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This commit is contained in:
Gabriele Cosmo
2016-06-09 10:28:22 +02:00
parent fbd4999cf7
commit 4aea781e80
5454 changed files with 223141 additions and 67347 deletions
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source/processes/hadronic/models/cascade/cascade/include/G4Analyser.hh
+3 -3
View File
@@ -31,7 +31,7 @@
#include "G4NuclWatcher.hh"
//#include "G4ExitonConfiguration.hh"
#include "g4std/vector"
#include <vector>
class G4Analyser {
@@ -40,7 +40,7 @@ public:
G4Analyser();
void setInelCsec(G4double csec,
G4bool withn);
void setWatchers(const G4std::vector<G4NuclWatcher>& watchers);
void setWatchers(const std::vector<G4NuclWatcher>& watchers);
void try_watchers(G4double a,
G4double z,
G4bool if_nucl);
@@ -70,7 +70,7 @@ private:
G4double averagePion0;
G4double averageA;
G4double averageZ;
G4std::vector<G4NuclWatcher> ana_watchers;
std::vector<G4NuclWatcher> ana_watchers;
G4double inel_csec;
G4bool withNuclei;
};
source/processes/hadronic/models/cascade/cascade/include/G4BertiniNucleiModel.hh
+13 -13
View File
@@ -30,15 +30,15 @@
#include "G4CascadSpecialFunctions.hh"
#include "G4ElementaryParticleCollider.hh"
#include "g4std/vector"
#include <vector>
class G4InuclNuclei;
using namespace G4InuclSpecialFunctions;
using namespace G4CascadSpecialFunctions;
typedef G4std::pair<G4InuclElementaryParticle, G4double> partner;
typedef G4std::vector<partner> partners;
typedef std::pair<G4InuclElementaryParticle, G4double> partner;
typedef std::vector<partner> partners;
class G4BertiniNucleiModel {
@@ -135,7 +135,7 @@ public:
return izone < number_of_zones ? zone_potentials[ip0][izone] : 0.0;
};
G4std::vector<G4CascadParticle>
std::vector<G4CascadParticle>
generateParticleFate(G4CascadParticle& cparticle,
G4ElementaryParticleCollider* theElementaryParticleCollider);
@@ -161,16 +161,16 @@ public:
G4CascadParticle initializeCascad(G4InuclElementaryParticle* particle);
G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> > initializeCascad(G4InuclNuclei* bullet, G4InuclNuclei* target);
std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> > initializeCascad(G4InuclNuclei* bullet, G4InuclNuclei* target);
G4std::pair<G4int, G4int> getTypesOfNucleonsInvolved() const {
return G4std::pair<G4int, G4int>(current_nucl1, current_nucl2);
std::pair<G4int, G4int> getTypesOfNucleonsInvolved() const {
return std::pair<G4int, G4int>(current_nucl1, current_nucl2);
};
G4bool worthToPropagate(const G4CascadParticle& cparticle) const;
private:
G4int verboseLevel; /*!< Each class has a verbosity level of its own. */
G4bool passFermi(const G4std::vector<G4InuclElementaryParticle>& particles,
G4bool passFermi(const std::vector<G4InuclElementaryParticle>& particles,
G4int zone);
void boundaryTransition(G4CascadParticle& cparticle);
@@ -195,15 +195,15 @@ private:
G4double getRatio(G4int ip) const;
G4std::vector<G4std::vector<G4double> > nucleon_densities;
std::vector<std::vector<G4double> > nucleon_densities;
G4std::vector<G4std::vector<G4double> > zone_potentials;
std::vector<std::vector<G4double> > zone_potentials;
G4std::vector<G4std::vector<G4double> > fermi_momenta;
std::vector<std::vector<G4double> > fermi_momenta;
G4std::vector<G4double> zone_radii;
std::vector<G4double> zone_radii;
G4std::vector<G4double> binding_energies;
std::vector<G4double> binding_energies;
G4double nuclei_radius;
source/processes/hadronic/models/cascade/cascade/include/G4BertiniRegionModel.hh
-77
View File
@@ -1,77 +0,0 @@
//
// ********************************************************************
// * DISCLAIMER *
// * *
// * The following disclaimer summarizes all the specific disclaimers *
// * of contributors to this software. The specific disclaimers,which *
// * govern, are listed with their locations in: *
// * http://cern.ch/geant4/license *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. *
// * *
// * This code implementation is the intellectual property of the *
// * GEANT4 collaboration. *
// * By copying, distributing or modifying the Program (or any work *
// * based on the Program) you indicate your acceptance of this *
// * statement, and all its terms. *
// ********************************************************************
#ifndef G4BERTINIREGIONMODEL
#define G4BERTINIREGIONMODEL
#include "G4ios.hh"
#include "g4std/vector"
#include <math.h>
#include "globals.hh"
#include "G4Proton.hh"
#include "G4Neutron.hh"
typedef G4std::vector<G4double>::const_iterator iterator;
class G4BertiniRegionModel /// :public G4VRegionModel
{
public:
G4BertiniRegionModel(const G4int numberOfLayers, const G4int A, const G4int Z);
~G4BertiniRegionModel();
/// instead of A and Z outer radius of the nucleus?
/// void Init(const G4int numberOfLayers, const G4int A, const G4int Z);
G4double GetDensity(G4double radius);
G4double GetPotentialEnergy(G4double r, G4int particle);
G4double GetMaximumNucleonMomentum(G4double radius, G4int nucleon);
/// G4double NumberOfRegions();
private:
G4int massNumber;
G4int protonNumber;
G4std::vector<G4double> radius; /// contains the outer radiuses of the shells
G4std::vector<G4double> density;
G4std::vector<G4double> protonFermiEnergy;
G4std::vector<G4double> neutronFermiEnergy;
G4std::vector<G4double> protonFermiMomentum;
G4std::vector<G4double> neutronFermiMomentum;
G4std::vector<G4double> protonPotentialEnergy;
G4std::vector<G4double> neutronPotentialEnergy;
static const G4double radius0;
static const G4double BE;
/// static const G4double pi = 3.141592;
G4double GetFermiMomentum(G4double density, G4double mass);
G4double GetFermiEnergy(G4double density, G4double mass);
};
#endif
source/processes/hadronic/models/cascade/cascade/include/G4BigBanger.hh
+2 -2
View File
@@ -41,13 +41,13 @@ public:
private:
G4int verboseLevel;
G4std::vector<G4InuclElementaryParticle> generateBangInSCM(G4double etot,
std::vector<G4InuclElementaryParticle> generateBangInSCM(G4double etot,
G4double a,
G4double z,
G4double mp,
G4double mn) const;
G4std::vector<G4double> generateMomentumModules(G4double etot,
std::vector<G4double> generateMomentumModules(G4double etot,
G4double a,
G4double z,
G4double mp,
source/processes/hadronic/models/cascade/cascade/include/G4CascadParticle.hh
+6 -6
View File
@@ -31,7 +31,7 @@ public:
G4CascadParticle();
G4CascadParticle(const G4InuclElementaryParticle& particle,
const G4std::vector<G4double>& pos,
const std::vector<G4double>& pos,
G4int izone,
G4double cpath)
@@ -44,11 +44,11 @@ public:
reflectionCounter = 0;
};
void updateParticleMomentum(const G4std::vector<G4double>& mom) {
void updateParticleMomentum(const std::vector<G4double>& mom) {
theParticle.setMomentum(mom);
};
void updatePosition(const G4std::vector<G4double>& pos) {
void updatePosition(const std::vector<G4double>& pos) {
position = pos;
};
@@ -76,7 +76,7 @@ public:
G4double getPathToTheNextZone(G4double rz_in,
G4double rz_out);
G4std::vector<G4double> getMomentum() const {
std::vector<G4double> getMomentum() const {
return theParticle.getMomentum();
};
@@ -84,7 +84,7 @@ public:
return theParticle;
};
G4std::vector<G4double> getPosition() const {
std::vector<G4double> getPosition() const {
return position;
};
@@ -126,7 +126,7 @@ private:
G4int verboseLevel;
G4InuclElementaryParticle theParticle;
G4std::vector<G4double> position;
std::vector<G4double> position;
G4int current_zone;
G4double current_path;
G4bool movingIn;
source/processes/hadronic/models/cascade/cascade/include/G4CascadSpecialFunctions.hh
+5 -5
View File
@@ -25,14 +25,14 @@
#include "globals.hh"
#include <math.h>
#include "g4std/algorithm"
#include "g4std/vector"
#include <algorithm>
#include <vector>
namespace G4CascadSpecialFunctions {
G4std::pair<G4int, G4double> getPositionInEnergyScale2(G4double e);
std::pair<G4int, G4double> getPositionInEnergyScale2(G4double e);
G4std::pair<G4int, G4double> getPositionInEnergyScale1(G4double e);
std::pair<G4int, G4double> getPositionInEnergyScale1(G4double e);
G4double absorptionCrosSection(G4double e,
G4int type);
@@ -40,7 +40,7 @@ namespace G4CascadSpecialFunctions {
G4double crossSection(G4double e,
G4int is);
G4std::pair<G4int, G4double> getPositionInEnergyScaleEMS(G4double e);
std::pair<G4int, G4double> getPositionInEnergyScaleEMS(G4double e);
}
#endif
source/processes/hadronic/models/cascade/cascade/include/G4CollisionOutput.hh
+14 -14
View File
@@ -22,13 +22,13 @@
#ifndef G4COLLISION_OUTPUT_HH
#define G4COLLISION_OUTPUT_HH
#include "g4std/iostream"
#include <iostream>
#include "G4InuclElementaryParticle.hh"
#include "G4InuclNuclei.hh"
#include "g4std/algorithm"
#include "g4std/vector"
#include <algorithm>
#include <vector>
class G4CollisionOutput {
@@ -46,7 +46,7 @@ public:
outgoingParticles.push_back(particle);
};
void addOutgoingParticles(const G4std::vector<G4InuclElementaryParticle>& particles) {
void addOutgoingParticles(const std::vector<G4InuclElementaryParticle>& particles) {
for(G4int i = 0; i < G4int(particles.size()); i++)
outgoingParticles.push_back(particles[i]);
};
@@ -55,12 +55,12 @@ public:
nucleiFragments.push_back(nuclei);
};
void addTargetFragments(const G4std::vector<G4InuclNuclei>& nuclea) {
void addTargetFragments(const std::vector<G4InuclNuclei>& nuclea) {
for(G4int i = 0; i < G4int(nuclea.size()); i++)
nucleiFragments.push_back(nuclea[i]);
};
G4std::vector<G4InuclElementaryParticle> getOutgoingParticles() const {
std::vector<G4InuclElementaryParticle> getOutgoingParticles() const {
return outgoingParticles;
};
@@ -68,20 +68,20 @@ public:
return nucleiFragments.size();
};
G4std::vector<G4InuclNuclei> getNucleiFragments() const {
std::vector<G4InuclNuclei> getNucleiFragments() const {
return nucleiFragments;
};
G4std::vector<G4double> getTotalOutputMomentum() const {
G4std::vector<G4double> tot_mom(4, 0.0);
std::vector<G4double> getTotalOutputMomentum() const {
std::vector<G4double> tot_mom(4, 0.0);
double eex_r = 0.0;
G4int i(0);
for(i = 0; i < G4int(outgoingParticles.size()); i++) {
G4std::vector<G4double> mom = outgoingParticles[i].getMomentum();
std::vector<G4double> mom = outgoingParticles[i].getMomentum();
for(G4int j = 0; j < 4; j++) tot_mom[j] += mom[j];
};
for(i = 0; i < G4int(nucleiFragments.size()); i++) {
G4std::vector<G4double> mom = nucleiFragments[i].getMomentum();
