects. Keep usual HEJ-style function call
double MH2gq_outsideH(CLHEP::HepLorentzVector p1out, CLHEP::HepLorentzVector p1in, CLHEP::HepLorentzVector p2out, CLHEP::HepLorentzVector p2in, CLHEP::HepLorentzVector pH, double mq, bool includeBottom, double mq2)
{
current cur2bplus,cur2bminus, cur2bplusFlip, cur2bminusFlip;
current retAns,retAnsb;
joi(p2out,true,p2in,true,cur2bplus);
joi(p2out,false,p2in,false,cur2bminus);
joi(ParityFlip(p2out),true,ParityFlip(p2in),true,cur2bplusFlip);
joi(ParityFlip(p2out),false,ParityFlip(p2in),false,cur2bminusFlip);
COM app1,app2,apm1,apm2;
COM app3, app4, apm3, apm4;
if(!includeBottom)
{
g_gH_HC(p1in,p1out,pH,mq,retAns);
app1=cdot(retAns,cur2bplus);
app2=cdot(retAns,cur2bminus);
g_gH_HC(ParityFlip(p1in),ParityFlip(p1out),ParityFlip(pH),mq,retAns);
app3=cdot(retAns,cur2bplusFlip);
app4=cdot(retAns,cur2bminusFlip);
// And non-conserving bits
g_gH_HNC(p1in,p1out,pH,mq,retAns);
apm1=cdot(retAns,cur2bplus);
apm2=cdot(retAns,cur2bminus);
g_gH_HNC(ParityFlip(p1in),ParityFlip(p1out),ParityFlip(pH),mq,retAns);
apm3=cdot(retAns,cur2bplusFlip);
apm4=cdot(retAns,cur2bminusFlip);
} else {
g_gH_HC(p1in,p1out,pH,mq,retAns);
g_gH_HC(p1in,p1out,pH,mq2,retAnsb);
app1=cdot(retAns,cur2bplus) + cdot(retAnsb,cur2bplus);
app2=cdot(retAns,cur2bminus) + cdot(retAnsb,cur2bminus);
g_gH_HC(ParityFlip(p1in),ParityFlip(p1out),ParityFlip(pH),mq,retAns);
g_gH_HC(ParityFlip(p1in),ParityFlip(p1out),ParityFlip(pH),mq2,retAnsb);
app3=cdot(retAns,cur2bplusFlip) + cdot(retAnsb,cur2bplusFlip);
app4=cdot(retAns,cur2bminusFlip) + cdot(retAnsb,cur2bminusFlip);
// And non-conserving bits
g_gH_HNC(p1in,p1out,pH,mq,retAns);
g_gH_HNC(p1in,p1out,pH,mq2,retAnsb);
apm1=cdot(retAns,cur2bplus) + cdot(retAnsb,cur2bplus);
apm2=cdot(retAns,cur2bminus) + cdot(retAnsb,cur2bminus);
g_gH_HNC(ParityFlip(p1in),ParityFlip(p1out),ParityFlip(pH),mq,retAns);
g_gH_HNC(ParityFlip(p1in),ParityFlip(p1out),ParityFlip(pH),mq2,retAnsb);
apm3=cdot(retAns,cur2bplusFlip) + cdot(retAnsb,cur2bplusFlip);
apm4=cdot(retAns,cur2bminusFlip) + cdot(retAnsb,cur2bminusFlip);
}
return abs2(app1) + abs2(app2) + abs2(app3) + abs2(app4) + abs2(apm1)
+ abs2(apm2) + abs2(apm3) + abs2(apm4);
}
#endif // HEJ_BUILD_WITH_QCDLOOP
double C2gHgm(CLHEP::HepLorentzVector p2, CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector pH)
{
static double A=1./(3.*M_PI*HEJ::vev);
// Implements Eq. (4.22) in hep-ph/0301013 with modifications to incoming plus momenta
double s12,p1p,p2p;
COM p1perp,p3perp,phperp;
// Determine first whether this is the case p1p\sim php>>p3p og the opposite
s12=p1.invariantMass2(-p2);
if (p2.pz()>0.) { // case considered in hep-ph/0301013
p1p=p1.plus();
p2p=p2.plus();
} else { // opposite case
p1p=p1.minus();
p2p=p2.minus();
}
p1perp=p1.px()+COM(0,1)*p1.py();
phperp=pH.px()+COM(0,1)*pH.py();
p3perp=-(p1perp+phperp);
COM temp=COM(0,1)*A/(2.*s12)*(p2p/p1p*conj(p1perp)*p3perp+p1p/p2p*p1perp*conj(p3perp));
temp=temp*conj(temp);
return temp.real();
}
double C2gHgp(CLHEP::HepLorentzVector p2, CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector pH)
{
static double A=1./(3.*M_PI*HEJ::vev);
// Implements Eq. (4.23) in hep-ph/0301013
double s12,php,p1p,phm;
COM p1perp,p3perp,phperp;
// Determine first whether this is the case p1p\sim php>>p3p or the opposite
s12=p1.invariantMass2(-p2);
