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diff --git a/MatrixElement/DIS/DISBase.h b/MatrixElement/DIS/DISBase.h
--- a/MatrixElement/DIS/DISBase.h
+++ b/MatrixElement/DIS/DISBase.h
@@ -1,471 +1,469 @@
// -*- C++ -*-
#ifndef HERWIG_DISBase_H
#define HERWIG_DISBase_H
//
// This is the declaration of the DISBase class.
//
#include "Herwig/MatrixElement/HwMEBase.h"
#include "Herwig/Shower/QTilde/Couplings/ShowerAlpha.h"
-#include "Herwig/Shower/QTilde/Base/ShowerTree.fh"
-#include "Herwig/Shower/QTilde/Base/HardTree.fh"
namespace Herwig {
using namespace ThePEG;
/**
* The DISBase class is the base class for the implementation
* of DIS type processes including corrections in both the old
* fashioned matrix element and POWHEG approaches
*
* @see \ref DISBaseInterfaces "The interfaces"
* defined for DISBase.
*/
class DISBase: public HwMEBase {
public:
/**
* The default constructor.
*/
DISBase();
/**
* The default constructor.
*/
virtual ~DISBase();
/**
* Members for the old-fashioned matrix element correction
*/
//@{
/**
* Has an old fashioned ME correction
*/
virtual bool hasMECorrection() {return true;}
/**
* Initialize the ME correction
*/
virtual void initializeMECorrection(RealEmissionProcessPtr, double &,
double & );
/**
* Apply the hard matrix element correction to a given hard process or decay
*/
virtual RealEmissionProcessPtr applyHardMatrixElementCorrection(RealEmissionProcessPtr);
/**
* Apply the soft matrix element correction
* @param initial The particle from the hard process which started the
* shower
* @param parent The initial particle in the current branching
* @param br The branching struct
* @return If true the emission should be vetoed
*/
virtual bool softMatrixElementVeto(ShowerProgenitorPtr,
ShowerParticlePtr,Branching);
//@}
/**
* Members for the POWHEG stype correction
*/
//@{
/**
* Has a POWHEG style correction
*/
virtual POWHEGType hasPOWHEGCorrection() {return Both;}
/**
* Apply the POWHEG style correction
*/
virtual RealEmissionProcessPtr generateHardest(RealEmissionProcessPtr,
ShowerInteraction::Type);
//@}
public:
/** @name Virtual functions required by the MEBase class. */
//@{
/**
* Return the scale associated with the last set phase space point.
*/
virtual Energy2 scale() const;
/**
* The number of internal degrees of freedom used in the matrix
* element.
*/
virtual int nDim() const;
/**
* Generate internal degrees of freedom given nDim() uniform
* random numbers in the interval \f$ ]0,1[ \f$. To help the phase space
* generator, the dSigHatDR should be a smooth function of these
* numbers, although this is not strictly necessary.
* @param r a pointer to the first of nDim() consecutive random numbers.
* @return true if the generation succeeded, otherwise false.
*/
virtual bool generateKinematics(const double * r);
/**
* Return the matrix element squared differential in the variables
* given by the last call to generateKinematics().
*/
virtual CrossSection dSigHatDR() const;
//@}
public:
/** @name Functions used by the persistent I/O system. */
//@{
/**
* Function used to write out object persistently.
* @param os the persistent output stream written to.
*/
void persistentOutput(PersistentOStream & os) const;
/**
* Function used to read in object persistently.
* @param is the persistent input stream read from.
* @param version the version number of the object when written.
*/
void persistentInput(PersistentIStream & is, int version);
//@}
/**
* The standard Init function used to initialize the interfaces.
* Called exactly once for each class by the class description system
* before the main function starts or
* when this class is dynamically loaded.
*/
static void Init();
protected:
/** @name Standard Interfaced functions. */
//@{
/**
* Initialize this object after the setup phase before saving an
* EventGenerator to disk.
* @throws InitException if object could not be initialized properly.
*/
virtual void doinit();
//@}
private:
/**
* The static object used to initialize the description of this class.
* Indicates that this is an abstract class with persistent data.
*/
static AbstractClassDescription<DISBase> initDISBase;
/**
* The assignment operator is private and must never be called.
* In fact, it should not even be implemented.
*/
DISBase & operator=(const DISBase &);
protected:
/**
* The NLO weight
*/
double NLOWeight() const;
/**
* Calculate the coefficient A for the correlations
*/
virtual double A(tcPDPtr lin, tcPDPtr lout, tcPDPtr qin, tcPDPtr qout,
Energy2 scale) const =0;
/**
* Members for the matrix element correction
*/
//@{
/**
* Generate the values of \f$x_p\f$ and \f$z_p\f$
* @param xp The value of xp, output
* @param zp The value of zp, output
*/
double generateComptonPoint(double &xp, double & zp);
/**
* Generate the values of \f$x_p\f$ and \f$z_p\f$
* @param xp The value of xp, output
* @param zp The value of zp, output
*/
double generateBGFPoint(double &xp, double & zp);
/**
* Return the coefficients for the matrix element piece for
* the QCD compton case. The output is the \f$a_i\f$ coefficients to
* give the function as
* \f$a_0+a_1\cos\phi+a_2\sin\phi+a_3\cos^2\phi+a_4\sin^2\phi\f$
* @param xp \f$x_p\f$
* @param x2 \f$x_2\f$
* @param xperp \f$x_\perp\f$