std::vector<G4double> mom = nucleiFragments[i].getMomentum();
for(G4int j = 0; j < 4; j++) tot_mom[j] += mom[j];
eex_r += 0.001 * nucleiFragments[i].getExitationEnergy();
};
@@ -142,13 +142,13 @@ public:
private:
G4int verboseLevel;
G4std::vector<G4InuclElementaryParticle> outgoingParticles;
std::vector<G4InuclElementaryParticle> outgoingParticles;
G4std::vector<G4InuclNuclei> nucleiFragments;
std::vector<G4InuclNuclei> nucleiFragments;
G4double eex_rest;
G4std::pair<G4std::pair<G4int, G4int>, G4int> selectPairToTune(G4double de) const;
std::pair<std::pair<G4int, G4int>, G4int> selectPairToTune(G4double de) const;
G4bool on_shell;
source/processes/hadronic/models/cascade/cascade/include/G4ElementaryParticleCollider.hh
+9 -9
View File
@@ -45,13 +45,13 @@ private:
G4int generateMultiplicity(G4int is,
G4double ekin) const;
G4std::vector<G4InuclElementaryParticle> generateSCMfinalState(G4double ekin,
std::vector<G4InuclElementaryParticle> generateSCMfinalState(G4double ekin,
G4double etot_scm, G4double pscm,
G4InuclElementaryParticle* particle1,
G4InuclElementaryParticle* particle2,
G4LorentzConvertor* toSCM) const;
G4std::vector<G4double> generateMomModules(const G4std::vector<G4int>& kinds,
std::vector<G4double> generateMomModules(const std::vector<G4int>& kinds,
G4int mult,
G4int is,
G4double ekin,
@@ -60,7 +60,7 @@ private:
G4bool reChargering(G4double ekin,
G4int is) const;
G4std::vector<G4double> particleSCMmomentumFor2to2(G4int is,
std::vector<G4double> particleSCMmomentumFor2to2(G4int is,
G4int kw,
G4double ekin,
G4double pscm) const;
@@ -69,7 +69,7 @@ private:
G4int kw,
G4double ekin) const;
G4std::vector<G4int> generateOutgoingKindsFor2toMany(G4int is,
std::vector<G4int> generateOutgoingKindsFor2toMany(G4int is,
G4int mult,
G4double ekin) const;
@@ -78,9 +78,9 @@ private:
G4int knd,
G4double ekin) const;
G4bool satisfyTriangle(const G4std::vector<G4double>& modules) const;
G4bool satisfyTriangle(const std::vector<G4double>& modules) const;
G4std::vector<G4double> particleSCMmomentumFor2to3(G4int is,
std::vector<G4double> particleSCMmomentumFor2to3(G4int is,
G4int knd,
G4double ekin,
G4double pmod) const;
@@ -88,15 +88,15 @@ private:
G4int getIL(G4int is,
G4int mult) const;
G4std::pair<G4double, G4double> adjustIntervalForElastic(G4double ekin,
std::pair<G4double, G4double> adjustIntervalForElastic(G4double ekin,
G4double ak,
G4double ae,
G4int k,
G4int l,
const G4std::vector<G4double>& ssv,
const std::vector<G4double>& ssv,
G4double st) const;
G4std::vector<G4InuclElementaryParticle>
std::vector<G4InuclElementaryParticle>
generateSCMpionAbsorption(G4double etot_scm,
G4InuclElementaryParticle* particle1,
G4InuclElementaryParticle* particle2) const;
source/processes/hadronic/models/cascade/cascade/include/G4FissionConfiguration.hh
+1 -1
View File
@@ -23,7 +23,7 @@
#define G4FISSION_CONFIGURATION_HH
#include "globals.hh"
#include "g4std/iostream"
#include <iostream>
class G4FissionConfiguration {
source/processes/hadronic/models/cascade/cascade/include/G4FissionStore.hh
+2 -2
View File
@@ -24,7 +24,7 @@
#include "G4FissionConfiguration.hh"
#include "g4std/vector"
#include <vector>
class G4FissionStore {
@@ -52,7 +52,7 @@ public:
private:
G4int verboseLevel;
G4std::vector<G4FissionConfiguration> configurations;
std::vector<G4FissionConfiguration> configurations;
};
source/processes/hadronic/models/cascade/cascade/include/G4Fissioner.hh
+3 -3
View File
@@ -52,14 +52,14 @@ G4int verboseLevel;
G4double R12) const;
void potentialMinimization(G4double& VP,
G4std::vector<G4double>& ED,
std::vector<G4double>& ED,
G4double& VC,
G4double AF,
G4double AS,
G4double ZF,
G4double ZS,
G4std::vector<G4double>& AL1,
G4std::vector<G4double>& BET1,
std::vector<G4double>& AL1,
std::vector<G4double>& BET1,
G4double& R12) const;
};
source/processes/hadronic/models/cascade/cascade/include/G4InteractionCase.hh
+4 -4
View File
@@ -26,14 +26,14 @@
#include "G4InuclParticle.hh"
//#endif
#include "g4std/algorithm"
#include <algorithm>
class G4InteractionCase {
public:
G4InteractionCase() {
bultag = G4std::pair<G4InuclParticle*, G4InuclParticle*>(0, 0);
bultag = std::pair<G4InuclParticle*, G4InuclParticle*>(0, 0);
inter_case = 0;
};
@@ -46,7 +46,7 @@ public:
void setBulletTarget(G4InuclParticle* part1,
G4InuclParticle* part2) {
bultag = G4std::pair<G4InuclParticle*, G4InuclParticle*>(part1, part2);
bultag = std::pair<G4InuclParticle*, G4InuclParticle*>(part1, part2);
};
void setInterCase(G4int ic) {
@@ -67,7 +67,7 @@ public:
private:
G4std::pair<G4InuclParticle*, G4InuclParticle*> bultag;
std::pair<G4InuclParticle*, G4InuclParticle*> bultag;
G4int inter_case;
source/processes/hadronic/models/cascade/cascade/include/G4InuclElementaryParticle.hh
+2 -2
View File
@@ -55,7 +55,7 @@ public:
valid_particle = false;
};
G4InuclElementaryParticle(const G4std::vector<G4double>& mom,
G4InuclElementaryParticle(const std::vector<G4double>& mom,
G4int type)
: G4InuclParticle(mom),
particleType(type) {
@@ -84,7 +84,7 @@ public:
particleMass = getParticleMass(ityp);
};
void setMomentum(const G4std::vector<G4double>& mom) {
void setMomentum(const std::vector<G4double>& mom) {
momentum = mom;
momentum[0] = sqrt(momentum[1] * momentum[1] + momentum[2] * momentum[2] +
source/processes/hadronic/models/cascade/cascade/include/G4InuclNuclei.hh
+2 -2
View File
@@ -45,7 +45,7 @@ public:
exitationEnergy = 0.0;
};
G4InuclNuclei(const G4std::vector<G4double>& mom,
G4InuclNuclei(const std::vector<G4double>& mom,
G4double a,
G4double z)
: G4InuclParticle(mom),
@@ -63,7 +63,7 @@ public:
Z(z) {
setNucleiMass();
G4std::vector<G4double> mom(4, 0.0);
std::vector<G4double> mom(4, 0.0);
mom[0] = ekin + nucleiMass;
mom[3] = sqrt(mom[0] * mom[0] - nucleiMass * nucleiMass);
G4InuclParticle::setMomentum(mom);
source/processes/hadronic/models/cascade/cascade/include/G4InuclParticle.hh
+6 -6
View File
@@ -26,8 +26,8 @@
#include "globals.hh"
#endif
#include "g4std/iostream"
#include "g4std/vector"
#include <iostream>
#include <vector>
class G4InuclParticle {
@@ -37,17 +37,17 @@ public:
virtual ~G4InuclParticle() { };
G4InuclParticle(const G4std::vector<G4double>& mom) {
G4InuclParticle(const std::vector<G4double>& mom) {
setMomentum(mom);
};
void setMomentum(const G4std::vector<G4double>& mom) {
void setMomentum(const std::vector<G4double>& mom) {
momentum = mom;
};
G4std::vector<G4double> getMomentum() const {
std::vector<G4double> getMomentum() const {
return momentum;
};
@@ -71,7 +71,7 @@ public:
protected:
G4std::vector<G4double> momentum;
std::vector<G4double> momentum;
};
source/processes/hadronic/models/cascade/cascade/include/G4InuclSpecialFunctions.hh
+6 -6
View File
@@ -24,8 +24,8 @@
#include "globals.hh"
#include <math.h>
#include "g4std/algorithm"
#include "g4std/vector"
#include <algorithm>
#include <vector>
namespace G4InuclSpecialFunctions {
@@ -46,9 +46,9 @@ namespace G4InuclSpecialFunctions {
G4double Z,
G4int ntype);
G4std::pair<G4std::vector<G4double>, G4std::vector<G4double> > paraMaker(G4double Z);
std::pair<std::vector<G4double>, std::vector<G4double> > paraMaker(G4double Z);
G4std::pair<G4double, G4double> paraMakerTruncated(G4double Z);
std::pair<G4double, G4double> paraMakerTruncated(G4double Z);
G4double getAL(G4double A);
@@ -62,11 +62,11 @@ namespace G4InuclSpecialFunctions {
G4double randomPHI();
G4std::pair<G4double, G4double> randomCOS_SIN();
std::pair<G4double, G4double> randomCOS_SIN();
G4double nucleiLevelDensity(G4double a);
G4std::vector<G4double> generateWithFixedTheta(G4double ct,
std::vector<G4double> generateWithFixedTheta(G4double ct,
G4double p);
}
#endif
source/processes/hadronic/models/cascade/cascade/include/G4LorentzConvertor.hh
+13 -13
View File
@@ -26,7 +26,7 @@
#include "globals.hh"
#endif
#include "g4std/vector"
#include <vector>
class G4LorentzConvertor {
@@ -34,9 +34,9 @@ public:
G4LorentzConvertor();
G4LorentzConvertor(const G4std::vector<G4double>& bmom,
G4LorentzConvertor(const std::vector<G4double>& bmom,
G4double bmass,
const G4std::vector<G4double>& tmom,
const std::vector<G4double>& tmom,
G4double tmass) {
setBullet(bmom, bmass);
@@ -44,7 +44,7 @@ public:
degenerated = false;
};
void setBullet(const G4std::vector<G4double>& bmom,
void setBullet(const std::vector<G4double>& bmom,
G4double bmass) {
bullet_mom = bmom;
@@ -52,7 +52,7 @@ public:
// G4cout << " bullet: e " << bmom[0] << " mass " << bmass << G4endl;
};
void setTarget(const G4std::vector<G4double>& tmom,
void setTarget(const std::vector<G4double>& tmom,
G4double tmass) {
target_mom = tmom;
@@ -64,7 +64,7 @@ public:
void toTheTargetRestFrame();
G4std::vector<G4double> backToTheLab(const G4std::vector<G4double>& mom) const;
std::vector<G4double> backToTheLab(const std::vector<G4double>& mom) const;
G4double getKinEnergyInTheTRS() const {
@@ -91,10 +91,10 @@ public:
return plab;
};
G4std::vector<G4double> rotate(const G4std::vector<G4double> mom) const;
std::vector<G4double> rotate(const std::vector<G4double> mom) const;
G4std::vector<G4double> rotate(const G4std::vector<G4double> mom1,
const G4std::vector<G4double> mom) const;
std::vector<G4double> rotate(const std::vector<G4double> mom1,
const std::vector<G4double> mom) const;
G4bool reflectionNeeded() const;
@@ -104,15 +104,15 @@ public:
private:
G4int verboseLevel;
G4std::vector<G4double> bullet_mom;
std::vector<G4double> bullet_mom;
G4double bullet_mass;
G4std::vector<G4double> target_mom;
std::vector<G4double> target_mom;
G4double target_mass;
G4std::vector<G4double> velocity;
std::vector<G4double> velocity;
G4std::vector<G4double> scm_momentum;
std::vector<G4double> scm_momentum;
G4double ecm_tot;
source/processes/hadronic/models/cascade/cascade/include/G4NuclWatcher.hh
+19 -19
View File
@@ -26,8 +26,8 @@
#include "globals.hh"
#endif
#include "g4std/algorithm"
#include "g4std/vector"
#include <algorithm>
#include <vector>
#include <math.h>
class G4NuclWatcher {
@@ -35,9 +35,9 @@ class G4NuclWatcher {
public:
G4NuclWatcher(G4double z,
G4std::vector<G4double> expa,
G4std::vector<G4double> expcs,
G4std::vector<G4double> experr,
std::vector<G4double> expa,
std::vector<G4double> expcs,
std::vector<G4double> experr,
G4bool check,
G4bool nucl)
: nuclz(z),
@@ -89,12 +89,12 @@ public:
return izotop_chsq;
};
G4std::pair<G4double, G4double> getAverageRatio() const {