if (p2.pz()>0.) { // case considered in hep-ph/0301013
php=pH.plus();
phm=pH.minus();
p1p=p1.plus();
} else { // opposite case
php=pH.minus();
phm=pH.plus();
p1p=p1.minus();
}
p1perp=p1.px()+COM(0,1)*p1.py();
phperp=pH.px()+COM(0,1)*pH.py();
p3perp=-(p1perp+phperp);
COM temp=-COM(0,1)*A/(2.*s12)*( conj(p1perp*p3perp)*pow(php/p1p,2)/(1.+php/p1p)
+s12*(pow(conj(phperp),2)/(pow(abs(phperp),2)+p1p*phm)
-pow(conj(p3perp)
+(1.+php/p1p)*conj(p1perp),2)/((1.+php/p1p)*(pH.m2()+2.*p1.dot(pH)))) );
temp=temp*conj(temp);
return temp.real();
}
double C2qHqm(CLHEP::HepLorentzVector p2, CLHEP::HepLorentzVector p1, CLHEP::HepLorentzVector pH)
{
static double A=1./(3.*M_PI*HEJ::vev);
// Implements Eq. (4.22) in hep-ph/0301013
double s12,p2p,p1p;
COM p1perp,p3perp,phperp;
// Determine first whether this is the case p1p\sim php>>p3p or the opposite
s12=p1.invariantMass2(-p2);
if (p2.pz()>0.) { // case considered in hep-ph/0301013
p2p=p2.plus();
p1p=p1.plus();
} else { // opposite case
p2p=p2.minus();
p1p=p1.minus();
}
p1perp=p1.px()+COM(0,1)*p1.py();
phperp=pH.px()+COM(0,1)*pH.py();
p3perp=-(p1perp+phperp);
COM temp=A/(2.*s12)*( sqrt(p2p/p1p)*p3perp*conj(p1perp)
+sqrt(p1p/p2p)*p1perp*conj(p3perp) );
temp=temp*conj(temp);
return temp.real();
}
diff --git a/src/get_analysis.cc b/src/get_analysis.cc
index 64d6fe0..dfcc5d5 100644
--- a/src/get_analysis.cc
+++ b/src/get_analysis.cc
@@ -1,32 +1,38 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/get_analysis.hh"
#include <dlfcn.h>
+#include <string>
#include "yaml-cpp/yaml.h"
-#include "HEJ/RivetAnalysis.hh"
#include "HEJ/EmptyAnalysis.hh"
+#include "HEJ/RivetAnalysis.hh"
namespace HEJ{
std::unique_ptr<Analysis> get_analysis(YAML::Node const & parameters){
if(!parameters["plugin"]){
if(parameters["rivet"])
return RivetAnalysis::create(parameters);
return EmptyAnalysis::create(parameters);
}
using AnalysisMaker = std::unique_ptr<Analysis> (*)(YAML::Node);
const auto plugin_name = parameters["plugin"].as<std::string>();
auto handle = dlopen(plugin_name.c_str(), RTLD_NOW);
char * error = dlerror();
if(error != nullptr) throw std::runtime_error(error);
void * sym = dlsym(handle, "make_analysis");
error = dlerror();
if(error != nullptr) throw std::runtime_error(error);
auto make_analysis = reinterpret_cast<AnalysisMaker>(sym);
return make_analysis(parameters);
}
}
diff --git a/src/kinematics.cc b/src/kinematics.cc
index 785a460..a878155 100644
--- a/src/kinematics.cc
+++ b/src/kinematics.cc
@@ -1,22 +1,27 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/kinematics.hh"
#include "fastjet/PseudoJet.hh"
-#include "HEJ/utility.hh"
+#include "HEJ/Particle.hh"
namespace HEJ{
//reconstruct incoming momenta from momentum conservation
std::tuple<fastjet::PseudoJet, fastjet::PseudoJet> incoming_momenta(
std::vector<Particle> const & outgoing
){
double xa(0.), xb(0.);
for(auto const & out: outgoing){
xa += out.p.e() - out.p.pz();
xb += out.p.e() + out.p.pz();
}
return std::tuple<fastjet::PseudoJet, fastjet::PseudoJet>{
{0,0,-xa/2.,xa/2.},
{0,0,xb/2.,xb/2.}
};
}
}
diff --git a/src/make_RNG.cc b/src/make_RNG.cc
index b0b8244..b1a3661 100644
--- a/src/make_RNG.cc
+++ b/src/make_RNG.cc
@@ -1,28 +1,35 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/make_RNG.hh"
+#include <algorithm>
#include <locale>
-#include "HEJ/Ranlux64.hh"