* @param norm Normalise to the large $l$ value of the ME
*/
vector<double> ComptonME(double xp, double x2, double xperp,
bool norm);
/**
* Return the coefficients for the matrix element piece for
* the QCD compton case. The output is the \f$a_i\f$ coefficients to
* give the function as
* \f$a_0+a_1\cos\phi+a_2\sin\phi+a_3\cos^2\phi+a_4\sin^2\phi\f$
* @param xp \f$x_p\f$
* @param x2 \f$x_3\f$
* @param x3 \f$x_2\f$
* @param xperp \f$x_\perp\f$
* @param norm Normalise to the large $l$ value of the ME
*/
vector<double> BGFME(double xp, double x2, double x3, double xperp,
bool norm);
//@}
/**
* Members for the POWHEG correction
*/
//@{
/**
* Generate a Compton process
*/
void generateCompton();
/**
* Generate a BGF process
*/
void generateBGF();
//@}
private:
/**
* Parameters for the matrix element correction
*/
//@{
/**
* Enchancement factor for ISR
*/
double initial_;
/**
* Enchancement factor for FSR
*/
double final_;
/**
* Relative fraction of compton and BGF processes to generate
*/
double procProb_;
/**
* Integral for compton process
*/
double comptonInt_;
/**
* Integral for BGF process
*/
double bgfInt_;
//@}
/**
* Parameters for the POWHEG correction
*/
//@{
/**
* Weight for the compton channel
*/
double comptonWeight_;
/**
* Weight for the BGF channel
*/
double BGFWeight_;
/**
* Minimum value of \f$p_T\f$
*/
Energy pTmin_;
//@}
/**
* Parameters for the point being generated
*/
//@{
/**
* \f$Q^2\f$
*/
Energy2 q2_;
/**
*
*/
double l_;
/**
* Borm momentum fraction
*/
double xB_;
/**
* Beam particle
*/
tcBeamPtr beam_;
/**
* Partons
*/
tcPDPtr partons_[2];
/**
* Leptons
*/
tcPDPtr leptons_[2];
/**
* PDF object
*/
tcPDFPtr pdf_;
/**
* Rotation to the Breit frame
*/
LorentzRotation rot_;
/**
* Lepton momenta
*/
Lorentz5Momentum pl_[2];
/**
* Quark momenta
*/
Lorentz5Momentum pq_[2];
/**
* q
*/
Lorentz5Momentum q_;
/**
* Compton parameters
*/
Energy pTCompton_;
bool ComptonISFS_;
vector<Lorentz5Momentum> ComptonMomenta_;
/**
* BGF parameters
*/
Energy pTBGF_;
vector<Lorentz5Momentum> BGFMomenta_;
//@}
/**
* The coefficient for the correlations
*/
double acoeff_;
/**
* Coupling
*/
ShowerAlphaPtr alpha_;
/**
* Gluon particle data object
*/
PDPtr gluon_;
private:
/**
* The radiative variables
*/
//@{
/**
* The \f$x_p\f$ or \f$z\f$ real integration variable
*/
double xp_;
//@}
/**
* The hadron
*/
tcBeamPtr hadron_;
/**
* Selects a dynamic or fixed factorization scale
*/
unsigned int scaleOpt_;
/**
* The factorization scale
*/
Energy muF_;
/**
* Prefactor if variable scale used
*/
double scaleFact_;
/**
* Whether to generate the positive, negative or leading order contribution
*/
unsigned int contrib_;
/**
* Power for sampling \f$x_p\f$
*/
double power_;
/**
* Jacobian for \f$x_p\f$ integral
*/
double jac_;
};
}
#include "ThePEG/Utilities/ClassTraits.h"
namespace ThePEG {
/** @cond TRAITSPECIALIZATIONS */
/** This template specialization informs ThePEG about the
* base classes of DISBase. */
template <>
struct BaseClassTrait<Herwig::DISBase,1> {
/** Typedef of the first base class of DISBase. */
typedef Herwig::HwMEBase NthBase;
};
/** This template specialization informs ThePEG about the name of
* the DISBase class and the shared object where it is defined. */
template <>
struct ClassTraits<Herwig::DISBase>
: public ClassTraitsBase<Herwig::DISBase> {
/** Return a platform-independent class name */
static string className() { return "Herwig::DISBase"; }
/**
* The name of a file containing the dynamic library where the class
* MENeutralCurrentDIS is implemented. It may also include several, space-separated,
* libraries if the class MENeutralCurrentDIS depends on other classes (base classes
* excepted). In this case the listed libraries will be dynamically
* linked in the order they are specified.
*/
static string library() { return "HwMEDIS.so"; }
};
/** @endcond */
}
#endif /* HERWIG_DISBase_H */
diff --git a/MatrixElement/Lepton/MEee2gZ2qq.cc b/MatrixElement/Lepton/MEee2gZ2qq.cc
--- a/MatrixElement/Lepton/MEee2gZ2qq.cc
+++ b/MatrixElement/Lepton/MEee2gZ2qq.cc
@@ -1,985 +1,987 @@
// -*- C++ -*-
//
// MEee2gZ2qq.cc is a part of Herwig - A multi-purpose Monte Carlo event generator
// Copyright (C) 2002-2011 The Herwig Collaboration
//
// Herwig is licenced under version 2 of the GPL, see COPYING for details.
// Please respect the MCnet academic guidelines, see GUIDELINES for details.
//
//
// This is the implementation of the non-inlined, non-templated member
// functions of the MEee2gZ2qq class.
//
#include "MEee2gZ2qq.h"
#include "ThePEG/Interface/ClassDocumentation.h"
#include "ThePEG/Interface/Switch.h"
#include "ThePEG/Interface/Parameter.h"
#include "ThePEG/Interface/Reference.h"
#include "ThePEG/Persistency/PersistentOStream.h"
#include "ThePEG/Persistency/PersistentIStream.h"
#include "ThePEG/PDT/EnumParticles.h"
#include "ThePEG/MatrixElement/Tree2toNDiagram.h"
#include "ThePEG/Handlers/StandardXComb.h"
#include "Herwig/MatrixElement/HardVertex.h"
#include "Herwig/Shower/QTilde/Base/Branching.h"
-#include "Herwig/Shower/QTilde/Base/HardTree.h"
#include "ThePEG/PDF/PolarizedBeamParticleData.h"
#include <numeric>
#include "ThePEG/Utilities/DescribeClass.h"
#include "Herwig/Shower/RealEmissionProcess.h"
+#include "Herwig/Shower/QTilde/Base/ShowerProgenitor.h"
