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diff --git a/Hadronization/DynamicClusterFissioner.cc b/Hadronization/DynamicClusterFissioner.cc
--- a/Hadronization/DynamicClusterFissioner.cc
+++ b/Hadronization/DynamicClusterFissioner.cc
@@ -1,412 +1,404 @@
// -*- C++ -*-
//
// ClusterFissioner.cc is a part of Herwig - A multi-purpose Monte Carlo event generator
// Copyright (C) 2002-2019 The Herwig Collaboration
//
// Herwig is licenced under version 3 of the GPL, see COPYING for details.
// Please respect the MCnet academic guidelines, see GUIDELINES for details.
//
//
// Thisk is the implementation of the non-inlined, non-templated member
// functions of the ClusterFissioner class.
//
#include "DynamicClusterFissioner.h"
#include <ThePEG/Interface/ClassDocumentation.h>
#include <ThePEG/Interface/Reference.h>
#include <ThePEG/Interface/Parameter.h>
#include <ThePEG/Interface/Switch.h>
#include <ThePEG/Persistency/PersistentOStream.h>
#include <ThePEG/Persistency/PersistentIStream.h>
#include <ThePEG/PDT/EnumParticles.h>
#include "Herwig/Utilities/Kinematics.h"
#include "ThePEG/Repository/UseRandom.h"
#include "ThePEG/Repository/EventGenerator.h"
#include <ThePEG/Utilities/DescribeClass.h>
using namespace Herwig;
DescribeClass<DynamicClusterFissioner,ClusterFissioner>
describeDynamicClusterFissioner("Herwig::DynamicClusterFissioner","Herwig.so");
DynamicClusterFissioner::DynamicClusterFissioner() :
_Qqtilde(4*GeV),
_Qg2tilde(4*GeV),
_AngOrdFission(1),
_restrictGluon(1)
{}
IBPtr DynamicClusterFissioner::clone() const {
return new_ptr(*this);
}
IBPtr DynamicClusterFissioner::fullclone() const {
return new_ptr(*this);
}
void DynamicClusterFissioner::persistentOutput(PersistentOStream & os) const {
os << _AngOrdFission << _restrictGluon << ounit(_Qqtilde,GeV) << ounit(_Qg2tilde,GeV) << _dynamicGluonMassGenerator << _dynamicPartonSplitter;
}
void DynamicClusterFissioner::persistentInput(PersistentIStream & is, int) {
is >> _AngOrdFission >> _restrictGluon >> iunit(_Qqtilde,GeV) >> iunit(_Qg2tilde,GeV) >> _dynamicGluonMassGenerator >> _dynamicPartonSplitter;
}
void DynamicClusterFissioner::Init() {
static Parameter<DynamicClusterFissioner,Energy> interfaceQqtilde
("Qqtilde",
"Scale of the non-pert. quark splitting in the cluster fission",
&DynamicClusterFissioner::_Qqtilde, GeV, 4.0*GeV, 1.5*GeV, 10000.0*GeV,false,false,false); //Set upper/lower bound and default later
static Parameter<DynamicClusterFissioner,Energy> interfaceQg2tilde
("Qg2tilde",
"Upper scale for the Sudakov for the non-pert. gluon splitting in the cluster fission",
&DynamicClusterFissioner::_Qg2tilde, GeV, 4.0*GeV, 0.5*GeV, 10000.0*GeV,false,false,false); //Set upper/lower bound and default later
static Switch<DynamicClusterFissioner,int> interfaceAngOrdFission
("AngularOrderedFission",
"Option to switch on angular ordering in the dynamic fission model",