+#include "HEJ/exceptions.hh"
#include "HEJ/Mixmax.hh"
+#include "HEJ/Ranlux64.hh"
namespace HEJ {
std::unique_ptr<HEJ::RNG> make_RNG(
std::string const & name,
optional<std::string> const & seed
) {
std::string lname;
std::transform(
begin(name), end(name), std::back_inserter(lname),
[](char c) { return std::tolower(c, std::locale()); }
);
if(lname == "mixmax") {
if(seed) return std::make_unique<Mixmax>(std::stol(*seed));
return std::make_unique<Mixmax>();
}
if(lname == "ranlux64") {
if(seed) return std::make_unique<Ranlux64>(*seed);
return std::make_unique<Ranlux64>();
}
throw std::invalid_argument{"Unknown random number generator: " + name};
}
}
diff --git a/src/make_writer.cc b/src/make_writer.cc
index 1283e82..0e15d61 100644
--- a/src/make_writer.cc
+++ b/src/make_writer.cc
@@ -1,25 +1,31 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/make_writer.hh"
-#include "HEJ/LesHouchesWriter.hh"
+#include "HEJ/exceptions.hh"
#include "HEJ/HepMCWriter.hh"
+#include "HEJ/LesHouchesWriter.hh"
namespace HEJ{
std::unique_ptr<EventWriter> make_format_writer(
FileFormat format, std::string const & outfile,
LHEF::HEPRUP const & heprup
){
switch(format){
case Les_Houches:
return std::unique_ptr<EventWriter>{
new LesHouchesWriter{outfile, heprup}
};
case HepMC:
return std::unique_ptr<EventWriter>{
new HepMCWriter{outfile, heprup}
};
default:
throw std::logic_error("unhandled file format");
}
}
}
diff --git a/src/resummation_jet.cc b/src/resummation_jet.cc
index 5fd0d27..0c41dbe 100644
--- a/src/resummation_jet.cc
+++ b/src/resummation_jet.cc
@@ -1,108 +1,113 @@
-#include <stdlib.h>
-#include <stdio.h>
-#include <math.h>
-#include <vector>
-#include <array>
-#include <algorithm>
-
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/resummation_jet.hh"
-#include "HEJ/utility.hh"
-#include <boost/numeric/ublas/matrix.hpp>
+#include <assert.h>
+#include <math.h>
+#include <stdio.h>
+
#include <boost/numeric/ublas/lu.hpp>
+#include <boost/numeric/ublas/matrix.hpp>
+
+#include "fastjet/PseudoJet.hh"
+
+#include "HEJ/utility.hh"
namespace HEJ{
std::vector<fastjet::PseudoJet> resummation_jet_momenta(
std::vector<fastjet::PseudoJet> const & p_born,
fastjet::PseudoJet const & qperp
) {
// for "new" reshuffling p^B = p + qperp*|p^B|/P^B
double Pperp_born = 0.;
for(auto const & p: p_born) Pperp_born += p.perp();
std::vector<fastjet::PseudoJet> p_res;
p_res.reserve(p_born.size());
for(auto & pB: p_born) {
const double px = pB.px() - qperp.px()*pB.perp()/Pperp_born;
const double py = pB.py() - qperp.py()*pB.perp()/Pperp_born;
const double pperp = sqrt(px*px + py*py);
// keep the rapidities fixed
const double pz = pperp*sinh(pB.rapidity());
const double E = pperp*cosh(pB.rapidity());
p_res.emplace_back(px, py, pz, E);
assert(
HEJ::nearby_ep(
p_res.back().rapidity(),
pB.rapidity(),
1e-5
)
);
}
return p_res;
}
namespace{
enum coordinates : size_t {
x1, x2
};
namespace ublas = boost::numeric::ublas;
template<class Matrix>
double det(ublas::matrix_expression<Matrix> const& m) {
ublas::permutation_matrix<size_t> pivots{m().size1()};
Matrix mLu{m()};
const auto is_singular = lu_factorize(mLu, pivots);
if(is_singular) return 0.;
double det = 1.0;
for (std::size_t i = 0; i < pivots.size(); ++i){
if (pivots(i) != i) det = -det;
det *= mLu(i,i);
}
return det;
}