+#include "Herwig/Shower/QTilde/Base/Branching.h"
+
using namespace Herwig;
const double MEee2gZ2qq::EPS_=0.00000001;
void MEee2gZ2qq::doinit() {
HwMEBase::doinit();
massOption(vector<unsigned int>(2,massopt_));
rescalingOption(3);
if(minflav_>maxflav_)
throw InitException() << "The minimum flavour " << minflav_
<< "must be lower the than maximum flavour " << maxflav_
<< " in MEee2gZ2qq::doinit() "
<< Exception::runerror;
// set the particle data objects
Z0_ = getParticleData(ParticleID::Z0);
gamma_ = getParticleData(ParticleID::gamma);
gluon_ = getParticleData(ParticleID::g);
// cast the SM pointer to the Herwig SM pointer
tcHwSMPtr hwsm= dynamic_ptr_cast<tcHwSMPtr>(standardModel());
// do the initialisation
if(!hwsm) throw InitException()
<< "Wrong type of StandardModel object in "
<< "MEee2gZ2qq::doinit() the Herwig version must be used"
<< Exception::runerror;
FFZVertex_ = hwsm->vertexFFZ();
FFPVertex_ = hwsm->vertexFFP();
FFGVertex_ = hwsm->vertexFFG();
}
void MEee2gZ2qq::getDiagrams() const {
// specific the diagrams
tcPDPtr ep = getParticleData(ParticleID::eplus);
tcPDPtr em = getParticleData(ParticleID::eminus);
tcPDPtr gamma = getParticleData(ParticleID::gamma);
tcPDPtr Z0 = getParticleData(ParticleID::Z0);
// setup the processes
for ( int i =minflav_; i<=maxflav_; ++i ) {
tcPDPtr qk = getParticleData(i);
tcPDPtr qb = qk->CC();
add(new_ptr((Tree2toNDiagram(2), em, ep, 1, gamma, 3, qk, 3, qb, -1)));
add(new_ptr((Tree2toNDiagram(2), em, ep, 1, Z0 , 3, qk, 3, qb, -2)));
}
}
Energy2 MEee2gZ2qq::scale() const {
return sqr(getParticleData(ParticleID::Z0)->mass());
// return sHat();
}
unsigned int MEee2gZ2qq::orderInAlphaS() const {
return 0;
}
unsigned int MEee2gZ2qq::orderInAlphaEW() const {
return 2;
}
Selector<MEBase::DiagramIndex>
MEee2gZ2qq::diagrams(const DiagramVector & diags) const {
double lastCont(0.5),lastBW(0.5);
if ( lastXCombPtr() ) {
lastCont = meInfo()[0];
lastBW = meInfo()[1];
}
Selector<DiagramIndex> sel;
for ( DiagramIndex i = 0; i < diags.size(); ++i ) {
if ( diags[i]->id() == -1 ) sel.insert(lastCont, i);
else if ( diags[i]->id() == -2 ) sel.insert(lastBW, i);
}
return sel;
}
Selector<const ColourLines *>
MEee2gZ2qq::colourGeometries(tcDiagPtr ) const {
static const ColourLines c("-5 4");
Selector<const ColourLines *> sel;
sel.insert(1.0, &c);
return sel;
}
void MEee2gZ2qq::persistentOutput(PersistentOStream & os) const {
os << FFZVertex_ << FFPVertex_ << FFGVertex_
<< Z0_ << gamma_ << gluon_ << minflav_
<< maxflav_ << massopt_ << alphaQCD_ << alphaQED_
<< ounit(pTminQED_,GeV) << ounit(pTminQCD_,GeV) << preFactor_
<< spinCorrelations_;
}
void MEee2gZ2qq::persistentInput(PersistentIStream & is, int) {
is >> FFZVertex_ >> FFPVertex_ >> FFGVertex_
>> Z0_ >> gamma_ >> gluon_ >> minflav_
>> maxflav_ >> massopt_ >> alphaQCD_ >> alphaQED_
>> iunit(pTminQED_,GeV) >> iunit(pTminQCD_,GeV) >> preFactor_
>> spinCorrelations_;
}
// The following static variable is needed for the type
// description system in ThePEG.
DescribeClass<MEee2gZ2qq,HwMEBase>
describeMEee2gZ2qq("Herwig::MEee2gZ2qq", "HwMELepton.so");
void MEee2gZ2qq::Init() {
static ClassDocumentation<MEee2gZ2qq> documentation
("The MEee2gZ2qq class implements the matrix element for e+e- -> q qbar");
static Parameter<MEee2gZ2qq,int> interfaceMinimumFlavour
("MinimumFlavour",
"The PDG code of the quark with the lowest PDG code to produce.",
&MEee2gZ2qq::minflav_, 1, 1, 6,
false, false, Interface::limited);
static Parameter<MEee2gZ2qq,int> interfaceMaximumFlavour
("MaximumFlavour",
"The PDG code of the quark with the highest PDG code to produce",
&MEee2gZ2qq::maxflav_, 5, 1, 6,
false, false, Interface::limited);
static Switch<MEee2gZ2qq,unsigned int> interfaceTopMassOption
("TopMassOption",
"Option for the treatment of the top quark mass",
&MEee2gZ2qq::massopt_, 1, false, false);
static SwitchOption interfaceTopMassOptionOnMassShell
(interfaceTopMassOption,
"OnMassShell",
"The top is produced on its mass shell",
1);
static SwitchOption interfaceTopMassOption2
(interfaceTopMassOption,
"OffShell",
"The top is generated off-shell using the mass and width generator.",
2);
static Parameter<MEee2gZ2qq,Energy> interfacepTMinQED
("pTMinQED",
"Minimum pT for hard QED radiation",
&MEee2gZ2qq::pTminQED_, GeV, 1.0*GeV, 0.001*GeV, 10.0*GeV,
false, false, Interface::limited);
static Parameter<MEee2gZ2qq,Energy> interfacepTMinQCD
("pTMinQCD",
"Minimum pT for hard QCD radiation",
&MEee2gZ2qq::pTminQCD_, GeV, 1.0*GeV, 0.001*GeV, 10.0*GeV,
false, false, Interface::limited);
static Parameter<MEee2gZ2qq,double> interfacePrefactor
("Prefactor",
"Prefactor for the overestimate of the emission probability",
&MEee2gZ2qq::preFactor_, 6.0, 1.0, 100.0,
false, false, Interface::limited);
static Reference<MEee2gZ2qq,ShowerAlpha> interfaceQCDCoupling
("AlphaQCD",
"Pointer to the object to calculate the strong coupling for the correction",
&MEee2gZ2qq::alphaQCD_, false, false, true, false, false);
static Reference<MEee2gZ2qq,ShowerAlpha> interfaceEMCoupling
("AlphaQED",
"Pointer to the object to calculate the EM coupling for the correction",
&MEee2gZ2qq::alphaQED_, false, false, true, false, false);
static Switch<MEee2gZ2qq,bool> interfaceSpinCorrelations
("SpinCorrelations",