&DynamicClusterFissioner::_AngOrdFission,0,false,false);
static SwitchOption interfaceAngOrdFissionNo
(interfaceAngOrdFission,
"No",
"No (Qqtilde and Qg2tilde independent)",
0);
static SwitchOption interfaceAngOrdFissionYes
(interfaceAngOrdFission,
"Yes",
"Qg2tilde=(1-z)*Qqtilde",
1);
static Switch<DynamicClusterFissioner,int> interfacerestrictGluon
("restrictGluon",
"Option to restrict the gluon virtuality in the dynamic fission in order to make sure that the splitting works out kinematically",
&DynamicClusterFissioner::_restrictGluon,0,false,false);
static SwitchOption interfacerestrictGluonNo
(interfacerestrictGluon,
"No",
"Gluon can have virtuality up to Qg2tilde. Might be necessary to start fission again with new z and qtilde for the quark",
0);
static SwitchOption interfacerestrictGluonYes
(interfacerestrictGluon,
"Yes",
"Gluon virtuality is restricted to the range that the kinematics allow once that z and qitlde are fixed for the quark",
1);
static Reference<DynamicClusterFissioner,DynamicGluonMassGenerator> interfaceDynamicGluonMassGenerator
("GluonMassGenerator",
"Set a reference to a gluon mass generator.",
&DynamicClusterFissioner::_dynamicGluonMassGenerator, false, false, true, true, false);
static Reference<DynamicClusterFissioner,DynamicPartonSplitter> interfaceDynamicPartonSplitter
("PartonSplitter",
"Set a reference to a parton splitter",
&DynamicClusterFissioner::_dynamicPartonSplitter, false, false, true, true, false);
}
InvEnergy DynamicClusterFissioner::Pqzproposal(double z,Energy qtilde, Energy Qqtilde, Energy mq) const{
return _dynamicGluonMassGenerator->ClusterAlphaS(0.*GeV2)*2.*(1.-sqr(mq/Qqtilde))/(qtilde*(1.-z));
}
InvEnergy DynamicClusterFissioner::Pqz(double z, Energy qtilde, Energy mq) const {
if ( z*qtilde > mq){
return _dynamicGluonMassGenerator->ClusterAlphaS(sqr(z*(1.0-z)*qtilde))*( (1.+z*z)/(1.-z) - ((2.*sqr(mq))/( z*(1.-z)*sqr(qtilde) )))/qtilde;}
else {
return 0./(1.*GeV);
}
}
void DynamicClusterFissioner::dynamicFission(tPPtr ptrP, tPPtr ptrPbar, PPtr& ptrQ, PPtr& ptrQbar) const {
LorentzMomentum P1, P2;
bool fromcolor;
Energy mq2, mg, MP1, Qqtilde, Qgtilde, qtilde, mq;
double z;
//minimal quark mass
Energy m0, mu, ms, md;
mu=getParticleData(ThePEG::ParticleID::u)->constituentMass();
md=getParticleData(ThePEG::ParticleID::d)->constituentMass();
ms=getParticleData(ThePEG::ParticleID::s)->constituentMass();
m0=md;
if(mu<m0){m0=mu;}
if(ms<m0){m0=ms;}
bool repeat2=true;
LorentzMomentum Pcl(ptrP->momentum()+ptrPbar->momentum());
Energy Mcl = Pcl.m();
//boost to rest frame of the cluster
Boost bv = Pcl.boostVector();
//upper scale of the quark splitting
Qqtilde = _Qqtilde;
while(repeat2){
//choose from which constituent we radiate the gluon
if ( UseRandom::rnd(0.0, 1.0)<0.5 ){
P1 = ptrP->momentum();
P2 = ptrPbar->momentum();
mq = ptrP->data().constituentMass();
mq2 = ptrPbar->data().constituentMass();
fromcolor=true;
}
else{
P2 = ptrP->momentum();