using ublas::matrix;
}
double resummation_jet_weight(
std::vector<fastjet::PseudoJet> const & p_born,
fastjet::PseudoJet const & qperp
) {
static constexpr int num_coordinates = 2;
auto Jacobian = matrix<double>{
num_coordinates*p_born.size(),
num_coordinates*p_born.size()
};
double P_perp = 0.;
for(auto const & J: p_born) P_perp += J.perp();
for(size_t l = 0; l < p_born.size(); ++l){
const double Jl_perp = p_born[l].perp();
for(size_t lp = 0; lp < p_born.size(); ++lp){
const int delta_l = l == lp;
const double Jlp_perp = p_born[lp].perp();
for(size_t x = x1; x <= x2; ++x){
for(size_t xp = x1; xp <= x2; ++xp){
const int delta_x = x == xp;
Jacobian(2*l + x, 2*lp + xp) =
+ delta_l*delta_x
- qperp[x]*p_born[lp][xp]/(P_perp*Jlp_perp)*(
+ delta_l - Jl_perp/P_perp
);
}
}
}
}
return det(Jacobian);
}
}
diff --git a/src/stream.cc b/src/stream.cc
index a0b2fff..d856096 100644
--- a/src/stream.cc
+++ b/src/stream.cc
@@ -1,27 +1,32 @@
+/**
+ * \authors Jeppe Andersen, Tuomas Hapola, Marian Heil, Andreas Maier, Jennifer Smillie
+ * \date 2019
+ * \copyright GPLv2 or later
+ */
#include "HEJ/stream.hh"
#include <boost/iostreams/filter/gzip.hpp>
namespace HEJ{
namespace{
bool is_gzip(std::ifstream & file){
static constexpr char magic_bytes[] = {'\x1f', '\x8b'};
if(file.peek() != magic_bytes[0]) return false;
file.get();
const char second = file.peek();
file.unget();
return second == magic_bytes[1];
}
}
istream::istream(std::string const & filename):
file_{filename, std::ios_base::in | std::ios_base::binary},
stream_{new boost_istream()}
{
if(is_gzip(file_)){
stream_->push(boost::iostreams::gzip_decompressor{});
}
stream_->push(file_);
}
}
diff --git a/t/ME_data/config_mt.yml b/t/ME_data/config_mt.yml
index f73d425..eae06e5 100644
--- a/t/ME_data/config_mt.yml
+++ b/t/ME_data/config_mt.yml
@@ -1,30 +1,29 @@
trials: 1
min extparton pt: 30
resummation jets:
min pt: 30
algorithm: antikt
R: 0.4
fixed order jets:
min pt: 30
FKL: reweight
unordered: reweight
qqx: discard
non-HEJ: discard
scales: 125
log correction: false
-unweight: false
random generator:
name: mixmax
seed: 1
Higgs coupling:
use impact factors: false
mt: 174
include bottom: false
diff --git a/t/ME_data/config_mtinf.yml b/t/ME_data/config_mtinf.yml
index 6fc22c8..dbac6c1 100644
--- a/t/ME_data/config_mtinf.yml
+++ b/t/ME_data/config_mtinf.yml
@@ -1,25 +1,24 @@
trials: 1
min extparton pt: 30
resummation jets:
min pt: 30
algorithm: antikt
R: 0.4
fixed order jets:
min pt: 30
FKL: reweight
unordered: reweight
qqx: discard
non-HEJ: discard
scales: 125
log correction: false
-unweight: false
random generator:
name: mixmax
seed: 1
diff --git a/t/ME_data/config_mtmb.yml b/t/ME_data/config_mtmb.yml
index 2085363..5f965cd 100644
--- a/t/ME_data/config_mtmb.yml
+++ b/t/ME_data/config_mtmb.yml
@@ -1,31 +1,30 @@
trials: 1
min extparton pt: 30
resummation jets:
min pt: 30
algorithm: antikt
R: 0.4
fixed order jets:
min pt: 30
FKL: reweight
unordered: reweight
qqx: discard
non-HEJ: discard
scales: 125
log correction: false
-unweight: false
random generator:
name: mixmax
seed: 1
Higgs coupling:
use impact factors: false
mt: 174
include bottom: true
mb: 4.7
diff --git a/t/check_res.cc b/t/check_res.cc
index e4c30a8..294a8d1 100644
--- a/t/check_res.cc
+++ b/t/check_res.cc
@@ -1,99 +1,101 @@
#include <iostream>
#include "LHEF/LHEF.h"