"Switch the construction of the veretx for spin correlations on/off",
&MEee2gZ2qq::spinCorrelations_, true, false, false);
static SwitchOption interfaceSpinCorrelationsYes
(interfaceSpinCorrelations,
"Yes",
"Swtich On",
true);
static SwitchOption interfaceSpinCorrelationsNo
(interfaceSpinCorrelations,
"No",
"Switch off",
false);
}
double MEee2gZ2qq::me2() const {
return loME(mePartonData(),rescaledMomenta(),true);
}
ProductionMatrixElement MEee2gZ2qq::HelicityME(vector<SpinorWaveFunction> & fin,
vector<SpinorBarWaveFunction> & ain,
vector<SpinorBarWaveFunction> & fout,
vector<SpinorWaveFunction> & aout,
double & me,
double & cont,
double & BW ) const {
// the particles should be in the order
// for the incoming
// 0 incoming fermion (u spinor)
// 1 incoming antifermion (vbar spinor)
// for the outgoing
// 0 outgoing fermion (ubar spinor)
// 1 outgoing antifermion (v spinor)
// me to be returned
ProductionMatrixElement output(PDT::Spin1Half,PDT::Spin1Half,
PDT::Spin1Half,PDT::Spin1Half);
ProductionMatrixElement gamma (PDT::Spin1Half,PDT::Spin1Half,
PDT::Spin1Half,PDT::Spin1Half);
ProductionMatrixElement Zboson(PDT::Spin1Half,PDT::Spin1Half,
PDT::Spin1Half,PDT::Spin1Half);
// wavefunctions for the intermediate particles
VectorWaveFunction interZ,interG;
// temporary storage of the different diagrams
Complex diag1,diag2;
// sum over helicities to get the matrix element
unsigned int inhel1,inhel2,outhel1,outhel2;
double total[3]={0.,0.,0.};
for(inhel1=0;inhel1<2;++inhel1) {
for(inhel2=0;inhel2<2;++inhel2) {
// intermediate Z
interZ = FFZVertex_->evaluate(scale(),1,Z0_,fin[inhel1],ain[inhel2]);
// intermediate photon
interG = FFPVertex_->evaluate(scale(),1,gamma_,fin[inhel1],ain[inhel2]);
for(outhel1=0;outhel1<2;++outhel1) {
for(outhel2=0;outhel2<2;++outhel2) {
// first the Z exchange diagram
diag1 = FFZVertex_->evaluate(scale(),aout[outhel2],fout[outhel1],
interZ);
// then the photon exchange diagram
diag2 = FFPVertex_->evaluate(scale(),aout[outhel2],fout[outhel1],
interG);
// add up squares of individual terms
total[1] += norm(diag1);
Zboson(inhel1,inhel2,outhel1,outhel2) = diag1;
total[2] += norm(diag2);
gamma (inhel1,inhel2,outhel1,outhel2) = diag2;
// the full thing including interference
diag1 += diag2;
total[0] += norm(diag1);
output(inhel1,inhel2,outhel1,outhel2)=diag1;
}
}
}
}
for(int ix=0;ix<3;++ix) total[ix] *= 0.25;
tcPolarizedBeamPDPtr beam[2] =
{dynamic_ptr_cast<tcPolarizedBeamPDPtr>(mePartonData()[0]),
dynamic_ptr_cast<tcPolarizedBeamPDPtr>(mePartonData()[1])};
if( beam[0] || beam[1] ) {
RhoDMatrix rho[2] =
{beam[0] ? beam[0]->rhoMatrix() : RhoDMatrix(mePartonData()[0]->iSpin()),
beam[1] ? beam[1]->rhoMatrix() : RhoDMatrix(mePartonData()[1]->iSpin())};
total[0] = output.average(rho[0],rho[1]);
total[1] = Zboson.average(rho[0],rho[1]);
total[2] = gamma .average(rho[0],rho[1]);
}
// results
for(int ix=0;ix<3;++ix) total[ix]*= 3.;
cont = total[2];
BW = total[1];
me = total[0];
return output;
}
void MEee2gZ2qq::constructVertex(tSubProPtr sub) {
if(!spinCorrelations_) return;
// extract the particles in the hard process
ParticleVector hard;
hard.push_back(sub->incoming().first);
hard.push_back(sub->incoming().second);
hard.push_back(sub->outgoing()[0]);
hard.push_back(sub->outgoing()[1]);
if(hard[0]->id()<hard[1]->id()) swap(hard[0],hard[1]);
if(hard[2]->id()<hard[3]->id()) swap(hard[2],hard[3]);
vector<SpinorWaveFunction> fin,aout;
vector<SpinorBarWaveFunction> ain,fout;
// get wave functions for off-shell momenta for later on
SpinorWaveFunction( fin ,hard[0],incoming,false,true);
SpinorBarWaveFunction(ain ,hard[1],incoming,false,true);
SpinorBarWaveFunction(fout,hard[2],outgoing,true ,true);
SpinorWaveFunction( aout,hard[3],outgoing,true ,true);
// now rescale the momenta and compute the matrix element with the
// rescaled momenta for correlations
vector<Lorentz5Momentum> momenta;
cPDVector data;
for(unsigned int ix=0;ix<4;++ix) {
momenta.push_back(hard[ix]->momentum());
data .push_back(hard[ix]->dataPtr());
}
rescaleMomenta(momenta,data);
SpinorWaveFunction ein (rescaledMomenta()[0],data[0],incoming);
SpinorBarWaveFunction pin (rescaledMomenta()[1],data[1],incoming);
SpinorBarWaveFunction qkout(rescaledMomenta()[2],data[2],outgoing);
SpinorWaveFunction qbout(rescaledMomenta()[3],data[3],outgoing);
for(unsigned int ix=0;ix<2;++ix) {
ein.reset(ix) ; fin [ix] = ein ;
pin.reset(ix) ; ain [ix] = pin ;
qkout.reset(ix); fout[ix] = qkout;
qbout.reset(ix); aout[ix] = qbout;
}
// calculate the matrix element
double me,cont,BW;
ProductionMatrixElement prodme=HelicityME(fin,ain,fout,aout,me,cont,BW);
// construct the vertex
HardVertexPtr hardvertex=new_ptr(HardVertex());
// set the matrix element for the vertex
hardvertex->ME(prodme);
// set the pointers and to and from the vertex
for(unsigned int ix=0;ix<4;++ix) {
tSpinPtr spin = hard[ix]->spinInfo();
if(ix<2) {
tcPolarizedBeamPDPtr beam =
dynamic_ptr_cast<tcPolarizedBeamPDPtr>(hard[ix]->dataPtr());
if(beam) spin->rhoMatrix() = beam->rhoMatrix();
}
spin->productionVertex(hardvertex);
}
}
void MEee2gZ2qq::rebind(const TranslationMap & trans) {
FFZVertex_ = trans.translate(FFZVertex_);
FFPVertex_ = trans.translate(FFPVertex_);
FFGVertex_ = trans.translate(FFGVertex_);
Z0_ = trans.translate(Z0_);