std::pair<G4double, G4double> getAverageRatio() const {
return G4std::pair<G4double, G4double>(average_ratio, aver_rat_err);
return std::pair<G4double, G4double>(average_ratio, aver_rat_err);
};
G4std::pair<G4double, G4double> getExpCs() const {
std::pair<G4double, G4double> getExpCs() const {
G4double cs = 0.0;
G4double err = 0.0;
@@ -105,7 +105,7 @@ public:
err += exper_err[iz];
};
return G4std::pair<G4double, G4double>(cs, err);
return std::pair<G4double, G4double>(cs, err);
};
G4bool to_check() const {
@@ -118,7 +118,7 @@ public:
return nucleable;
};
G4std::pair<G4double, G4double> getInuclCs() const {
std::pair<G4double, G4double> getInuclCs() const {
G4double cs = 0.0;
G4double err = 0.0;
@@ -128,7 +128,7 @@ public:
err += simulated_errors[iz];
};
return G4std::pair<G4double, G4double>(cs, err);
return std::pair<G4double, G4double>(cs, err);
};
void print() {
@@ -146,7 +146,7 @@ public:
G4double exp_cs_err = 0.0;
G4double inucl_cs = 0.0;
G4double inucl_cs_err = 0.0;
G4std::vector<G4bool> not_used(simulated_cs.size(), true);
std::vector<G4bool> not_used(simulated_cs.size(), true);
G4int nmatched = exper_as.size();
G4int nused = simulated_cs.size();
G4double lhood = 0.0;
@@ -253,19 +253,19 @@ private:
G4double aver_matched;
G4std::vector<G4double> exper_as;
std::vector<G4double> exper_as;
G4std::vector<G4double> exper_cs;
std::vector<G4double> exper_cs;
G4std::vector<G4double> exper_err;
std::vector<G4double> exper_err;
G4std::vector<G4double> simulated_as;
std::vector<G4double> simulated_as;
G4std::vector<G4double> simulated_cs;
std::vector<G4double> simulated_cs;
G4std::vector<G4double> simulated_errors;
std::vector<G4double> simulated_errors;
G4std::vector<G4double> simulated_prob;
std::vector<G4double> simulated_prob;
G4bool checkable;
source/processes/hadronic/models/cascade/cascade/include/G4NucleiModel.hh
+13 -13
View File
@@ -32,15 +32,15 @@
#include "G4CascadSpecialFunctions.hh"
#include "G4ElementaryParticleCollider.hh"
#include "g4std/vector"
#include <vector>
class G4InuclNuclei;
using namespace G4InuclSpecialFunctions;
using namespace G4CascadSpecialFunctions;
typedef G4std::pair<G4InuclElementaryParticle, G4double> partner;
typedef G4std::vector<partner> partners;
typedef std::pair<G4InuclElementaryParticle, G4double> partner;
typedef std::vector<partner> partners;
class G4NucleiModel {
@@ -99,7 +99,7 @@ public:
return izone < number_of_zones ? zone_potentials[ip0][izone] : 0.0;
};
G4std::vector<G4CascadParticle>
std::vector<G4CascadParticle>
generateParticleFate(G4CascadParticle& cparticle,
G4ElementaryParticleCollider* theElementaryParticleCollider);
@@ -125,10 +125,10 @@ public:
G4CascadParticle initializeCascad(G4InuclElementaryParticle* particle);
G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> > initializeCascad(G4InuclNuclei* bullet, G4InuclNuclei* target);
std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> > initializeCascad(G4InuclNuclei* bullet, G4InuclNuclei* target);
G4std::pair<G4int, G4int> getTypesOfNucleonsInvolved() const {
return G4std::pair<G4int, G4int>(current_nucl1, current_nucl2);
std::pair<G4int, G4int> getTypesOfNucleonsInvolved() const {
return std::pair<G4int, G4int>(current_nucl1, current_nucl2);
};
G4bool worthToPropagate(const G4CascadParticle& cparticle) const;
@@ -137,7 +137,7 @@ public:
private:
G4int verboseLevel;
G4bool passFermi(const G4std::vector<G4InuclElementaryParticle>& particles,
G4bool passFermi(const std::vector<G4InuclElementaryParticle>& particles,
G4int zone);
void boundaryTransition(G4CascadParticle& cparticle);
@@ -159,15 +159,15 @@ G4int verboseLevel;
G4double getRatio(G4int ip) const;
G4std::vector<G4std::vector<G4double> > nucleon_densities;
std::vector<std::vector<G4double> > nucleon_densities;
G4std::vector<G4std::vector<G4double> > zone_potentials;
std::vector<std::vector<G4double> > zone_potentials;
G4std::vector<G4std::vector<G4double> > fermi_momenta;
std::vector<std::vector<G4double> > fermi_momenta;
G4std::vector<G4double> zone_radii;
std::vector<G4double> zone_radii;
G4std::vector<G4double> binding_energies;
std::vector<G4double> binding_energies;
G4double nuclei_radius;
source/processes/hadronic/models/cascade/cascade/include/G4RegionModel.hh
-78
View File
@@ -1,78 +0,0 @@
//
// ********************************************************************
// * DISCLAIMER *
// * *
// * The following disclaimer summarizes all the specific disclaimers *
// * of contributors to this software. The specific disclaimers,which *
// * govern, are listed with their locations in: *
// * http://cern.ch/geant4/license *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. *
// * *
// * This code implementation is the intellectual property of the *
// * GEANT4 collaboration. *
// * By copying, distributing or modifying the Program (or any work *
// * based on the Program) you indicate your acceptance of this *
// * statement, and all its terms. *
// ********************************************************************
#ifndef G4REGIONMODEL
#define G4REGIONMODEL
#include "G4ios.hh"
#include "g4std/vector"
#include <math.h>
#include "globals.hh"
#include "G4Proton.hh"
#include "G4Neutron.hh"
//#include "G4NucleusModel.hh"
typedef G4std::vector<G4double>::const_iterator iterator;
class G4RegionModel //:public G4VRegionModel
{
public:
G4RegionModel(const G4int numberOfLayers, const G4int A, const G4int Z);
~G4RegionModel();
//instead of A and Z outer radius of the nucleus?
//void Init(const G4int numberOfLayers, const G4int A, const G4int Z);
G4double GetDensity(G4double radius);
G4double GetPotentialEnergy(G4double r, G4int particle);
G4double GetMaximumNucleonMomentum(G4double radius, G4int nucleon);
// G4double NumberOfRegions();
private:
G4int massNumber;
G4int protonNumber;
G4std::vector<G4double> radius; //contains the outer radiuses of the shells
G4std::vector<G4double> density;
G4std::vector<G4double> protonFermiEnergy;
G4std::vector<G4double> neutronFermiEnergy;
G4std::vector<G4double> protonFermiMomentum;
G4std::vector<G4double> neutronFermiMomentum;
G4std::vector<G4double> protonPotentialEnergy;
G4std::vector<G4double> neutronPotentialEnergy;
static const G4double radius0;
static const G4double BE;
//static const G4double pi = 3.141592;
G4double GetFermiMomentum(G4double density, G4double mass);
G4double GetFermiEnergy(G4double density, G4double mass);
};
#endif
source/processes/hadronic/models/cascade/cascade/include/G4WatcherGun.hh
+3 -3
View File
@@ -23,7 +23,7 @@
#define G4WATCHER_GUN_HH
#include "G4NuclWatcher.hh"
#include "g4std/vector"
#include <vector>
class G4WatcherGun {
@@ -32,14 +32,14 @@ public:
G4WatcherGun();
void setWatchers();
G4std::vector<G4NuclWatcher> getWatchers() const {
std::vector<G4NuclWatcher> getWatchers() const {
return watchers;
};
private:
G4int verboseLevel;
G4std::vector<G4NuclWatcher> watchers;
std::vector<G4NuclWatcher> watchers;
};
source/processes/hadronic/models/cascade/cascade/src/G4Analyser.cc
+7 -7
View File
@@ -65,7 +65,7 @@ void G4Analyser::setInelCsec(G4double csec,
}
}
void G4Analyser::setWatchers(const G4std::vector<G4NuclWatcher>& watchers) {
void G4Analyser::setWatchers(const std::vector<G4NuclWatcher>& watchers) {
if (verboseLevel > 3) {
G4cout << " >>> G4Analyser::setWatchers" << G4endl;
@@ -106,7 +106,7 @@ void G4Analyser::analyse(const G4CollisionOutput& output) {
}
if (withNuclei) {
G4std::vector<G4InuclNuclei> nucleus = output.getNucleiFragments();
std::vector<G4InuclNuclei> nucleus = output.getNucleiFragments();
if (nucleus.size() >= 0) {
G4int nbig = 0;
@@ -129,7 +129,7 @@ void G4Analyser::analyse(const G4CollisionOutput& output) {
if (nbig > 1) fissy_prob += 1.0;
eventNumber += 1.0;
G4std::vector<G4InuclElementaryParticle> particles = output.getOutgoingParticles();
std::vector<G4InuclElementaryParticle> particles = output.getOutgoingParticles();
averageMultiplicity += particles.size();
for (G4int i = 0; i < G4int(particles.size()); i++) {
@@ -176,7 +176,7 @@ void G4Analyser::analyse(const G4CollisionOutput& output) {
} else {
eventNumber += 1.0;
G4std::vector<G4InuclElementaryParticle> particles = output.getOutgoingParticles();
std::vector<G4InuclElementaryParticle> particles = output.getOutgoingParticles();
averageMultiplicity += particles.size();
for (G4int i = 0; i < G4int(particles.size()); i++) {
@@ -294,14 +294,14 @@ void G4Analyser::handleWatcherStatistics() {
ana_watchers[iw].print();
if (ana_watchers[iw].to_check()) {
G4std::pair<G4double, G4double> rat_err = ana_watchers[iw].getAverageRatio();
std::pair<G4double, G4double> rat_err = ana_watchers[iw].getAverageRatio();
averat += rat_err.first;
ave_err += rat_err.second;
gl_chsq += ana_watchers[iw].getChsq();
G4std::pair<G4double, G4double> cs_err = ana_watchers[iw].getExpCs();
std::pair<G4double, G4double> cs_err = ana_watchers[iw].getExpCs();
tot_exper += cs_err.first;
tot_exper_err += cs_err.second;
G4std::pair<G4double, G4double> inucl_cs_err = ana_watchers[iw].getInuclCs();
std::pair<G4double, G4double> inucl_cs_err = ana_watchers[iw].getInuclCs();
tot_inucl += inucl_cs_err.first;
tot_inucl_err += inucl_cs_err.second;
G4double iz_checked = ana_watchers[iw].getNmatched();
source/processes/hadronic/models/cascade/cascade/src/G4BertiniNucleiModel.cc
+50 -50
View File
@@ -24,7 +24,7 @@
#include "G4LorentzConvertor.hh"
#include "G4CollisionOutput.hh"
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
G4BertiniNucleiModel::G4BertiniNucleiModel()
: verboseLevel(2) {
@@ -75,7 +75,7 @@ void G4BertiniNucleiModel::generateModel(G4double a,
G4double CU2 = 0.0;
if (a > 3.5) { /// a > 3
G4std::vector<G4double> ur;
std::vector<G4double> ur;
G4int icase = 0;
if (a > 11.5) { /// a > 11
@@ -106,8 +106,8 @@ void G4BertiniNucleiModel::generateModel(G4double a,
};
G4double tot_vol = 0.0;
G4std::vector<G4double> v;
G4std::vector<G4double> v1;
std::vector<G4double> v;
std::vector<G4double> v1;
G4int i(0);
for (i = 0; i < number_of_zones; i++) {
@@ -130,9 +130,9 @@ void G4BertiniNucleiModel::generateModel(G4double a,
/// proton
G4double dd0 = 3.0 * z * oneBypiTimes4 / tot_vol;
G4std::vector<G4double> rod;
G4std::vector<G4double> pf;
G4std::vector<G4double> vz;
std::vector<G4double> rod;
std::vector<G4double> pf;
std::vector<G4double> vz;
for (i = 0; i < number_of_zones; i++) {