-#include "HEJ/stream.hh"
+
+#include "HEJ/Event.hh"
#include "HEJ/EventReweighter.hh"
#include "HEJ/Mixmax.hh"
+#include "HEJ/stream.hh"
namespace{
const fastjet::JetDefinition jet_def{fastjet::kt_algorithm, 0.4};
const fastjet::JetDefinition Born_jet_def{jet_def};
constexpr double Born_jetptmin = 30;
constexpr double extpartonptmin = 30;
constexpr double max_ext_soft_pt_fraction =
std::numeric_limits<double>::infinity();
constexpr double jetptmin = 35;
constexpr bool log_corr = false;
using EventTreatment = HEJ::EventTreatment;
using namespace HEJ::event_type;
HEJ::EventTreatMap treat{
{no_2_jets, EventTreatment::discard},
{bad_final_state, EventTreatment::discard},
{nonHEJ, EventTreatment::discard},
{unof, EventTreatment::discard},
{unob, EventTreatment::discard},
{qqxexb, EventTreatment::discard},
{qqxexf, EventTreatment::discard},
{qqxmid, EventTreatment::discard},
{FKL, EventTreatment::reweight}
};
};
int main(int argn, char** argv) {
if(argn == 5 && std::string(argv[4]) == "uno"){
--argn;
treat[unof] = EventTreatment::reweight;
treat[unob] = EventTreatment::reweight;
treat[FKL] = EventTreatment::discard;
}
if(argn != 4){
std::cerr << "Usage: check_res eventfile xsection tolerance [uno]";
return EXIT_FAILURE;
}
const double xsec_ref = std::stod(argv[2]);
const double tolerance = std::stod(argv[3]);
HEJ::istream in{argv[1]};
LHEF::Reader reader{in};
HEJ::PhaseSpacePointConfig psp_conf;
psp_conf.jet_param = HEJ::JetParameters{jet_def, jetptmin};
psp_conf.min_extparton_pt = extpartonptmin;
psp_conf.max_ext_soft_pt_fraction = max_ext_soft_pt_fraction;
HEJ::MatrixElementConfig ME_conf;
ME_conf.log_correction = log_corr;
ME_conf.Higgs_coupling = HEJ::HiggsCouplingSettings{};
HEJ::EventReweighterConfig conf;
conf.psp_config = std::move(psp_conf);
conf.ME_config = std::move(ME_conf);
conf.jet_param = psp_conf.jet_param;
conf.treat = treat;
reader.readEvent();
const bool has_Higgs = std::find(
begin(reader.hepeup.IDUP),
end(reader.hepeup.IDUP),
25
) != end(reader.hepeup.IDUP);
const double mu = has_Higgs?125.:91.188;
HEJ::ScaleGenerator scale_gen{
{{std::to_string(mu), HEJ::FixedScale{mu}}}, {}, 1.
};
HEJ::Mixmax ran{};
HEJ::EventReweighter hej{reader.heprup, std::move(scale_gen), conf, ran};
double xsec = 0.;
double xsec_err = 0.;
do{
HEJ::Event ev{
HEJ::UnclusteredEvent{reader.hepeup},
Born_jet_def, Born_jetptmin
};
auto resummed_events = hej.reweight(ev, 20);
for(auto const & ev: resummed_events) {
xsec += ev.central().weight;
xsec_err += ev.central().weight*ev.central().weight;
}
} while(reader.readEvent());
xsec_err = std::sqrt(xsec_err);
const double significance =
std::abs(xsec - xsec_ref) / std::sqrt( xsec_err*xsec_err + tolerance*tolerance );
std::cout << xsec_ref << " +/- " << tolerance << " ~ "
<< xsec << " +- " << xsec_err << " => " << significance << " sigma\n";
if(significance > 3.){
std::cerr << "Cross section is off by over 3 sigma!\n";
return EXIT_FAILURE;
}
}
diff --git a/t/jet_config.yml b/t/jet_config.yml
index 324ced5..510c3f0 100644
--- a/t/jet_config.yml
+++ b/t/jet_config.yml
@@ -1,27 +1,26 @@
trials: 10
min extparton pt: 30
resummation jets:
min pt: 35
algorithm: antikt
R: 0.4
fixed order jets:
min pt: 30
FKL: reweight
unordered: discard
qqx: discard
non-HEJ: discard
log correction: false
-unweight: false
scales: 91.188