gamma_ = trans.translate(gamma_);
gluon_ = trans.translate(gluon_);
HwMEBase::rebind(trans);
}
IVector MEee2gZ2qq::getReferences() {
IVector ret = HwMEBase::getReferences();
ret.push_back(FFZVertex_);
ret.push_back(FFPVertex_);
ret.push_back(FFGVertex_);
ret.push_back(Z0_ );
ret.push_back(gamma_ );
ret.push_back(gluon_ );
return ret;
}
void MEee2gZ2qq::initializeMECorrection(RealEmissionProcessPtr,
double & initial,
double & final) {
d_Q_ = sqrt(sHat());
d_m_ = 0.5*(meMomenta()[2].mass()+meMomenta()[3].mass());
// set the other parameters
d_rho_ = sqr(d_m_/d_Q_);
d_v_ = sqrt(1.-4.*d_rho_);
// maximum evolution scale
d_kt1_ = (1. + sqrt(1. - 4.*d_rho_))/2.;
double num = d_rho_ * d_kt1_ + 0.25 * d_v_ *(1.+d_v_)*(1.+d_v_);
double den = d_kt1_ - d_rho_;
d_kt2_ = num/den;
// maximums for reweighting
initial = 1.;
final = 1.;
}
RealEmissionProcessPtr MEee2gZ2qq::applyHardMatrixElementCorrection(RealEmissionProcessPtr born) {
return calculateRealEmission(born,true,ShowerInteraction::QCD);
}
RealEmissionProcessPtr MEee2gZ2qq::calculateRealEmission(RealEmissionProcessPtr born, bool veto,
ShowerInteraction::Type inter) {
vector<Lorentz5Momentum> emission;
unsigned int iemit,ispect;
pair<Energy,ShowerInteraction::Type> output =
generateHard(born,emission,iemit,ispect,veto,inter);
if(emission.empty()) {
if(inter!=ShowerInteraction::QCD) born->pT()[ShowerInteraction::QED] = pTminQED_;
if(inter!=ShowerInteraction::QED) born->pT()[ShowerInteraction::QCD] = pTminQCD_;
return born;
}
else {
Energy pTveto = output.first;
if(inter!=ShowerInteraction::QCD) born->pT()[ShowerInteraction::QED] = pTveto;
if(inter!=ShowerInteraction::QED) born->pT()[ShowerInteraction::QCD] = pTveto;
}
// generate the momenta for the hard emission
ShowerInteraction::Type force = output.second;
born->interaction(force);
// get the quark and antiquark
ParticleVector qq;
for(unsigned int ix=0;ix<2;++ix) qq.push_back(born->bornOutgoing()[ix]);
bool order = qq[0]->id()>0;
if(!order) swap(qq[0],qq[1]);
// perform final check to ensure energy greater than constituent mass
for (int i=0; i<2; i++) {
if (emission[i+2].e() < qq[i]->data().constituentMass())
return RealEmissionProcessPtr();
}
if(force!=ShowerInteraction::QED &&
emission[4].e() < gluon_->constituentMass())
return RealEmissionProcessPtr();
// set masses
for (int i=0; i<2; i++) emission[i+2].setMass(qq[i]->mass());
emission[4].setMass(ZERO);
// create the new quark, antiquark and gluon
PPtr newq = qq[0]->dataPtr()->produceParticle(emission[2]);
PPtr newa = qq[1]->dataPtr()->produceParticle(emission[3]);
PPtr newg;
if(force==ShowerInteraction::QCD)
newg = gluon_->produceParticle(emission[4]);
else
newg = gamma_->produceParticle(emission[4]);
// create the output real emission process
for(unsigned int ix=0;ix<born->bornIncoming().size();++ix) {
born->incoming().push_back(born->bornIncoming()[ix]->dataPtr()->
produceParticle(born->bornIncoming()[ix]->momentum()));
}
if(order) {
born->outgoing().push_back(newq);
born->outgoing().push_back(newa);
}
else {
born->outgoing().push_back(newa);
born->outgoing().push_back(newq);
swap(iemit,ispect);
}
born->outgoing().push_back(newg);
// set emitter and spectator
born->emitter (iemit);
born->spectator(ispect);
born->emitted(4);
// make colour connections
if(force==ShowerInteraction::QCD) {
newg->colourNeighbour(newq);
newa->colourNeighbour(newg);
}
else {
newa->colourNeighbour(newq);
}
return born;
}
bool MEee2gZ2qq::softMatrixElementVeto(ShowerProgenitorPtr initial,
ShowerParticlePtr parent,Branching br) {
// check we should be applying the veto
if(parent->id()!=initial->progenitor()->id()||
br.ids[0]->id()!=br.ids[1]->id()||
br.ids[2]->id()!=ParticleID::g) return false;
// calculate pt
double d_z = br.kinematics->z();
Energy d_qt = br.kinematics->scale();
Energy2 d_m2 = parent->momentum().m2();
Energy pPerp = (1.-d_z)*sqrt( sqr(d_z*d_qt) - d_m2);
// if not hardest so far don't apply veto
if(pPerp<initial->highestpT()) return false;
// calculate x and xb
double kti = sqr(d_qt/d_Q_);
double w = sqr(d_v_) + kti*(-1. + d_z)*d_z*(2. + kti*(-1. + d_z)*d_z);
if (w < 0) return false;
double x = (1. + sqr(d_v_)*(-1. + d_z) + sqr(kti*(-1. + d_z))*d_z*d_z*d_z
+ d_z*sqrt(w)
- kti*(-1. + d_z)*d_z*(2. + d_z*(-2 + sqrt(w))))/
(1. - kti*(-1. + d_z)*d_z + sqrt(w));
double xb = 1. + kti*(-1. + d_z)*d_z;
// calculate the weight
if(parent->id()<0) swap(x,xb);
// if exceptionally out of phase space, leave this emission, as there
// is no good interpretation for the soft ME correction.
if( x<0 || xb<0) return false;
double xg = 2. - xb - x;
// always return one in the soft gluon region
if(xg < EPS_) return false;
// check it is in the phase space
if((1.-x)*(1.-xb)*(1.-xg) < d_rho_*xg*xg) {
parent->vetoEmission(parent->id()>0 ? ShowerPartnerType::QCDColourLine :
ShowerPartnerType::QCDColourLine,br.kinematics->scale());
return true;
}
double k1 = getKfromX(x, xb);
double k2 = getKfromX(xb, x);
double weight = 1.;
// quark emission
if(parent->id() > 0 && k1 < d_kt1_) {
weight = MEV(x, xb)/PS(x, xb);
// is it also in the anti-quark emission zone?
if(k2 < d_kt2_) weight *= 0.5;
}
// antiquark emission
if(parent->id() < 0 && k2 < d_kt2_) {
weight = MEV(x, xb)/PS(xb, x);
// is it also in the quark emission zone?