G4double rd = dd0 * v[i] / v1[i];
@@ -164,7 +164,7 @@ void G4BertiniNucleiModel::generateModel(G4double a,
zone_potentials.push_back(vz);
fermi_momenta.push_back(pf);
/// pion
G4std::vector<G4double> vp(number_of_zones, pion_vp);
std::vector<G4double> vp(number_of_zones, pion_vp);
zone_potentials.push_back(vp);
} else { /// a < 4
@@ -172,9 +172,9 @@ void G4BertiniNucleiModel::generateModel(G4double a,
number_of_zones = 1;
zone_radii.push_back(radForSmall);
G4double vol = 1.0 / piTimes4thirds / pow(zone_radii[0], 3);
G4std::vector<G4double> rod;
G4std::vector<G4double> pf;
G4std::vector<G4double> vz;
std::vector<G4double> rod;
std::vector<G4double> pf;
std::vector<G4double> vz;
G4int i(0);
for (i = 0; i < number_of_zones; i++) {
@@ -207,7 +207,7 @@ void G4BertiniNucleiModel::generateModel(G4double a,
fermi_momenta.push_back(pf);
/// pion
G4std::vector<G4double> vp(number_of_zones, pion_vp_small);
std::vector<G4double> vp(number_of_zones, pion_vp_small);
zone_potentials.push_back(vp);
};
@@ -355,8 +355,8 @@ G4InuclElementaryParticle G4BertiniNucleiModel::generateNucleon(G4int type,
const G4double one_third = 1.0 / 3.0;
///G4double pmod = getFermiMomentum(type, zone) * pow(inuclRndm(), one_third);
G4double pmod = fermi_momenta[type - 1][zone] * pow(inuclRndm(), one_third);
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double pt = pmod * COS_SIN.second;
mom[1] = pt * cos(FI);
@@ -374,11 +374,11 @@ G4InuclElementaryParticle G4BertiniNucleiModel::generateQuasiDeutron(G4int type1
G4cout << " >>> G4BertiniNucleiModel::generateQuasiDeutron" << G4endl;
}
G4std::vector<G4double> mom = generateNucleon(type1, zone).getMomentum();
std::vector<G4double> mom = generateNucleon(type1, zone).getMomentum();
G4std::vector<G4double> mom1 = generateNucleon(type2, zone).getMomentum();
std::vector<G4double> mom1 = generateNucleon(type2, zone).getMomentum();
G4std::vector<G4double> dmom(4);
std::vector<G4double> dmom(4);
for(G4int i = 1; i < 4; i++) dmom[i] = mom[i] + mom1[i];
@@ -422,7 +422,7 @@ partners G4BertiniNucleiModel::generateInteractionPartners(G4CascadParticle& cpa
G4int ptype = cparticle.getParticle().type();
G4int zone = cparticle.getCurrentZone();
G4double pmass = cparticle.getParticle().getMass();
G4std::vector<G4double> pmom = cparticle.getParticle().getMomentum();
std::vector<G4double> pmom = cparticle.getParticle().getMomentum();
G4double r_in;
G4double r_out;
@@ -460,7 +460,7 @@ partners G4BertiniNucleiModel::generateInteractionPartners(G4CascadParticle& cpa
} else { /// normal case
G4std::vector<G4InuclElementaryParticle> particles;
std::vector<G4InuclElementaryParticle> particles;
G4LorentzConvertor dummy_convertor;
dummy_convertor.setBullet(pmom, pmass);
@@ -509,8 +509,8 @@ partners G4BertiniNucleiModel::generateInteractionPartners(G4CascadParticle& cpa
}
if (cparticle.getParticle().pion()) { /// absorption possible
G4std::vector<G4InuclElementaryParticle> qdeutrons;
G4std::vector<G4double> acsecs;
std::vector<G4InuclElementaryParticle> qdeutrons;
std::vector<G4double> acsecs;
G4double tot_abs_csec = 0.0;
G4double abs_sec;
G4double vol = pow(zone_radii[zone], 3);
@@ -650,14 +650,14 @@ partners G4BertiniNucleiModel::generateInteractionPartners(G4CascadParticle& cpa
return thePartners;
}
G4std::vector<G4CascadParticle> G4BertiniNucleiModel::generateParticleFate(G4CascadParticle& cparticle,
std::vector<G4CascadParticle> G4BertiniNucleiModel::generateParticleFate(G4CascadParticle& cparticle,
G4ElementaryParticleCollider* theElementaryParticleCollider) {
if (verboseLevel > 3) {
G4cout << " >>> G4BertiniNucleiModel::generateParticleFate" << G4endl;
}
G4std::vector<G4CascadParticle> outgouing_cparticles;
std::vector<G4CascadParticle> outgouing_cparticles;
partners thePartners = generateInteractionPartners(cparticle);
@@ -682,7 +682,7 @@ G4std::vector<G4CascadParticle> G4BertiniNucleiModel::generateParticleFate(G4Cas
} else { /// there are possible interactions
G4std::vector<G4double> old_position = cparticle.getPosition();
std::vector<G4double> old_position = cparticle.getPosition();
G4InuclElementaryParticle bullet = cparticle.getParticle();
G4bool no_interaction = true;
G4int zone = cparticle.getCurrentZone();
@@ -705,13 +705,13 @@ G4std::vector<G4CascadParticle> G4BertiniNucleiModel::generateParticleFate(G4Cas
output.printCollisionOutput();
}
G4std::vector<G4InuclElementaryParticle> outgoing_particles =
std::vector<G4InuclElementaryParticle> outgoing_particles =
output.getOutgoingParticles();
if(passFermi(outgoing_particles, zone)) { /// interaction
cparticle.propagateAlongThePath(thePartners[i].second);
G4std::vector<G4double> new_position = cparticle.getPosition();
std::vector<G4double> new_position = cparticle.getPosition();
for (G4int ip = 0; ip < G4int(outgoing_particles.size()); ip++)
outgouing_cparticles.push_back(G4CascadParticle(outgoing_particles[ip],
@@ -783,7 +783,7 @@ G4std::vector<G4CascadParticle> G4BertiniNucleiModel::generateParticleFate(G4Cas
return outgouing_cparticles;
}
G4bool G4BertiniNucleiModel::passFermi(const G4std::vector<G4InuclElementaryParticle>& particles,
G4bool G4BertiniNucleiModel::passFermi(const std::vector<G4InuclElementaryParticle>& particles,
G4int zone) {
if (verboseLevel > 3) {
G4cout << " >>> G4BertiniNucleiModel::passFermi" << G4endl;
@@ -825,8 +825,8 @@ void G4BertiniNucleiModel::boundaryTransition(G4CascadParticle& cparticle) {
} else {
G4std::vector<G4double> mom = cparticle.getMomentum();
G4std::vector<G4double> pos = cparticle.getPosition();
std::vector<G4double> mom = cparticle.getMomentum();
std::vector<G4double> pos = cparticle.getPosition();
G4int type = cparticle.getParticle().type();
G4double pr = 0.0;
G4double r = 0.0;
@@ -926,7 +926,7 @@ G4CascadParticle G4BertiniNucleiModel::initializeCascad(G4InuclElementaryParticl
G4double s1 = sqrt(inuclRndm());
G4double phi = randomPHI();
G4double rz = nuclei_radius * s1;
G4std::vector<G4double> pos(3);
std::vector<G4double> pos(3);
pos[0] = rz * cos(phi);
pos[1] = rz * sin(phi);
pos[2] = -nuclei_radius * sqrt(1.0 - s1 * s1);
@@ -940,7 +940,7 @@ G4CascadParticle G4BertiniNucleiModel::initializeCascad(G4InuclElementaryParticl
return cpart;
}
G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4InuclNuclei* target) {
@@ -960,8 +960,8 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
const G4double s4max = 7.0;
const G4int itry_max = 100;
G4std::vector<G4CascadParticle> casparticles;
G4std::vector<G4InuclElementaryParticle> particles;
std::vector<G4CascadParticle> casparticles;
std::vector<G4InuclElementaryParticle> particles;
G4double ab = bullet->getA();
@@ -983,14 +983,14 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
if (itryg > 0) particles.resize(0);
G4std::vector<G4std::vector<G4double> > coordinates; /// nucleons coordinates in nuclei rest frame
G4std::vector<G4std::vector<G4double> > momentums;
std::vector<std::vector<G4double> > coordinates; /// nucleons coordinates in nuclei rest frame
std::vector<std::vector<G4double> > momentums;
if (ab < 3.0) { /// deutron, simplest case
G4double r = 2.214 - 3.4208 * log(1.0 - 0.981 * inuclRndm());
G4double s = 2.0 * inuclRndm() - 1.0;
G4double r1 = r * sqrt(1.0 - s * s);
G4std::vector<G4double> coord1(3);
std::vector<G4double> coord1(3);
G4double phi = randomPHI();
coord1[0] = r1 * cos(phi);
coord1[1] = r1 * sin(phi);
@@ -1026,8 +1026,8 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4cout << " p nuc " << p << G4endl;
}
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double P1 = p * COS_SIN.second;
mom[1] = P1 * cos(FI);
@@ -1041,7 +1041,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
} else {
G4int ia = G4int(ab + 0.5);
G4std::vector<G4double> coord1(3);
std::vector<G4double> coord1(3);
G4bool badco = true;
G4int itry = 0;
@@ -1068,7 +1068,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
if (sqrt(s) * exp(-s) > u && s < s3max) {
s = r0forAeq3 * sqrt(s);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
u = s * COS_SIN.second;
G4double phi = randomPHI();
coord1[0] = u * cos(phi);
@@ -1156,7 +1156,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
if (sqrt(s) * exp(-s) * (1.0 + b * s) > u && s < s4max) {
s = r0forAeq4 * sqrt(s);
G4std::pair<double, double> COS_SIN = randomCOS_SIN();
std::pair<double, double> COS_SIN = randomCOS_SIN();
u = s * COS_SIN.second;
G4double phi = randomPHI();
coord1[0] = u * cos(phi);
@@ -1227,14 +1227,14 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4cout << " can not generate the nucleons coordinates for a " << ab <<
G4endl;
return G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
return std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
(casparticles, particles);
} else { /// momentums
G4double p;
G4double u;
G4double x;
G4std::vector<G4double> mom(4);
std::vector<G4double> mom(4);
/// G4bool badp = True;
G4int i(0);
@@ -1248,7 +1248,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
if (x > inuclRndm()) {
p = sqrt(0.01953 * u);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double pt = p * COS_SIN.second;
G4double phi = randomPHI();
mom[1] = pt * cos(phi);
@@ -1263,7 +1263,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
if (itry == itry_max) {
G4cout << " can not generate proper momentum for a " << ab << G4endl;
return G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
return std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
(casparticles, particles);
};
};
@@ -1292,7 +1292,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4double s1 = sqrt(inuclRndm());
G4double phi = randomPHI();
G4double rz = (nuclei_radius + rb) * s1;
G4std::vector<double> global_pos(3);
std::vector<double> global_pos(3);
global_pos[0] = rz * cos(phi);
global_pos[1] = rz * sin(phi);
global_pos[2] = -(nuclei_radius + rb) * sqrt(1.0 - s1 * s1);
@@ -1304,7 +1304,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
};
/// all nucleons at rest
G4std::vector<G4InuclElementaryParticle> raw_particles;
std::vector<G4InuclElementaryParticle> raw_particles;
G4int ia = G4int(ab + 0.5);
G4int iz = G4int(zb + 0.5);
@@ -1325,7 +1325,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
particleIterator ipart;
for (ipart = raw_particles.begin(); ipart != raw_particles.end(); ipart++) {
G4std::vector<G4double> mom =