random generator:
name: ranlux64
event output:
- tst.lhe
diff --git a/t/jet_config_with_import.yml b/t/jet_config_with_import.yml
index 5988914..aeb3566 100644
--- a/t/jet_config_with_import.yml
+++ b/t/jet_config_with_import.yml
@@ -1,30 +1,29 @@
trials: 10
min extparton pt: 30
resummation jets:
min pt: 35
algorithm: antikt
R: 0.4
fixed order jets:
min pt: 30
FKL: reweight
unordered: discard
qqx: discard
non-HEJ: discard
log correction: false
-unweight: false
scales: softest_jet_pt
event output:
- tst.lhe
random generator:
name: ranlux64
import scales:
./libscales.so: softest_jet_pt
diff --git a/t/test_ME_generic.cc b/t/test_ME_generic.cc
index 33a9077..00e19f0 100644
--- a/t/test_ME_generic.cc
+++ b/t/test_ME_generic.cc
@@ -1,104 +1,104 @@
// Generic tester for the ME for a given set of PSP
// reference weights and PSP (as LHE file) have to be given as _individual_ files
#include <fstream>
#include "LHEF/LHEF.h"
#include "HEJ/MatrixElement.hh"
#include "HEJ/Event.hh"
#include "HEJ/YAMLreader.hh"
#include "HEJ/stream.hh"
constexpr double alpha_s = 0.118;
constexpr double ep = 1e-6;
void dump(HEJ::Event const & ev){
{
LHEF::Writer writer{std::cout};
std::cout << std::setprecision(6);
writer.hepeup = to_HEPEUP(std::move(ev), nullptr);
writer.writeEvent();
}
std::cout << "Rapidity ordering:\n";
for(const auto & part: ev.outgoing()){
std::cout << std::setw(2) << part.type << ": "<< std::setw(7) << part.rapidity() << std::endl;
}
}
int main(int argn, char** argv){
if(argn != 4 && argn != 5){
std::cerr << "\n# Usage:\n."<< argv[0] <<" config.yml ME_weights input_file.lhe\n\n";
return EXIT_FAILURE;
}
bool OUTPUT_MODE = false;
if(argn == 5 && std::string("OUTPUT")==std::string(argv[4]))
OUTPUT_MODE = true;
const HEJ::Config config = HEJ::load_config(argv[1]);
std::fstream wgt_file;
if ( OUTPUT_MODE ) {
std::cout << "_______________________USING OUTPUT MODE!_______________________" << std::endl;
wgt_file.open(argv[2], std::fstream::out);
wgt_file.precision(10);
} else {
wgt_file.open(argv[2], std::fstream::in);
}
HEJ::istream in{argv[3]};
LHEF::Reader reader{in};
HEJ::MatrixElement ME{
[](double){ return alpha_s; },
HEJ::to_MatrixElementConfig(config)
};
double max_ratio = 0.;
size_t idx_max_ratio = 0;
HEJ::Event ev_max_ratio;
double av_ratio = 0;
size_t i = 0;
while(reader.readEvent()){
++i;
HEJ::Event event{
HEJ::UnclusteredEvent{reader.hepeup},
config.resummation_jets.def,
config.resummation_jets.min_pt
};
- const double our_ME = ME.tree(event, true).central;
+ const double our_ME = ME.tree(event).central;
if ( OUTPUT_MODE ) {
wgt_file << our_ME << std::endl;
} else {
std::string line;
if(!std::getline(wgt_file,line)) break;
const double ref_ME = std::stod(line);
const double diff = std::abs(our_ME/ref_ME-1.);
av_ratio+=diff;
if( diff > max_ratio ) {
max_ratio = diff;
idx_max_ratio = i;
ev_max_ratio = event;
}
if( diff > ep ){
size_t precision(std::cout.precision());
std::cout.precision(16);
std::cout<< "Large difference in PSP " << i << "\nis: "<<our_ME << " should: " << ref_ME << " => difference: " << diff << std::endl;
std::cout.precision(precision);
dump(event);
return EXIT_FAILURE;
}
}
}
wgt_file.close();
if ( !OUTPUT_MODE ) {
size_t precision(std::cout.precision());
std::cout.precision(16);
std::cout << "Avg ratio after " << i << " PSP: " << av_ratio/i << std::endl;