if(k1 < d_kt1_) weight *= 0.5;
}
// compute veto from weight
bool veto = !UseRandom::rndbool(weight);
// if not vetoed reset max
// if vetoing reset the scale
if(veto) {
parent->vetoEmission(parent->id()>0 ? ShowerPartnerType::QCDColourLine :
ShowerPartnerType::QCDColourLine,br.kinematics->scale());
}
// return the veto
return veto;
}
double MEee2gZ2qq::getKfromX(double x1, double x2) {
double uval = 0.5*(1. + d_rho_/(1.-x2+d_rho_));
double num = x1 - (2. - x2)*uval;
double den = sqrt(x2*x2 - 4.*d_rho_);
double zval = uval + num/den;
return (1.-x2)/(zval*(1.-zval));
}
double MEee2gZ2qq::MEV(double x1, double x2) {
// Vector part
double num = (x1+2.*d_rho_)*(x1+2.*d_rho_) + (x2+2.*d_rho_)*(x2+2.*d_rho_)
- 8.*d_rho_*(1.+2.*d_rho_);
double den = (1.+2.*d_rho_)*(1.-x1)*(1.-x2);
return (num/den - 2.*d_rho_/((1.-x1)*(1.-x1))
- 2*d_rho_/((1.-x2)*(1.-x2)))/d_v_;
}
double MEee2gZ2qq::PS(double x, double xbar) {
double u = 0.5*(1. + d_rho_ / (1.-xbar+d_rho_));
double z = u + (x - (2.-xbar)*u)/sqrt(xbar*xbar - 4.*d_rho_);
double brack = (1.+z*z)/(1.-z)- 2.*d_rho_/(1-xbar);
// interesting: the splitting function without the subtraction
// term. Actually gives a much worse approximation in the collinear
// limit. double brack = (1.+z*z)/(1.-z);
double den = (1.-xbar)*sqrt(xbar*xbar - 4.*d_rho_);
return brack/den;
}
pair<Energy,ShowerInteraction::Type>
MEee2gZ2qq::generateHard(RealEmissionProcessPtr born,
vector<Lorentz5Momentum> & emmision,
unsigned int & iemit, unsigned int & ispect,
bool applyVeto,ShowerInteraction::Type inter) {
vector<ShowerInteraction::Type> interactions;
if(inter==ShowerInteraction::Both) {
interactions.push_back(ShowerInteraction::QED);
interactions.push_back(ShowerInteraction::QCD);
}
else
interactions.push_back(inter);
// incoming particles
tPPtr em = born->bornIncoming()[0];
tPPtr ep = born->bornIncoming()[1];
if(em->id()<0) swap(em,ep);
// outgoing particles
tPPtr qk = born->bornOutgoing()[0];
tPPtr qb = born->bornOutgoing()[1];
if(qk->id()<0) swap(qk,qb);
// extract the momenta
loMomenta_.clear();
loMomenta_.push_back(em->momentum());
loMomenta_.push_back(ep->momentum());
loMomenta_.push_back(qk->momentum());
loMomenta_.push_back(qb->momentum());
// and ParticleData objects
partons_.resize(5);
partons_[0]=em->dataPtr();
partons_[1]=ep->dataPtr();
partons_[2]=qk->dataPtr();
partons_[3]=qb->dataPtr();
partons_[4]=cPDPtr();
// boost from lab to CMS frame with outgoing particles
// along the z axis
LorentzRotation eventFrame( ( loMomenta_[2] + loMomenta_[3] ).findBoostToCM() );
Lorentz5Momentum spectator = eventFrame*loMomenta_[2];
eventFrame.rotateZ( -spectator.phi() );
eventFrame.rotateY( -spectator.theta() );
eventFrame.invert();
// mass of the final-state system
Energy2 M2 = (loMomenta_[2]+loMomenta_[3]).m2();
Energy M = sqrt(M2);
double mu1 = loMomenta_[2].mass()/M;
double mu2 = loMomenta_[3].mass()/M;
double mu12 = sqr(mu1), mu22 = sqr(mu2);
double lambda = sqrt(1.+sqr(mu12)+sqr(mu22)-2.*mu12-2.*mu22-2.*mu12*mu22);
// max pT
Energy pTmax = 0.5*sqrt(M2)*
(1.-sqr(loMomenta_[2].mass()+loMomenta_[3].mass())/M2);
// max y
if ( pTmax < pTminQED_ && pTmax < pTminQCD_ ) return make_pair(ZERO,ShowerInteraction::QCD);
vector<Energy> pTemit;
vector<vector<Lorentz5Momentum> > emittedMomenta;;
vector<unsigned int> iemitter,ispectator;
for(unsigned int iinter=0;iinter<interactions.size();++iinter) {
Energy pTmin(ZERO);
double a,ymax;
if(interactions[iinter]==ShowerInteraction::QCD) {
pTmin = pTminQCD_;
ymax = acosh(pTmax/pTmin);
partons_[4] = gluon_;
// prefactor for the overestimate of the Sudakov
a = 4./3.*alphaQCD_->overestimateValue()/Constants::twopi*
2.*ymax*preFactor_;
}
else {
pTmin = pTminQED_;
ymax = acosh(pTmax/pTmin);
partons_[4] = gamma_;
a = alphaQED_->overestimateValue()/Constants::twopi*
2.*ymax*preFactor_*sqr(double(mePartonData()[2]->iCharge())/3.);
}
// variables for the emission
Energy pT[2];
double y[2],phi[2],x3[2],x1[2][2],x2[2][2];
double contrib[2][2];
// storage of the real emission momenta
vector<Lorentz5Momentum> realMomenta[2][2]=
{{vector<Lorentz5Momentum>(5),vector<Lorentz5Momentum>(5)},
{vector<Lorentz5Momentum>(5),vector<Lorentz5Momentum>(5)}};
for(unsigned int ix=0;ix<2;++ix)
for(unsigned int iy=0;iy<2;++iy)
for(unsigned int iz=0;iz<2;++iz)
realMomenta[ix][iy][iz] = loMomenta_[iz];
// generate the emission
for(unsigned int ix=0;ix<2;++ix) {
if(ix==1) {
swap(mu1 ,mu2 );
swap(mu12,mu22);
}
pT[ix] = pTmax;
y [ix] = 0.;
bool reject = true;
do {
// generate pT
pT[ix] *= pow(UseRandom::rnd(),1./a);
if(pT[ix]<pTmin) {
pT[ix] = -GeV;
break;
}
// generate y
y[ix] = -ymax+2.*UseRandom::rnd()*ymax;
// generate phi
phi[ix] = UseRandom::rnd()*Constants::twopi;
// calculate x3 and check in allowed region
x3[ix] = 2.*pT[ix]*cosh(y[ix])/M;
if(x3[ix] < 0. || x3[ix] > 1. -sqr( mu1 + mu2 ) ) continue;
// find the possible solutions for x1
double xT2 = sqr(2./M*pT[ix]);
double root = (-sqr(x3[ix])+xT2)*
(xT2*mu22+2.*x3[ix]-sqr(mu12)+2.*mu22+2.*mu12-sqr(x3[ix])-1.