std::vector<G4double> mom =
toTheBulletRestFrame.backToTheLab(ipart->getMomentum());
ipart->setMomentum(mom);
@@ -1333,7 +1333,7 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
/// fill cascad particles and outgoing particles
for (G4int ip = 0; ip < G4int(raw_particles.size()); ip++) {
G4std::vector<G4double> mom = raw_particles[ip].getMomentum();
std::vector<G4double> mom = raw_particles[ip].getMomentum();
G4double pmod = sqrt(mom[1] * mom[1] + mom[2] * mom[2] + mom[3] * mom[3]);
G4double t0 = -(mom[1] * coordinates[ip][0] + mom[2] * coordinates[ip][1] +
mom[3] * coordinates[ip][2]) / pmod;
@@ -1407,6 +1407,6 @@ G4BertiniNucleiModel::initializeCascad(G4InuclNuclei* bullet,
particles[ip].printParticle();
}
return G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
return std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
(casparticles, particles);
}
source/processes/hadronic/models/cascade/cascade/src/G4BertiniRegionModel.cc
-189
View File
@@ -1,189 +0,0 @@
//
// ********************************************************************
// * DISCLAIMER *
// * *
// * The following disclaimer summarizes all the specific disclaimers *
// * of contributors to this software. The specific disclaimers,which *
// * govern, are listed with their locations in: *
// * http://cern.ch/geant4/license *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. *
// * *
// * This code implementation is the intellectual property of the *
// * GEANT4 collaboration. *
// * By copying, distributing or modifying the Program (or any work *
// * based on the Program) you indicate your acceptance of this *
// * statement, and all its terms. *
// ********************************************************************
#include "G4BertiniRegionModel.hh"
const G4double G4BertiniRegionModel::radius0 = 1.0E-15;
const G4double G4BertiniRegionModel::BE = 7;
G4BertiniRegionModel::G4BertiniRegionModel(const G4int numberOfLayers, const G4int A, const G4int Z)
{
//count the radiuses, densities and fermi momenta with A and Z
G4double r = radius0*pow(A, 1/3);
if(numberOfLayers==1){
radius.push_back(r);
G4double rho = A / (4/3*pi*pow(r,3));
density.push_back(rho);
G4double protonMass = G4Proton::Proton()->GetPDGMass();
G4double neutronMass = G4Neutron::Neutron()->GetPDGMass();
G4double protonDensity = Z / (4/3*pi*pow(r,3));
G4double neutronDensity = (A-Z) / (4/3*pi*pow(r,3));
protonFermiEnergy.push_back(GetFermiEnergy(protonDensity, protonMass));
neutronFermiEnergy.push_back(GetFermiEnergy(neutronDensity, neutronMass));
protonFermiMomentum.push_back(GetFermiMomentum(protonDensity, protonMass));
neutronFermiMomentum.push_back(GetFermiMomentum(neutronDensity, neutronMass));
G4double fermiEP = *protonFermiEnergy.begin();
G4double fermiEN = *neutronFermiEnergy.begin();
protonPotentialEnergy.push_back(-(fermiEP + BE));
neutronPotentialEnergy.push_back(-(fermiEN + BE));
}
else{
if(numberOfLayers==3){
radius.push_back(0.1*r);
radius.push_back(0.2*r);
radius.push_back(0.9*r);
}
}
}
G4BertiniRegionModel::~G4BertiniRegionModel(){}
/*
void G4BertiniRegionModel::Init(const G4int numberOfLayers, const G4int A, const G4int Z){
//count the radiuses, densities and fermi momenta with A and Z
G4double r = radius0*pow(A, 1/3);
if(numberOfLayers==1){
radius.push_back(r);
G4double rho = A / (4/3*pi*pow(r,3));
density.push_back(rho);
G4double protonMass = G4Proton::Proton()->GetPDGMass()/MeV;
G4double neutronMass = G4Neutron::Neutron()->GetPDGMass()/MeV ;
G4double protonDensity = Z / (4/3*pi*pow(r,3));
G4double neutronDensity = (A-Z) / (4/3*pi*pow(r,3));
protonFermiEnergy.push_back(GetFermiEnergy(protonDensity, protonMass));
neutronFermiEnergy.push_back(GetFermiEnergy(neutronDensity, neutronMass));
protonFermiMomentum.push_back(GetFermiMomentum(protonDensity, protonMass));
neutronFermiMomentum.push_back(GetFermiMomentum(neutronDensity, neutronMass));
G4double fermiEP = *protonFermiEnergy.begin();
G4double fermiEN = *neutronFermiEnergy.begin();
protonPotentialEnergy.push_back(-(fermiEP + BE));
neutronPotentialEnergy.push_back(-(fermiEN + BE));
}
else{
if(numberOfLayers==3){
radius.push_back(0.1*r);
radius.push_back(0.2*r);
radius.push_back(0.9*r);
}
}
}
*/
//--------------------------------------------------------------
G4double G4BertiniRegionModel::GetDensity(G4double r){
iterator j=density.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
return 0;
}
G4double G4BertiniRegionModel::GetPotentialEnergy(G4double r, G4int particle){
if(particle == 0){ //proton
iterator j=protonPotentialEnergy.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
return 0;
}
if(particle == 1){ //neutron
iterator j=neutronPotentialEnergy.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
return 0;
}
return 0;
}
G4double G4BertiniRegionModel::GetMaximumNucleonMomentum(G4double r,
G4int nucleon){
if(nucleon == 0){
iterator j=protonFermiMomentum.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
}
if(nucleon==1){
iterator j=neutronFermiMomentum.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
}
G4Exception("G4BertiniRegionModel::GetMaximumNucleonMomentum - return value undefined");
return 0;
}
G4double G4BertiniRegionModel::GetFermiMomentum(G4double aDensity,
G4double aMass){
return sqrt(2*aMass*GetFermiEnergy(aDensity, aMass));
}
G4double G4BertiniRegionModel::GetFermiEnergy(G4double aDensity,
G4double aMass){
//G4double hbar = 1.0E-6;
return (pow(hbar_Planck,2)/(2*aMass)*pow((3*pi2*aDensity),2/3));
}
source/processes/hadronic/models/cascade/cascade/src/G4BigBanger.cc
+29 -29
View File
@@ -24,9 +24,9 @@
#include "G4InuclNuclei.hh"
#include "G4ParticleLargerEkin.hh"
#include "G4LorentzConvertor.hh"
#include "g4std/algorithm"
#include <algorithm>
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
G4BigBanger::G4BigBanger()
: verboseLevel(1) {
@@ -47,14 +47,14 @@ G4CollisionOutput G4BigBanger::collide(G4InuclParticle* bullet,
const G4double small_ekin = 1.0e-6;
G4CollisionOutput output;
G4std::vector<G4double> totscm;
G4std::vector<G4double> totlab;
std::vector<G4double> totscm;
std::vector<G4double> totlab;
if(G4InuclNuclei* nuclei_target = dynamic_cast<G4InuclNuclei*>(target)) {
G4double A = nuclei_target->getA();
G4double Z = nuclei_target->getZ();
G4std::vector<G4double> PEX = nuclei_target->getMomentum();
std::vector<G4double> PEX = nuclei_target->getMomentum();
G4double EEXS = nuclei_target->getExitationEnergy();
G4InuclElementaryParticle dummy(small_ekin, 1);
G4LorentzConvertor toTheNucleiSystemRestFrame;
@@ -72,7 +72,7 @@ G4CollisionOutput G4BigBanger::collide(G4InuclParticle* bullet,
etot << " nm " << nuclei_target->getMass() << G4endl;
}
G4std::vector<G4InuclElementaryParticle> particles =
std::vector<G4InuclElementaryParticle> particles =
generateBangInSCM(etot, A, Z, dummy.getParticleMass(1), dummy.getParticleMass(2));
if (verboseLevel > 2) {
@@ -82,18 +82,18 @@ G4CollisionOutput G4BigBanger::collide(G4InuclParticle* bullet,
}
if(!particles.empty()) { // convert back to Lab
if (verboseLevel > 2) {
G4std::vector<G4double> totscm(4, 0.0);
G4std::vector<G4double> totlab(4, 0.0);
std::vector<G4double> totscm(4, 0.0);
std::vector<G4double> totlab(4, 0.0);
}
particleIterator ipart;
for(ipart = particles.begin(); ipart != particles.end(); ipart++) {
if (verboseLevel > 2) {
G4std::vector<G4double> mom_scm = ipart->getMomentum();
std::vector<G4double> mom_scm = ipart->getMomentum();
for(G4int i = 0; i < 4; i++) totscm[i] += mom_scm[i];
}
G4std::vector<G4double> mom =
std::vector<G4double> mom =
toTheNucleiSystemRestFrame.backToTheLab(ipart->getMomentum());
ipart->setMomentum(mom);
@@ -102,7 +102,7 @@ G4CollisionOutput G4BigBanger::collide(G4InuclParticle* bullet,
for(G4int i = 0; i < 4; i++) totlab[i] += mom[i];
}
};
G4std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
if (verboseLevel > 2) {
G4cout << " In SCM: total outgoing momentum " << G4endl
<< " E " << totscm[0] << " px " << totscm[1]
@@ -123,7 +123,7 @@ G4CollisionOutput G4BigBanger::collide(G4InuclParticle* bullet,
return output;
}
G4std::vector<G4InuclElementaryParticle>
std::vector<G4InuclElementaryParticle>
G4BigBanger::generateBangInSCM(G4double etot,
G4double a,
G4double z,
@@ -143,14 +143,14 @@ G4BigBanger::generateBangInSCM(G4double etot,
if (verboseLevel > 2) {
G4cout << " ia " << ia << " iz " << iz << G4endl;
}
G4std::vector<G4InuclElementaryParticle> particles;
std::vector<G4InuclElementaryParticle> particles;
if(ia == 1) {
// abnormal situation
G4double m = iz > 0 ? mp : mn;
G4double pmod = sqrt((etot + 2.0 * m) * etot);
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double Pt = pmod * COS_SIN.second;
@@ -165,18 +165,18 @@ G4BigBanger::generateBangInSCM(G4double etot,
return particles;
};
G4std::vector<G4double> pmod = generateMomentumModules(etot, a, z, mp, mn);
std::vector<G4double> pmod = generateMomentumModules(etot, a, z, mp, mn);
G4bool bad = true;
G4int itry = 0;
while(bad && itry < itry_max) {
itry++;
G4std::vector<G4std::vector<G4double> > scm_momentums;
G4std::vector<G4double> tot_mom(4);
std::vector<std::vector<G4double> > scm_momentums;
std::vector<G4double> tot_mom(4);
if(ia == 2) {
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
double FI = randomPHI();
double Pt = pmod[0] * COS_SIN.second;
@@ -188,7 +188,7 @@ G4BigBanger::generateBangInSCM(G4double etot,
scm_momentums.push_back(mom);
G4std::vector<G4double> mom1(4);
std::vector<G4double> mom1(4);
for(G4int i = 1; i < 4; i++) mom1[i] = - mom[i];
@@ -197,8 +197,8 @@ G4BigBanger::generateBangInSCM(G4double etot,
}
else {
for(G4int i = 0; i < ia - 2; i++) {
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double Pt = pmod[i] * COS_SIN.second;
@@ -223,19 +223,19 @@ G4BigBanger::generateBangInSCM(G4double etot,
}
if(fabs(ct) < ang_cut) {
G4std::vector<G4double> mom2 = generateWithFixedTheta(ct, pmod[ia - 2]);
std::vector<G4double> mom2 = generateWithFixedTheta(ct, pmod[ia - 2]);
// rotate to the normal system
G4std::vector<G4double> apr = tot_mom;
std::vector<G4double> apr = tot_mom;
G4int i;
for(i = 1; i < 4; i++) apr[i] /= tot_mod;
G4double a_tr = sqrt(apr[1] * apr[1] + apr[2] * apr[2]);
G4std::vector<G4double> mom(4);
std::vector<G4double> mom(4);
mom[1] = mom2[3] * apr[1] + ( mom2[1] * apr[2] + mom2[2] * apr[3] * apr[1]) / a_tr; // ::: replace with clhep tools?