std::cout << "maximal ratio at " << idx_max_ratio << ": " << max_ratio << std::endl;
std::cout.precision(precision);
}
return EXIT_SUCCESS;
}
diff --git a/t/test_ME_jets.cc b/t/test_ME_jets.cc
deleted file mode 100644
index c26f1df..0000000
--- a/t/test_ME_jets.cc
+++ /dev/null
@@ -1,81 +0,0 @@
-#include "LHEF/LHEF.h"
-#include "HEJ/MatrixElement.hh"
-#include "HEJ/Event.hh"
-
-struct Event{
- double weight;
- std::array<HEJ::Particle, 2> incoming;
- std::vector<HEJ::Particle> outgoing;
-
- Event(
- double wt,
- HEJ::Particle in1, HEJ::Particle in2,
- std::initializer_list<HEJ::Particle> out
- ):
- weight{wt},
- incoming{std::move(in1), std::move(in2)},
- outgoing{out}
- {}
-};
-
-constexpr
-HEJ::pid::ParticleID PDG(int id){
- return static_cast<HEJ::pid::ParticleID>(id);
-}
-
-constexpr double alpha_s = 0.119002421608181;
-constexpr double mu = 91.188;
-constexpr double R = 0.4;
-constexpr double min_jet_pt = 20.;
-constexpr auto jet_def = fastjet::antikt_algorithm;
-constexpr double ep = 1e-9;
-
-void dump(Event const & ev){
- LHEF::Writer writer{std::cerr};
- std::cerr << std::setprecision(15);
- HEJ::UnclusteredEvent tmp;
- tmp.incoming = ev.incoming;
- tmp.outgoing = ev.outgoing;
- tmp.central = {mu, mu, 0.};
- HEJ::Event out_ev{std::move(tmp), {jet_def, R}, min_jet_pt};
- writer.hepeup = to_HEPEUP(std::move(out_ev), nullptr);
- writer.writeEvent();
-}
-
-int main(){
- std::vector<Event> events = {
- /*
- * reference matrix elements obtained from traditional HEJ
- * weights correspond to wt the end of MEt2 in Jets.cxx
- */
-#include "ME_jets.dat"
- };
-
- HEJ::MatrixElementConfig config;
- config.jet_param.def = fastjet::JetDefinition(jet_def, R);
- config.jet_param.min_pt = min_jet_pt;
- config.log_correction = false;
-
- HEJ::MatrixElement ME{
- [](double){ return alpha_s; },
- config
- };
- for(size_t i = 0; i < events.size(); ++i){
- std::sort(
- begin(events[i].outgoing), end(events[i].outgoing),
- HEJ::rapidity_less{}
- );
- const double our_ME = ME.tree(
- mu, events[i].incoming, events[i].outgoing, true
- );
- const double deviation = our_ME/events[i].weight - 1.;
- if(std::abs(deviation) > ep){
- std::cerr
- << "Matrix element deviates by factor of " << 1+deviation << ":\n"
- "Is " << our_ME << ", should be " << events[i].weight << "\n"
- "Event:\n";
- dump(events[i]);
- return EXIT_FAILURE;
- }
- }
-}
diff --git a/t/test_descriptions.cc b/t/test_descriptions.cc
index 88004d2..d212ad5 100644
--- a/t/test_descriptions.cc
+++ b/t/test_descriptions.cc
@@ -1,61 +1,62 @@
#include <iostream>
#include <cstddef>
-#include "HEJ/ScaleFunction.hh"
+#include "HEJ/Event.hh"
#include "HEJ/EventReweighter.hh"
+#include "HEJ/ScaleFunction.hh"
#define ASSERT(x) if(!(x)) { \
std::cerr << "Assertion '" #x "' failed.\n"; \
return EXIT_FAILURE; \
}
int main() {
constexpr double mu = 125.;
HEJ::ScaleFunction fun{"125", HEJ::FixedScale{mu}};
ASSERT(fun.name() == "125");
HEJ::ScaleGenerator scale_gen{
{std::move(fun)}, {0.5, 1, 2.}, 2.1
};
HEJ::UnclusteredEvent tmp;
tmp.outgoing.push_back(
{HEJ::ParticleID::gluon, fastjet::PtYPhiM(50., -1., 0.3, 0.)}
);
tmp.outgoing.push_back(
{HEJ::ParticleID::gluon, fastjet::PtYPhiM(30., 1., -0.3, 0.)}
);
HEJ::Event ev{
std::move(tmp),
fastjet::JetDefinition{fastjet::kt_algorithm, 0.4},
20.