+2.*mu12*mu22-sqr(mu22)-2.*mu22*x3[ix]-2.*mu12*x3[ix]);
double c1=2.*sqr(x3[ix])-4.*mu22-6.*x3[ix]+4.*mu12-xT2*x3[ix]
+2.*xT2-2.*mu12*x3[ix]+2.*mu22*x3[ix]+4.;
if(root<0.) continue;
x1[ix][0] = 1./(4.-4.*x3[ix]+xT2)*(c1-2.*sqrt(root));
x1[ix][1] = 1./(4.-4.*x3[ix]+xT2)*(c1+2.*sqrt(root));
// change sign of y if 2nd particle emits
if(ix==1) y[ix] *=-1.;
// loop over the solutions
for(unsigned int iy=0;iy<2;++iy) {
contrib[ix][iy]=0.;
// check x1 value allowed
if(x1[ix][iy]<2.*mu1||x1[ix][iy]>1.+mu12-mu22) continue;
// calculate x2 value and check allowed
x2[ix][iy] = 2.-x3[ix]-x1[ix][iy];
double root = max(0.,sqr(x1[ix][iy])-4.*mu12);
root = sqrt(root);
double x2min = 1.+mu22-mu12
-0.5*(1.-x1[ix][iy]+mu12-mu22)/(1.-x1[ix][iy]+mu12)*(x1[ix][iy]-2.*mu12+root);
double x2max = 1.+mu22-mu12
-0.5*(1.-x1[ix][iy]+mu12-mu22)/(1.-x1[ix][iy]+mu12)*(x1[ix][iy]-2.*mu12-root);
if(x2[ix][iy]<x2min||x2[ix][iy]>x2max) continue;
// check the z components
double z1 = sqrt(sqr(x1[ix][iy])-4.*mu12-xT2);
double z2 = -sqrt(sqr(x2[ix][iy])-4.*mu22);
double z3 = pT[ix]*sinh(y[ix])*2./M;
if(ix==1) z3 *=-1.;
if(abs(-z1+z2+z3)<1e-9) z1 *= -1.;
if(abs(z1+z2+z3)>1e-5) continue;
// if using as an ME correction the veto
if(applyVeto) {
double xb = x1[ix][iy], xc = x2[ix][iy];
double b = mu12, c = mu22;
double r = 0.5*(1.+b/(1.+c-xc));
double z1 = r + (xb-(2.-xc)*r)/sqrt(sqr(xc)-4.*c);
double kt1 = (1.-b+c-xc)/z1/(1.-z1);
r = 0.5*(1.+c/(1.+b-xb));
double z2 = r + (xc-(2.-xb)*r)/sqrt(sqr(xb)-4.*b);
double kt2 = (1.-c+b-xb)/z2/(1.-z2);
if(ix==1) {
swap(z1 ,z2);
swap(kt1,kt2);
}
// veto the shower region
if( kt1 < d_kt1_ || kt2 < d_kt2_ ) continue;
}
// construct the momenta
realMomenta[ix][iy][4] =
Lorentz5Momentum(pT[ix]*cos(phi[ix]),pT[ix]*sin(phi[ix]),
pT[ix]*sinh(y[ix]) ,pT[ix]*cosh(y[ix]),ZERO);
if(ix==0) {
realMomenta[ix][iy][2] =
Lorentz5Momentum(-pT[ix]*cos(phi[ix]),-pT[ix]*sin(phi[ix]),
z1*0.5*M,x1[ix][iy]*0.5*M,M*mu1);
realMomenta[ix][iy][3] =
Lorentz5Momentum(ZERO,ZERO, z2*0.5*M,x2[ix][iy]*0.5*M,M*mu2);
}
else {
realMomenta[ix][iy][2] =
Lorentz5Momentum(ZERO,ZERO,-z2*0.5*M,x2[ix][iy]*0.5*M,M*mu2);
realMomenta[ix][iy][3] =
Lorentz5Momentum(-pT[ix]*cos(phi[ix]),-pT[ix]*sin(phi[ix]),
-z1*0.5*M,x1[ix][iy]*0.5*M,M*mu1);
}
// boost the momenta back to the lab
for(unsigned int iz=2;iz<5;++iz)
realMomenta[ix][iy][iz] *= eventFrame;
// jacobian and prefactors for the weight
Energy J = M/sqrt(xT2)*abs(-x1[ix][iy]*x2[ix][iy]+2.*mu22*x1[ix][iy]
+x2[ix][iy]+x2[ix][iy]*mu12+mu22*x2[ix][iy]
-sqr(x2[ix][iy]))
/pow(sqr(x2[ix][iy])-4.*mu22,1.5);
// prefactors etc
contrib[ix][iy] = 0.5*pT[ix]/J/preFactor_/lambda;
// matrix element piece
contrib[ix][iy] *= meRatio(partons_,realMomenta[ix][iy],
ix,interactions[iinter],false);
// coupling piece
if(interactions[iinter]==ShowerInteraction::QCD)
contrib[ix][iy] *= alphaQCD_->ratio(sqr(pT[ix]));
else
contrib[ix][iy] *= alphaQED_->ratio(sqr(pT[ix]));
}
if(contrib[ix][0]+contrib[ix][1]>1.) {
ostringstream s;
s << "MEee2gZ2qq::generateHardest weight for channel " << ix
<< "is " << contrib[ix][0]+contrib[ix][1]
<< " which is greater than 1";
generator()->logWarning( Exception(s.str(), Exception::warning) );
}
reject = UseRandom::rnd() > contrib[ix][0] + contrib[ix][1];
}
while (reject);
if(pT[ix]<pTmin)
pT[ix] = -GeV;
}
// pt of emission
if(pT[0]<ZERO && pT[1]<ZERO) {
pTemit.push_back(-GeV);
emittedMomenta.push_back(vector<Lorentz5Momentum>());
iemitter .push_back(0);
ispectator.push_back(0);
continue;
}
// now pick the emission with highest pT
vector<Lorentz5Momentum> emission;
if(pT[0]>pT[1]) {
iemitter .push_back(2);
ispectator.push_back(3);
pTemit.push_back(pT[0]);
if(UseRandom::rnd()<contrib[0][0]/(contrib[0][0]+contrib[0][1]))
emission = realMomenta[0][0];
else
emission = realMomenta[0][1];
}
else {
iemitter .push_back(3);
ispectator.push_back(2);
pTemit.push_back(pT[1]);
if(UseRandom::rnd()<contrib[1][0]/(contrib[1][0]+contrib[1][1]))
emission = realMomenta[1][0];
else
emission = realMomenta[1][1];
}
emittedMomenta.push_back(emission);
}
// select the type of emission
int iselect=-1;
pTmax = ZERO;
for(unsigned int ix=0;ix<interactions.size();++ix) {
if(pTemit[ix]>pTmax) {
iselect = ix;
pTmax = pTemit[ix];
}
}
// no emission return
if(iselect<0) {
return make_pair(ZERO,ShowerInteraction::QCD);
}
partons_[4] = interactions[iselect]==ShowerInteraction::QCD ? gluon_ : gamma_;
iemit = iemitter[iselect];
ispect = ispectator[iselect];
emmision = emittedMomenta[iselect];
// return pT of emission
return make_pair(pTmax,interactions[iselect]);
}
RealEmissionProcessPtr MEee2gZ2qq::generateHardest(RealEmissionProcessPtr born,
ShowerInteraction::Type inter) {
return calculateRealEmission(born,false,inter);
}
double MEee2gZ2qq::meRatio(vector<cPDPtr> partons,
vector<Lorentz5Momentum> momenta,
unsigned int iemitter,
ShowerInteraction::Type inter,
bool subtract) const {
Lorentz5Momentum q = momenta[2]+momenta[3]+momenta[4];
Energy2 Q2=q.m2();
Energy2 lambda = sqrt((Q2-sqr(momenta[2].mass()+momenta[3].mass()))*
(Q2-sqr(momenta[2].mass()-momenta[3].mass())));
InvEnergy2 D[2];
double lome[2];
for(unsigned int iemit=0;iemit<2;++iemit) {
unsigned int ispect = iemit==0 ? 1 : 0;