mom[2] = mom2[3] * apr[2] + (-mom2[1] * apr[1] + mom2[2] * apr[3] * apr[2]) / a_tr;
mom[3] = mom2[3] * apr[3] - mom2[2] * a_tr;
scm_momentums.push_back(mom);
// and the last one
G4std::vector<G4double> mom1(4);
std::vector<G4double> mom1(4);
for(i = 1; i < 4; i++) mom1[i] = - mom[i] - tot_mom[i];
scm_momentums.push_back(mom1);
bad = false;
@@ -257,7 +257,7 @@ G4BigBanger::generateBangInSCM(G4double etot,
}
G4std::vector<G4double> G4BigBanger::generateMomentumModules(G4double etot,
std::vector<G4double> G4BigBanger::generateMomentumModules(G4double etot,
G4double a,
G4double z,
G4double mp,
@@ -270,7 +270,7 @@ G4std::vector<G4double> G4BigBanger::generateMomentumModules(G4double etot,
G4int ia = int(a + 0.1);
G4int iz = int(z + 0.1);
G4std::vector<G4double> pmod;
std::vector<G4double> pmod;
G4double xtot = 0.0;
G4double promax = maxProbability(a);
source/processes/hadronic/models/cascade/cascade/src/G4CascadParticle.cc
+2 -2
View File
@@ -42,7 +42,7 @@ G4double G4CascadParticle::getPathToTheNextZone(G4double rz_in,
G4double rp = 0.0;
G4double rr = 0.0;
G4double pp = 0.0;
G4std::vector<G4double> mom = theParticle.getMomentum();
std::vector<G4double> mom = theParticle.getMomentum();
for (G4int i = 1; i < 4; i++) {
rp += mom[i] * position[i - 1];
@@ -87,7 +87,7 @@ void G4CascadParticle::propagateAlongThePath(G4double path) {
G4cout << " >>> G4CascadParticle::propagateAlongThePath" << G4endl;
}
G4std::vector<G4double> mom = theParticle.getMomentum();
std::vector<G4double> mom = theParticle.getMomentum();
G4double pmod = theParticle.getMomModule();
for(G4int i = 0; i < 3; i++) position[i] += mom[i + 1] * path / pmod;
source/processes/hadronic/models/cascade/cascade/src/G4CascadSpecialFunctions.cc
+8 -8
View File
@@ -22,7 +22,7 @@
#include "G4CascadSpecialFunctions.hh"
G4std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScale2(G4double e) {
std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScale2(G4double e) {
G4int verboseLevel = 2;
if (verboseLevel > 3) {
@@ -48,10 +48,10 @@
};
};
return G4std::pair<G4int, G4double>(ik, sk);
return std::pair<G4int, G4double>(ik, sk);
}
G4std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScale1(G4double e) {
std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScale1(G4double e) {
G4int verboseLevel = 2;
if (verboseLevel > 3) {
@@ -92,7 +92,7 @@ G4std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScale1
G4cout << " e " << e << " ik " << ik << " sk " << sk << G4endl;
}
return G4std::pair<G4int, G4double>(ik, sk);
return std::pair<G4int, G4double>(ik, sk);
}
G4double G4CascadSpecialFunctions::absorptionCrosSection(G4double e,
@@ -122,7 +122,7 @@ G4double G4CascadSpecialFunctions::absorptionCrosSection(G4double e,
return corr_fac * csec;
}
G4std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScaleEMS(G4double e) {
std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScaleEMS(G4double e) {
G4int verboseLevel = 2;
if (verboseLevel > 3) {
@@ -162,7 +162,7 @@ G4std::pair<G4int, G4double> G4CascadSpecialFunctions::getPositionInEnergyScaleE
sk = 1.0;
};
return G4std::pair<G4int, G4double>(ik, sk);
return std::pair<G4int, G4double>(ik, sk);
}
G4double G4CascadSpecialFunctions::crossSection(G4double e,
@@ -347,7 +347,7 @@ G4double G4CascadSpecialFunctions::crossSection(G4double e,
};
} else {
G4std::pair<G4int, G4double> iksk = getPositionInEnergyScaleEMS(e);
std::pair<G4int, G4double> iksk = getPositionInEnergyScaleEMS(e);
G4int ik = iksk.first;
G4double sk = iksk.second;
@@ -363,7 +363,7 @@ G4double G4CascadSpecialFunctions::crossSection(G4double e,
};
} else {
G4std::pair<G4int, G4double> iksk = getPositionInEnergyScale2(e);
std::pair<G4int, G4double> iksk = getPositionInEnergyScale2(e);
G4int ik = iksk.first;
G4double sk = iksk.second;
source/processes/hadronic/models/cascade/cascade/src/G4CascadeInterface.cc
+12 -12
View File
@@ -42,8 +42,8 @@
#include "G4LorentzRotation.hh"
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef G4std::vector<G4InuclNuclei>::iterator nucleiIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclNuclei>::iterator nucleiIterator;
G4CascadeInterface::G4CascadeInterface()
:verboseLevel(0) {
@@ -106,7 +106,7 @@ G4VParticleChange* G4CascadeInterface::ApplyYourself(const G4Track& aTrack,
toZ.rotateY(-projectileMomentum.theta());
G4LorentzRotation toLabFrame = toZ.inverse();
G4std::vector<G4double> momentumBullet(4);
std::vector<G4double> momentumBullet(4);
momentumBullet[0] =0.;
momentumBullet[1] =0;
momentumBullet[2] =0;
@@ -123,7 +123,7 @@ G4VParticleChange* G4CascadeInterface::ApplyYourself(const G4Track& aTrack,
G4InuclNuclei* target = NULL;
G4InuclParticle* targetH = NULL;
G4std::vector<G4double> targetMomentum(4, 0.0);
std::vector<G4double> targetMomentum(4, 0.0);
G4double theNucleusA = theNucleus.GetN();
@@ -135,9 +135,9 @@ G4VParticleChange* G4CascadeInterface::ApplyYourself(const G4Track& aTrack,
theNucleus.GetZ());
target->setEnergy();
G4std::vector<G4double> bmom = bullet->getMomentum();
std::vector<G4double> bmom = bullet->getMomentum();
eInit = sqrt(bmom[0] * bmom[0]);
G4std::vector<G4double> tmom = target->getMomentum();
std::vector<G4double> tmom = target->getMomentum();
eInit += sqrt(tmom[0] * tmom[0]);
sumBaryon += theNucleusA;
@@ -177,9 +177,9 @@ G4VParticleChange* G4CascadeInterface::ApplyYourself(const G4Track& aTrack,
sumBaryon += 1;
G4std::vector<G4double> bmom = bullet->getMomentum();
std::vector<G4double> bmom = bullet->getMomentum();
eInit = sqrt(bmom[0] * bmom[0]);
G4std::vector<G4double> tmom = targetH->getMomentum();
std::vector<G4double> tmom = targetH->getMomentum();
eInit += sqrt(tmom[0] * tmom[0]);
if (verboseLevel > 2) {
@@ -206,8 +206,8 @@ G4VParticleChange* G4CascadeInterface::ApplyYourself(const G4Track& aTrack,
// Convert cascade data to use hadronics interface
G4std::vector<G4InuclNuclei> nucleiFragments = output.getNucleiFragments();
G4std::vector<G4InuclElementaryParticle> particles = output.getOutgoingParticles();
std::vector<G4InuclNuclei> nucleiFragments = output.getNucleiFragments();
std::vector<G4InuclElementaryParticle> particles = output.getOutgoingParticles();
G4int numSecondaries = nucleiFragments.size()+particles.size();
theResult.SetStatusChange(fStopAndKill);
@@ -219,7 +219,7 @@ G4VParticleChange* G4CascadeInterface::ApplyYourself(const G4Track& aTrack,
for (ipart = particles.begin(); ipart != particles.end(); ipart++) {
outgoingParticle = ipart->type();
G4std::vector<G4double> mom = ipart->getMomentum();
std::vector<G4double> mom = ipart->getMomentum();
eTot += sqrt(mom[0] * mom[0]);
G4double ekin = ipart->getKineticEnergy() * GeV;
@@ -305,7 +305,7 @@ G4VParticleChange* G4CascadeInterface::ApplyYourself(const G4Track& aTrack,
for (ifrag = nucleiFragments.begin(); ifrag != nucleiFragments.end(); ifrag++)
{
G4double eKin = ifrag->getKineticEnergy() * GeV;
G4std::vector<G4double> mom = ifrag->getMomentum();
std::vector<G4double> mom = ifrag->getMomentum();
eTot += sqrt(mom[0] * mom[0]);
G4ThreeVector aMom(mom[1], mom[2], mom[3]);
source/processes/hadronic/models/cascade/cascade/src/G4CollisionOutput.cc
+19 -19
View File
@@ -22,9 +22,9 @@
#include "G4CollisionOutput.hh"
#include "G4ParticleLargerEkin.hh"
#include "g4std/algorithm"
#include <algorithm>
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
G4CollisionOutput::G4CollisionOutput()
: verboseLevel(0) {
@@ -45,14 +45,14 @@ void G4CollisionOutput::setOnShell(G4InuclParticle* bullet,
on_shell = false;
G4std::vector<G4double> ini_mom = bullet->getMomentum();
G4std::vector<G4double> momt = target->getMomentum();
std::vector<G4double> ini_mom = bullet->getMomentum();
std::vector<G4double> momt = target->getMomentum();
G4int i;
for(i = 0; i < 4; i++) ini_mom[i] += momt[i];
G4std::vector<G4double> out_mom = getTotalOutputMomentum();
G4std::vector<G4double> mon_non_cons(4);
std::vector<G4double> out_mom = getTotalOutputMomentum();
std::vector<G4double> mon_non_cons(4);
if(verboseLevel > 2){
G4cout << " bullet momentum = " << ini_mom[0]<<", "<< ini_mom[1]<<", "<< ini_mom[2]<<", "<< ini_mom[3]<<G4endl;
G4cout << " target momentum = " << momt[0]<<", "<< momt[1]<<", "<< momt[2]<<", "<< momt[3]<<G4endl;
@@ -80,7 +80,7 @@ void G4CollisionOutput::setOnShell(G4InuclParticle* bullet,
if(npart > 0) {
G4std::vector<G4double> last_mom = outgoingParticles[npart - 1].getMomentum();
std::vector<G4double> last_mom = outgoingParticles[npart - 1].getMomentum();
for(G4int i = 1; i < 4; i++) last_mom[i] += mon_non_cons[i];
outgoingParticles[npart - 1].setMomentum(last_mom);
@@ -91,7 +91,7 @@ void G4CollisionOutput::setOnShell(G4InuclParticle* bullet,
if(nnuc > 0) {
G4std::vector<G4double> last_mom = nucleiFragments[nnuc - 1].getMomentum();