};
auto rescaled = scale_gen(std::move(ev));
ASSERT(rescaled.central().description->scale_name == "125");
for(auto const & var: rescaled.variations()) {
ASSERT(var.description->scale_name == "125");
}
ASSERT(rescaled.central().description->mur_factor == 1.);
ASSERT(rescaled.central().description->muf_factor == 1.);
ASSERT(rescaled.variations(0).description->mur_factor == 1.);
ASSERT(rescaled.variations(0).description->muf_factor == 1.);
ASSERT(rescaled.variations(1).description->mur_factor == 0.5);
ASSERT(rescaled.variations(1).description->muf_factor == 0.5);
ASSERT(rescaled.variations(2).description->mur_factor == 0.5);
ASSERT(rescaled.variations(2).description->muf_factor == 1.);
ASSERT(rescaled.variations(3).description->mur_factor == 1.);
ASSERT(rescaled.variations(3).description->muf_factor == 0.5);
ASSERT(rescaled.variations(4).description->mur_factor == 1.);
ASSERT(rescaled.variations(4).description->muf_factor == 2.);
ASSERT(rescaled.variations(5).description->mur_factor == 2.);
ASSERT(rescaled.variations(5).description->muf_factor == 1.);
ASSERT(rescaled.variations(6).description->mur_factor == 2.);
ASSERT(rescaled.variations(6).description->muf_factor == 2.);
}
diff --git a/t/test_scale_arithmetics.cc b/t/test_scale_arithmetics.cc
new file mode 100644
index 0000000..015dd6a
--- /dev/null
+++ b/t/test_scale_arithmetics.cc
@@ -0,0 +1,87 @@
+
+// Generic tester for the ME for a given set of PSP
+// reference weights and PSP (as LHE file) have to be given as _individual_ files
+
+#include <fstream>
+
+#include "LHEF/LHEF.h"
+
+#include "HEJ/EventReweighter.hh"
+#include "HEJ/make_RNG.hh"
+#include "HEJ/Event.hh"
+#include "HEJ/YAMLreader.hh"
+#include "HEJ/stream.hh"
+
+constexpr double alpha_s = 0.118;
+constexpr double ep = 1e-13;
+
+void dump(HEJ::Event const & ev){
+ {
+ LHEF::Writer writer{std::cout};
+ std::cout << std::setprecision(6);
+ writer.hepeup = to_HEPEUP(std::move(ev), nullptr);
+ writer.writeEvent();
+ }
+ std::cout << "Rapidity ordering:\n";
+ for(const auto & part: ev.outgoing()){
+ std::cout << std::setw(2) << part.type << ": "<< std::setw(7) << part.rapidity() << std::endl;
+ }
+}
+
+int main(int argn, char** argv){
+ if(argn != 3){
+ std::cerr << "\n# Usage:\n."<< argv[0] <<" config.yml input_file.lhe\n\n";
+ return EXIT_FAILURE;
+ }
+ HEJ::Config config = HEJ::load_config(argv[1]);
+ config.scales = HEJ::to_ScaleConfig(
+ YAML::Load("scales: [H_T, 1 * H_T, 2/2 * H_T, 2*H_T/2, H_T/2*2, H_T/2/2*4, H_T*H_T/H_T]")
+ );
+
+ HEJ::istream in{argv[2]};
+ LHEF::Reader reader{in};
+
+ auto ran = HEJ::make_RNG(config.rng.name, config.rng.seed);
+
+ HEJ::ScaleGenerator scale_gen{
+ config.scales.base,
+ config.scales.factors,
+ config.scales.max_ratio
+ };
+
+ HEJ::EventReweighter resum{
+ reader.heprup,
+ std::move(scale_gen),
+ to_EventReweighterConfig(config),
+ *ran
+ };
+
+ size_t i = 0;
+ while(reader.readEvent()){
+ ++i;
+
+ HEJ::Event event{
+ HEJ::UnclusteredEvent{reader.hepeup},
+ config.resummation_jets.def,
+ config.resummation_jets.min_pt
+ };
+
+ auto resummed = resum.reweight(event, config.trials);
+ for(auto && ev: resummed) {
+ for(auto &&var: ev.variations()) {
+ if(std::abs(var.muf - ev.central().muf) > ep) {
+ std::cerr
+ << std::setprecision(15)
+ << "unequal scales: " << var.muf
+ << " != " << ev.central().muf << '\n'
+ << "in resummed event:\n";
+ dump(ev);
+ std::cerr << "\noriginal event:\n";
+ dump(event);
+ return EXIT_FAILURE;
+ }
+ }
+ }
+ }
+
+}

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