Energy2 pipj = momenta[4 ] * momenta[2+iemit ];
Energy2 pipk = momenta[4 ] * momenta[2+ispect];
Energy2 pjpk = momenta[2+iemit] * momenta[2+ispect];
double y = pipj/(pipj+pipk+pjpk);
double z = pipk/( pipk+pjpk);
Energy mij = sqrt(2.*pipj+sqr(momenta[2+iemit].mass()));
Energy2 lamB = sqrt((Q2-sqr(mij+momenta[2+ispect].mass()))*
(Q2-sqr(mij-momenta[2+ispect].mass())));
Energy2 Qpk = q*momenta[2+ispect];
Lorentz5Momentum pkt =
lambda/lamB*(momenta[2+ispect]-Qpk/Q2*q)
+0.5/Q2*(Q2+sqr(momenta[2+ispect].mass())-sqr(momenta[2+ispect].mass()))*q;
Lorentz5Momentum pijt =
q-pkt;
double muj = momenta[2+iemit ].mass()/sqrt(Q2);
double muk = momenta[2+ispect].mass()/sqrt(Q2);
double vt = sqrt((1.-sqr(muj+muk))*(1.-sqr(muj-muk)))/(1.-sqr(muj)-sqr(muk));
double v = sqr(2.*sqr(muk)+(1.-sqr(muj)-sqr(muk))*(1.-y))-4.*sqr(muk);
if(v<=0.) return 0.;
v = sqrt(v)/(1.-y)/(1.-sqr(muj)-sqr(muk));
// dipole term
D[iemit] = 0.5/pipj*(2./(1.-(1.-z)*(1.-y))
-vt/v*(2.-z+sqr(momenta[2+iemit].mass())/pipj));
// matrix element
vector<Lorentz5Momentum> lomom(4);
lomom[0] = momenta[0];
lomom[1] = momenta[1];
if(iemit==0) {
lomom[2] = pijt;
lomom[3] = pkt ;
}
else {
lomom[3] = pijt;
lomom[2] = pkt ;
}
lome[iemit] = loME(partons,lomom,false)/3.;
}
InvEnergy2 ratio = realME(partons,momenta,inter)
*abs(D[iemitter])/(abs(D[0]*lome[0])+abs(D[1]*lome[1]));
double output = Q2*ratio;
if(subtract) output -= 2.*Q2*D[iemitter];
return output;
}
double MEee2gZ2qq::loME(const vector<cPDPtr> & partons,
const vector<Lorentz5Momentum> & momenta,
bool first) const {
// compute the spinors
vector<SpinorWaveFunction> fin,aout;
vector<SpinorBarWaveFunction> ain,fout;
SpinorWaveFunction ein (momenta[0],partons[0],incoming);
SpinorBarWaveFunction pin (momenta[1],partons[1],incoming);
SpinorBarWaveFunction qkout(momenta[2],partons[2],outgoing);
SpinorWaveFunction qbout(momenta[3],partons[3],outgoing);
for(unsigned int ix=0;ix<2;++ix) {
ein.reset(ix) ;
fin.push_back( ein );
pin.reset(ix) ;
ain.push_back( pin );
qkout.reset(ix);
fout.push_back(qkout);
qbout.reset(ix);
aout.push_back(qbout);
}
// compute the matrix element
double me,lastCont,lastBW;
HelicityME(fin,ain,fout,aout,me,lastCont,lastBW);
// save the components
if(first) {
DVector save;
save.push_back(lastCont);
save.push_back(lastBW);
meInfo(save);
}
// return the answer
return me;
}
InvEnergy2 MEee2gZ2qq::realME(const vector<cPDPtr> & partons,
const vector<Lorentz5Momentum> & momenta,
ShowerInteraction::Type inter) const {
// compute the spinors
vector<SpinorWaveFunction> fin,aout;
vector<SpinorBarWaveFunction> ain,fout;
vector<VectorWaveFunction> gout;
SpinorWaveFunction ein (momenta[0],partons[0],incoming);
SpinorBarWaveFunction pin (momenta[1],partons[1],incoming);
SpinorBarWaveFunction qkout(momenta[2],partons[2],outgoing);
SpinorWaveFunction qbout(momenta[3],partons[3],outgoing);
VectorWaveFunction gluon(momenta[4],partons[4],outgoing);
for(unsigned int ix=0;ix<2;++ix) {
ein.reset(ix) ;
fin.push_back( ein );
pin.reset(ix) ;
ain.push_back( pin );
qkout.reset(ix);
fout.push_back(qkout);
qbout.reset(ix);
aout.push_back(qbout);
gluon.reset(2*ix);
gout.push_back(gluon);
}
AbstractFFVVertexPtr vertex = inter == ShowerInteraction::QCD ?
FFGVertex_ : FFPVertex_;
vector<Complex> diag(4,0.);
ProductionMatrixElement output(PDT::Spin1Half,PDT::Spin1Half,
PDT::Spin1Half,PDT::Spin1Half,
PDT::Spin1);
double total(0.);
for(unsigned int inhel1=0;inhel1<2;++inhel1) {
for(unsigned int inhel2=0;inhel2<2;++inhel2) {
// intermediate Z
VectorWaveFunction interZ =
FFZVertex_->evaluate(scale(),1,Z0_,fin[inhel1],ain[inhel2]);
// intermediate photon
VectorWaveFunction interG =
FFPVertex_->evaluate(scale(),1,gamma_,fin[inhel1],ain[inhel2]);
for(unsigned int outhel1=0;outhel1<2;++outhel1) {
for(unsigned int outhel2=0;outhel2<2;++outhel2) {
for(unsigned int outhel3=0;outhel3<2;++outhel3) {
SpinorBarWaveFunction off1 =
vertex->evaluate(scale(),3,partons[2],fout[outhel1],gout[outhel3]);
diag[0] = FFZVertex_->evaluate(scale(),aout[outhel2],off1,interZ);
diag[1] = FFPVertex_->evaluate(scale(),aout[outhel2],off1,interG);
SpinorWaveFunction off2 =
vertex->evaluate(scale(),3,partons[3],aout[outhel2],gout[outhel3]);
diag[2] = FFZVertex_->evaluate(scale(),off2,fout[outhel1],interZ);
diag[3] = FFPVertex_->evaluate(scale(),off2,fout[outhel1],interG);
// sum of diagrams
Complex sum = std::accumulate(diag.begin(),diag.end(),Complex(0.));
// matrix element
output(inhel1,inhel2,outhel1,outhel2,outhel3)=sum;
// me2
total += norm(sum);
}
}
}
}
}
// spin average
total *= 0.25;
tcPolarizedBeamPDPtr beam[2] =
{dynamic_ptr_cast<tcPolarizedBeamPDPtr>(partons[0]),
dynamic_ptr_cast<tcPolarizedBeamPDPtr>(partons[1])};
if( beam[0] || beam[1] ) {
RhoDMatrix rho[2] =
{beam[0] ? beam[0]->rhoMatrix() : RhoDMatrix(mePartonData()[0]->iSpin()),
beam[1] ? beam[1]->rhoMatrix() : RhoDMatrix(mePartonData()[1]->iSpin())};
total = output.average(rho[0],rho[1]);
}
// divide out the coupling
total /= norm(vertex->norm());
// and charge (if needed)
if(inter==ShowerInteraction::QED)
total /= sqr(double(mePartonData()[2]->iCharge())/3.);
// return the total
return total*UnitRemoval::InvE2;
}
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