std::vector<G4double> last_mom = nucleiFragments[nnuc - 1].getMomentum();
for(G4int i = 1; i < 4; i++) last_mom[i] += mon_non_cons[i];
nucleiFragments[nnuc - 1].setMomentum(last_mom);
@@ -130,8 +130,8 @@ void G4CollisionOutput::setOnShell(G4InuclParticle* bullet,
if(need_hard_tuning) {
G4std::pair<G4std::pair<G4int, G4int>, G4int> tune_par = selectPairToTune(mon_non_cons[0]);
G4std::pair<G4int, G4int> tune_particles = tune_par.first;
std::pair<std::pair<G4int, G4int>, G4int> tune_par = selectPairToTune(mon_non_cons[0]);
std::pair<G4int, G4int> tune_particles = tune_par.first;
G4int mom_ind = tune_par.second;
if(verboseLevel > 2) {
@@ -141,8 +141,8 @@ void G4CollisionOutput::setOnShell(G4InuclParticle* bullet,
if(tune_particles.first >= 0 && tune_particles.second >= 0 &&
mom_ind >= 1) { // tunning possible
G4std::vector<G4double> mom1 = outgoingParticles[tune_particles.first].getMomentum();
G4std::vector<G4double> mom2 = outgoingParticles[tune_particles.second].getMomentum();
std::vector<G4double> mom1 = outgoingParticles[tune_particles.first].getMomentum();
std::vector<G4double> mom2 = outgoingParticles[tune_particles.second].getMomentum();
G4double newE12 = mom1[0] + mom2[0] + mon_non_cons[0];
G4double R = 0.5 * (newE12 * newE12 + mom2[0] * mom2[0] - mom1[0] * mom1[0]) / newE12;
G4double Q = -(mom1[mom_ind] + mom2[mom_ind]) / newE12;
@@ -193,7 +193,7 @@ void G4CollisionOutput::setOnShell(G4InuclParticle* bullet,
outgoingParticles[tune_particles.first ].setMomentum(mom1);
outgoingParticles[tune_particles.second].setMomentum(mom2);
out_mom = getTotalOutputMomentum();
G4std::sort(outgoingParticles.begin(), outgoingParticles.end(), G4ParticleLargerEkin());
std::sort(outgoingParticles.begin(), outgoingParticles.end(), G4ParticleLargerEkin());
for(G4int i = 0; i < 4; i++) mon_non_cons[i] = ini_mom[i] - out_mom[i];
pnc = sqrt(mon_non_cons[1] * mon_non_cons[1] +
mon_non_cons[2] * mon_non_cons[2] +
@@ -232,15 +232,15 @@ void G4CollisionOutput::setOnShell(G4InuclParticle* bullet,
}
G4std::pair<G4std::pair<G4int, G4int>, G4int> G4CollisionOutput::selectPairToTune(G4double de) const {
std::pair<std::pair<G4int, G4int>, G4int> G4CollisionOutput::selectPairToTune(G4double de) const {
if (verboseLevel > 3) {
G4cout << " >>> G4CollisionOutput::selectPairToTune" << G4endl;
}
G4std::pair<G4int, G4int> tup(-1, -1);
std::pair<G4int, G4int> tup(-1, -1);
G4int i3 = -1;
G4std::pair<G4std::pair<G4int, G4int>, G4int> badp(tup, i3);
std::pair<std::pair<G4int, G4int>, G4int> badp(tup, i3);
if(outgoingParticles.size() < 2) {
@@ -257,11 +257,11 @@ G4std::pair<G4std::pair<G4int, G4int>, G4int> G4CollisionOutput::selectPairToTun
for(G4int i = 0; i < G4int(outgoingParticles.size()) - 1; i++) {
G4std::vector<G4double> mom1 = outgoingParticles[i].getMomentum();
std::vector<G4double> mom1 = outgoingParticles[i].getMomentum();
for(G4int j = i+1; j < G4int(outgoingParticles.size()); j++) {
G4std::vector<G4double> mom2 = outgoingParticles[j].getMomentum();
std::vector<G4double> mom2 = outgoingParticles[j].getMomentum();
for(G4int l = 1; l < 4; l++) {
if(mom1[l] * mom2[l] < 0.0) {
@@ -304,7 +304,7 @@ G4std::pair<G4std::pair<G4int, G4int>, G4int> G4CollisionOutput::selectPairToTun
};
};
return G4std::pair<G4std::pair<G4int, G4int>, G4int>(tup, i3);
return std::pair<std::pair<G4int, G4int>, G4int>(tup, i3);
};
};
source/processes/hadronic/models/cascade/cascade/src/G4ElementaryParticleCollider.cc
+55 -55
View File
@@ -23,9 +23,9 @@
#include "G4Collider.hh"
#include "G4ElementaryParticleCollider.hh"
#include "G4ParticleLargerEkin.hh"
#include "g4std/algorithm"
#include <algorithm>
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
G4ElementaryParticleCollider::G4ElementaryParticleCollider()
: verboseLevel(1) {
@@ -43,8 +43,8 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
G4cout << " >>> G4ElementaryParticleCollider::collide" << G4endl;
}
G4std::vector<G4double> totscm(4, 0.0); //::: fix
G4std::vector<G4double> totlab(4, 0.0);
std::vector<G4double> totscm(4, 0.0); //::: fix
std::vector<G4double> totlab(4, 0.0);
// generate nucleon or pion collission with NUCLEON
// or pion with quasideutron
@@ -70,8 +70,8 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
particle1->printParticle();
particle2->printParticle();
G4std::vector<G4double> momb = particle1->getMomentum();
G4std::vector<G4double> momt = particle2->getMomentum();
std::vector<G4double> momb = particle1->getMomentum();
std::vector<G4double> momt = particle2->getMomentum();
for(G4int i = 0; i < 4; i++) momb[i] += momt[i];
G4cout << " total input: px " << momb[1] << " py " << momb[2]
@@ -102,7 +102,7 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
pscm << G4endl;
}
G4std::vector<G4InuclElementaryParticle> particles =
std::vector<G4InuclElementaryParticle> particles =
generateSCMfinalState(ekin, etot_scm, pscm, particle1, particle2, &convertToSCM);
if(verboseLevel > 2){
@@ -120,7 +120,7 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
for(ipart = particles.begin(); ipart != particles.end(); ipart++) {
if(verboseLevel > 2){
G4std::vector<G4double> mom_scm = ipart->getMomentum();
std::vector<G4double> mom_scm = ipart->getMomentum();
G4cout << mom_scm[0] << " " << mom_scm[1] << " "
<< mom_scm[2] << " " << mom_scm[3] << G4endl;
@@ -131,7 +131,7 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
}
G4std::vector<G4double> mom =
std::vector<G4double> mom =
convertToSCM.backToTheLab(ipart->getMomentum());
if(verboseLevel > 2){
@@ -141,7 +141,7 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
ipart->setMomentum(mom);
};
G4std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
if(verboseLevel > 2){
G4cout << " In SCM: total outgoing momentum " << G4endl
@@ -180,7 +180,7 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
G4cout << " etot_scm " << etot_scm << G4endl;
}
G4std::vector<G4InuclElementaryParticle> particles =
std::vector<G4InuclElementaryParticle> particles =
generateSCMpionAbsorption(etot_scm, particle1, particle2);
if(verboseLevel > 2){
@@ -197,19 +197,19 @@ G4CollisionOutput G4ElementaryParticleCollider::collide(G4InuclParticle* bullet
for(ipart = particles.begin(); ipart != particles.end(); ipart++) {
if(verboseLevel > 2){
G4std::vector<G4double> mom_scm = ipart->getMomentum();
std::vector<G4double> mom_scm = ipart->getMomentum();
for(G4int i = 0; i < 4; i++) totscm[i] += mom_scm[i];
}
G4std::vector<G4double> mom =
std::vector<G4double> mom =
convertToSCM.backToTheLab(ipart->getMomentum());
ipart->setMomentum(mom);
};
G4std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
if(verboseLevel > 2){
G4cout << " In SCM: total outgoing momentum " << G4endl
@@ -350,7 +350,7 @@ G4int G4ElementaryParticleCollider::generateMultiplicity(G4int is,
};
const G4double large_cut = 4.0;
G4std::pair<G4int, G4double> iksk = getPositionInEnergyScale2(ekin);
std::pair<G4int, G4double> iksk = getPositionInEnergyScale2(ekin);
G4int ik = iksk.first;
G4double sk = iksk.second;
G4int l = is;
@@ -359,7 +359,7 @@ G4int G4ElementaryParticleCollider::generateMultiplicity(G4int is,
if (l == 10) l = 3;
if (l == 5 || l == 6) l = 4;
G4std::vector<G4double> sigm(5);
std::vector<G4double> sigm(5);
G4double stot = 0.0;
if (l == 7 || l == 14) { // pi0 P or pi0 N
@@ -404,7 +404,7 @@ G4int G4ElementaryParticleCollider::generateMultiplicity(G4int is,
return mul + 2;
}
G4std::vector<G4InuclElementaryParticle> G4ElementaryParticleCollider::
std::vector<G4InuclElementaryParticle> G4ElementaryParticleCollider::
generateSCMfinalState(G4double ekin,
G4double etot_scm,
G4double pscm,
@@ -420,8 +420,8 @@ generateSCMfinalState(G4double ekin,
const G4double difr_const = 0.3678794;
const G4int itry_max = 10;
G4InuclElementaryParticle dummy;
G4std::vector<G4InuclElementaryParticle> particles;
G4std::vector<G4int> particle_kinds;
std::vector<G4InuclElementaryParticle> particles;
std::vector<G4int> particle_kinds;
G4int type1 = particle1->type();
G4int type2 = particle2->type();
G4int is = type1 * type2;
@@ -487,7 +487,7 @@ generateSCMfinalState(G4double ekin,
particle_kinds.push_back(type2);
};
G4std::vector<G4double> mom;
std::vector<G4double> mom;
if (kw == 2) { // need to rescale momentum
G4double m1 = dummy.getParticleMass(particle_kinds[0]);
@@ -514,7 +514,7 @@ generateSCMfinalState(G4double ekin,
G4cout << " after rotation px " << mom[1] << " py " << mom[2] <<
" pz " << mom[3] << G4endl;
}
G4std::vector<G4double> mom1(4);
std::vector<G4double> mom1(4);
for (G4int i = 1; i < 4; i++) mom1[i] = -mom[i];
@@ -542,13 +542,13 @@ generateSCMfinalState(G4double ekin,
G4cout << " itry in while " << itry << G4endl;
}
G4std::vector<G4double> modules =
std::vector<G4double> modules =
generateMomModules(particle_kinds, multiplicity, is, ekin, etot_scm);