P1 = ptrPbar->momentum();
mq = ptrPbar->data().constituentMass();
mq2 = ptrP->data().constituentMass();
fromcolor=false;
}
//and check if it is kinematically possible for that constituent
if (!canSplitMinimally(Mcl,mq,mq2,m0)){
swap(P1,P2);
swap(mq,mq2);
fromcolor=(!fromcolor);
}
P1.boost(-bv);
P2.boost(-bv);
//Qqtilde = Qqtilde + mq;
//get z and qtilde
double zmin=mq/Qqtilde;
double zmax=1-(4*sqr(m0)/( sqr(Mcl-mq2)-sqr(mq) ));
//if ((_AngOrdFission==1) && (1-(4*m0/Qqtilde)<zmax)){
// zmax=1-(4*m0/Qqtilde);
// }
double rzmin=-log(1-zmin);
double rzmax=-log(1-zmax);
bool repeat = true;
while (repeat){
//generate z and qtilde from a proposal distribution and check that at least with minimal quark mass the kinematics can work out
bool repeat3 = true;
double ymin, ymax;
while (repeat3){
z = 1.0 - exp(-UseRandom::rnd(rzmin,rzmax));
ymin =mq/(z*Qqtilde);
if ((_AngOrdFission==1)&&(4*m0/((1.-z)*Qqtilde)>ymin)){
ymin=4*m0/((1.-z)*Qqtilde);
}
ymax =sqrt( ( sqr(Mcl-mq2) -sqr(mq) -(4*sqr(m0)/(1-z)) )/( z*(1-z) ) )/Qqtilde;
if (ymax >1.){
ymax=1.;
}
if (ymin<ymax){
repeat3=false;
}
}
double rymin=-log(ymax);
double rymax=-log(ymin);
qtilde=Qqtilde*exp(-UseRandom::rnd(rymin,rymax));
//compare with actual distrubition
if (Pqzproposal(z,qtilde,Qqtilde,mq)*UseRandom::rnd(0.0,1.0)<Pqz(z,qtilde,mq)){
repeat = false;
}
}
//scale for the Sudakov in the gluon splitting
if (_AngOrdFission==1){
Qgtilde=(1.-z)*qtilde;
}
else{
Qgtilde=_Qg2tilde;
}
//gluon virtuality
if (_restrictGluon==1){
//restirct the gluon virtuality to the range where kinematic reconstruction is possible, i.e. Mcl>MP1+mq2 is always true
Energy mgmax=sqrt((1.-z)*(sqr(Mcl-mq2) - sqr(mq) -z*(1.-z)*sqr(qtilde)));
mg=_dynamicGluonMassGenerator->generate(Qgtilde,mgmax);
}
else{
//no additional restriction on gluon virtuality. Mcl>MP1+mq2 might fail and new z and qtilde for the quark are generated
mg=_dynamicGluonMassGenerator->generate(Qgtilde);
}
//kinematic reconstruction / get momenta P1prime and P2prime before radiating
//invariant mass of quark before radiating
MP1 = sqrt(sqr(mq)+z*(1.0-z)*sqr(qtilde)+(sqr(mg)/(1.-z)));
if(Mcl>MP1+mq2){
repeat2 = false;
}
}//end while(repeat2)
Energy absP = sqrt(sqr(sqr(Mcl))+sqr(sqr(MP1))+sqr(sqr(mq2))-2.0*(sqr(Mcl*MP1)+sqr(Mcl*mq2)+sqr(MP1*mq2)))/(2.0*Mcl);
Lorentz5Momentum P1prime(absP*P1.vect().unit(),sqrt(sqr(absP)+sqr(MP1)),MP1);
Lorentz5Momentum P2prime(absP*P2.vect().unit(),sqrt(sqr(absP)+sqr(mq2)),mq2);
//splitting
//construct the backwards light-like vector
LorentzVector<double> nbar(-P1prime.vect().unit(),1.0);
//construct the transverse momentum with random azimuthal angle
//construct an orthonormal basis of transverse 4-vectors
ThreeVector<double> Three_qperp1 = nbar.vect().orthogonal().unit();
ThreeVector<double> Three_qperp2 = nbar.vect().unit().cross(Three_qperp1);
LorentzVector<double> qperp1(Three_qperp1,0.0);
LorentzVector<double> qperp2(Three_qperp2,0.0);
using Constants::pi;
double phi = UseRandom::rnd( -pi , pi );
Energy gperpabs=sqrt(sqr(1.-z)*(sqr(z*qtilde)-sqr(mq)) );
LorentzMomentum gperp = gperpabs*cos(phi)*qperp1+gperpabs*sin(phi)*qperp2;
//quark and gluon momenta
Lorentz5Momentum k(z*P1prime + ((sqr(mq)-sqr(z*MP1)+sqr(gperpabs))/(2.0*z*P1prime.dot(nbar)))*nbar - gperp,mq);
Lorentz5Momentum g((1.-z)*P1prime + ((sqr(mg)-sqr((1.-z)*MP1)+sqr(gperpabs))/(2.0*(1.-z)*P1prime.dot(nbar)))*nbar +gperp,mg);
//create particles and give them to PartonSplitter
PPtr ptrPprime = PPtr();
PPtr ptrG = PPtr();
ptrG = getParticle(ThePEG::ParticleID::g);
ptrG->set5Momentum(g);
if (fromcolor){
ptrP->set5Momentum(k);
ptrPbar->set5Momentum(P2prime);
ptrPprime = getParticle(ptrP->id());
ptrPprime->set5Momentum(P1prime);
//_dynamicPartonSplitter->splitTimeLikeGluon(ptrG,ptrPprime,ptrPbar,ptrQ,ptrQbar,Qgtilde,nbar,fromcolor);
_dynamicPartonSplitter->splitTimeLikeGluon(ptrG,ptrQ, ptrQbar, ptrPprime, ptrPbar,Qgtilde,nbar,fromcolor);
}
else{
ptrP->set5Momentum(P2prime);
ptrPbar->set5Momentum(k);
ptrPprime = getParticle(ptrPbar->id());
ptrPprime->set5Momentum(P1prime);
//_dynamicPartonSplitter->splitTimeLikeGluon(ptrG,ptrP,ptrPprime,ptrQ,ptrQbar,Qgtilde,nbar,fromcolor);
_dynamicPartonSplitter->splitTimeLikeGluon(ptrG,ptrQ, ptrQbar, ptrP, ptrPprime,Qgtilde,nbar,fromcolor);
}
//boost back to lab frame
//(this must be possible in a nicer way)
Lorentz5Momentum temp;
temp = ptrP->momentum();
temp.boost(bv);
ptrP->set5Momentum(temp);
temp = ptrPbar->momentum();
temp.boost(bv);
ptrPbar->set5Momentum(temp);
temp = ptrQ->momentum();
temp.boost(bv);
ptrQ->set5Momentum(temp);
temp = ptrQbar->momentum();
temp.boost(bv);
ptrQbar->set5Momentum(temp);
-
- Lorentz5Momentum clu1mom = ptrP->momentum()+ptrQbar->momentum();
- Lorentz5Momentum clu2mom = ptrPbar->momentum()+ptrQ->momentum();
- Energy clu1mass = clu1mom.m();
- Energy clu2mass = clu2mom.m();
-if (Mcl/(1.*GeV) < 91.2001 && Mcl/(1.*GeV) > 91.1999){
- std::cout << clu1mass/(1.*GeV) << " " << clu2mass/(1.*GeV) << std::endl;
-}
}
bool DynamicClusterFissioner::canSplitMinimally(Energy Mcl, Energy m1, Energy m2, Energy m0) const {
if (Mcl<m1+m2+2*m0){ return false; }
Energy Qtilde=_Qqtilde;
if (Qtilde>m1){
if (_AngOrdFission==0){
if (Qtilde>2*m0+m1){
return Mcl>m2+m1+2*m0;
}
else{
return Mcl>m2+sqrt(Qtilde*(m1- (4*sqr(m0)/(Qtilde-m1)) ));
}
}
else{
if (Qtilde>4*m0+m1){
return Mcl>m2+sqrt((m0+m1)*(4*m0+m1));
}
else{
return Mcl<m2+sqrt( sqr(m1) + (4*sqr(m0)*(4*m1+Qtilde))/(Qtilde-m1) );
}
}
}
else{
return false;
}
}
bool DynamicClusterFissioner::canSplitMinimally(tcClusterPtr clu, Energy minmass) const {
Energy Mcl=clu->mass();
Energy m1 = clu->particle(0)->data().constituentMass();
Energy m2 = clu->particle(1)->data().constituentMass();
return ((canSplitMinimally(Mcl,m1,m2,minmass))||(canSplitMinimally(Mcl,m2,m1,minmass)));
}

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