if (G4int(modules.size()) == multiplicity) {
if (multiplicity == 3) {
G4std::vector<G4double> mom3 =
std::vector<G4double> mom3 =
particleSCMmomentumFor2to3(is, knd_last, ekin, modules[2]);
mom3 = toSCM->rotate(mom3);
@@ -565,11 +565,11 @@ generateSCMfinalState(G4double ekin,
G4cout << " ok for mult " << multiplicity << G4endl;
}
G4std::vector<G4double> mom1 = generateWithFixedTheta(ct, modules[0]);
std::vector<G4double> mom1 = generateWithFixedTheta(ct, modules[0]);
mom1 = toSCM->rotate(mom3, mom1);
G4std::vector<G4double> mom2(4);
std::vector<G4double> mom2(4);
for(G4int i = 1; i < 4; i++) mom2[i] = - (mom3[i] + mom1[i]);
@@ -584,8 +584,8 @@ generateSCMfinalState(G4double ekin,
} else { // multiplicity > 3
// generate first mult - 2 momentums
G4std::vector<G4std::vector<G4double> > scm_momentums;
G4std::vector<G4double> tot_mom(4);
std::vector<std::vector<G4double> > scm_momentums;
std::vector<G4double> tot_mom(4);
for (G4int i = 0; i < multiplicity - 2; i++) {
G4double p0 = particle_kinds[i] < 3 ? 0.36 : 0.25;
@@ -628,7 +628,7 @@ generateSCMfinalState(G4double ekin,
G4double pt = modules[i]*st;
G4double phi = randomPHI();
G4std::vector<G4double> mom(4);
std::vector<G4double> mom(4);
mom[1] = pt * cos(phi);
mom[2] = pt * sin(phi);
@@ -659,14 +659,14 @@ generateSCMfinalState(G4double ekin,
tot_mom = toSCM->rotate(tot_mom);
G4std::vector<G4double> mom =
std::vector<G4double> mom =
generateWithFixedTheta(ct, modules[multiplicity - 2]);
mom = toSCM->rotate(tot_mom, mom);
scm_momentums.push_back(mom);
// and the last one
G4std::vector<G4double> mom1(4);
std::vector<G4double> mom1(4);
for (i = 1; i < 4; i++) mom1[i] = -mom[i] - tot_mom[i];
@@ -705,9 +705,9 @@ generateSCMfinalState(G4double ekin,
return particles;
}
G4std::vector<G4double> G4ElementaryParticleCollider::
std::vector<G4double> G4ElementaryParticleCollider::
generateMomModules(
const G4std::vector<G4int>& kinds,
const std::vector<G4int>& kinds,
G4int mult,
G4int is,
G4double ekin,
@@ -727,8 +727,8 @@ generateMomModules(
G4InuclElementaryParticle dummy;
G4int itry = 0;
G4std::vector<G4double> modules(mult);
G4std::vector<G4double> masses2(mult);
std::vector<G4double> modules(mult);
std::vector<G4double> masses2(mult);
for (G4int i = 0; i < mult; i++) {
G4double mass = dummy.getParticleMass(kinds[i]);
@@ -801,7 +801,7 @@ generateMomModules(
}
G4bool G4ElementaryParticleCollider::satisfyTriangle(
const G4std::vector<G4double>& modules) const {
const std::vector<G4double>& modules) const {
if (verboseLevel > 3) {
G4cout << " >>> G4ElementaryParticleCollider::satisfyTriangle" << G4endl;
@@ -852,7 +852,7 @@ G4int G4ElementaryParticleCollider::getIL(G4int is,
return ifdef[mult - 3][l - 1];
}
G4std::vector<G4int> G4ElementaryParticleCollider::
std::vector<G4int> G4ElementaryParticleCollider::
generateOutgoingKindsFor2toMany(
G4int is,
G4int mult,
@@ -1085,7 +1085,7 @@ generateOutgoingKindsFor2toMany(
{0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0}}
};
G4std::vector<G4int> kinds;
std::vector<G4int> kinds;
G4int l = is;
@@ -1102,7 +1102,7 @@ generateOutgoingKindsFor2toMany(
};
G4int il = getIL(is, mult);
G4std::pair<G4int, G4double> iksk = getPositionInEnergyScale1(ekin);
std::pair<G4int, G4double> iksk = getPositionInEnergyScale1(ekin);
G4int ik = iksk.first;
G4double sk = iksk.second;
G4int n;
@@ -1130,7 +1130,7 @@ generateOutgoingKindsFor2toMany(
n = 13;
};
G4std::vector<G4double> sig;
std::vector<G4double> sig;
G4double stot = 0.0;
if(l == 7 || l == 14) {
@@ -1303,7 +1303,7 @@ G4double G4ElementaryParticleCollider::getMomModuleFor2toMany(
return fabs(PRA);
}
G4std::vector<G4double> G4ElementaryParticleCollider::
std::vector<G4double> G4ElementaryParticleCollider::
particleSCMmomentumFor2to3(
G4int is,
G4int knd,
@@ -1367,7 +1367,7 @@ particleSCMmomentumFor2to3(
G4double pt = pmod * sqrt(1.0 - ct * ct);
G4double phi = randomPHI();
G4std::vector<G4double> mom(4);
std::vector<G4double> mom(4);
mom[1] = pt * cos(phi);
mom[2] = pt * sin(phi);
@@ -1490,7 +1490,7 @@ G4bool G4ElementaryParticleCollider::reChargering(G4double ekin,
G4bool rech = false;
if (is == 6 || is == 5 || is == 7 || is == 14) {
G4std::pair<G4int, G4double> iksk = getPositionInEnergyScale2(ekin);
std::pair<G4int, G4double> iksk = getPositionInEnergyScale2(ekin);
G4int ik = iksk.first;
G4double sk = iksk.second;
G4double chrg;
@@ -1509,14 +1509,14 @@ G4bool G4ElementaryParticleCollider::reChargering(G4double ekin,
return rech;
}
G4std::pair<G4double, G4double> G4ElementaryParticleCollider::
std::pair<G4double, G4double> G4ElementaryParticleCollider::
adjustIntervalForElastic(
G4double ekin,
G4double ak,
G4double ae,
G4int k,
G4int l,
const G4std::vector<G4double>& ssv,
const std::vector<G4double>& ssv,
G4double st) const {
if (verboseLevel > 3) {
@@ -1645,10 +1645,10 @@ adjustIntervalForElastic(
};
};
return G4std::pair<G4double, G4double>(a, b);
return std::pair<G4double, G4double>(a, b);
}
G4std::vector<G4double> G4ElementaryParticleCollider::
std::vector<G4double> G4ElementaryParticleCollider::
particleSCMmomentumFor2to2(
G4int is,
G4int kw,
@@ -1727,7 +1727,7 @@ particleSCMmomentumFor2to2(
G4int k1 = k - 1;
// first set all coefficients
G4std::vector<G4double> ssv(4);
std::vector<G4double> ssv(4);
G4double st = 0.0;
for(G4int i = 0; i < 4; i++) {
@@ -1742,7 +1742,7 @@ particleSCMmomentumFor2to2(
G4double b = 0.0;
if(k <= 3) {
G4std::pair<G4double, G4double> ab = adjustIntervalForElastic(ekin, ak, ae, k, is, ssv, st);
std::pair<G4double, G4double> ab = adjustIntervalForElastic(ekin, ak, ae, k, is, ssv, st);
a = ab.first;
b = ab.second;
@@ -1771,7 +1771,7 @@ particleSCMmomentumFor2to2(
G4double pt = pscm * sqrt(1.0 - ct * ct);
G4double phi = randomPHI();
G4std::vector<G4double> mom(4);
std::vector<G4double> mom(4);
mom[1] = pt * cos(phi);
mom[2] = pt * sin(phi);
@@ -1870,7 +1870,7 @@ G4int G4ElementaryParticleCollider::getElasticCase(G4int is,
return k;
}
G4std::vector<G4InuclElementaryParticle> G4ElementaryParticleCollider::
std::vector<G4InuclElementaryParticle> G4ElementaryParticleCollider::
generateSCMpionAbsorption(G4double etot_scm,
G4InuclElementaryParticle* particle1,
G4InuclElementaryParticle* particle2) const {
@@ -1883,8 +1883,8 @@ generateSCMpionAbsorption(G4double etot_scm,
// the nucleon distribution assumed to be isotropic in SCM
G4InuclElementaryParticle dummy;
G4std::vector<G4InuclElementaryParticle> particles;
G4std::vector<G4int> particle_kinds;
std::vector<G4InuclElementaryParticle> particles;
std::vector<G4int> particle_kinds;
G4int type1 = particle1->type();
G4int type2 = particle2->type();
@@ -1949,8 +1949,8 @@ generateSCMpionAbsorption(G4double etot_scm,
G4double a = 0.5 * (etot_scm * etot_scm - m1 - m2);
G4double pmod = sqrt((a * a - m1 * m2) / (m1 + m2 + 2.0 * a));
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double pt = pmod * COS_SIN.second;
@@ -1958,7 +1958,7 @@ generateSCMpionAbsorption(G4double etot_scm,
mom[2] = pt * sin(FI);
mom[3] = pmod * COS_SIN.first;
G4std::vector<G4double> mom1 = mom;
std::vector<G4double> mom1 = mom;
for(G4int i = 1; i < 4; i++) mom1[i] *= -1.0;
particles.push_back(G4InuclElementaryParticle(mom , particle_kinds[0]));
source/processes/hadronic/models/cascade/cascade/src/G4EquilibriumEvaporator.cc
+30 -30
View File
@@ -65,12 +65,12 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
const G4double small_ekin = 1.0e-6;
const G4int itry_gam_max = 100;
G4std::vector<G4double> W(8);
G4std::vector<G4double> A1(6);
G4std::vector<G4double> Z1(6);
G4std::vector<G4double> u(6);
G4std::vector<G4double> V(6);
G4std::vector<G4double> TM(6);
std::vector<G4double> W(8);
std::vector<G4double> A1(6);
std::vector<G4double> Z1(6);
std::vector<G4double> u(6);
std::vector<G4double> V(6);
std::vector<G4double> TM(6);
G4double coul_coeff;
G4CollisionOutput output;
@@ -78,7 +78,7 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
if (G4InuclNuclei* nuclei_target = dynamic_cast<G4InuclNuclei*>(target)) {
G4double A = nuclei_target->getA();
G4double Z = nuclei_target->getZ();
G4std::vector<G4double> PEX = nuclei_target->getMomentum();
std::vector<G4double> PEX = nuclei_target->getMomentum();
G4double EEXS = nuclei_target->getExitationEnergy();
if (verboseLevel > 3) {
@@ -88,7 +88,7 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
G4InuclElementaryParticle dummy(small_ekin, 1);
G4LorentzConvertor toTheNucleiSystemRestFrame;
toTheNucleiSystemRestFrame.setBullet(dummy.getMomentum(), dummy.getMass());
G4std::vector<G4double> ppout(4, 0.0);
std::vector<G4double> ppout(4, 0.0);
if (timeToBigBang(A, Z, EEXS)) {
@@ -109,7 +109,7 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
G4InuclNuclei dummy_nuc;
G4double EEXS_new;
G4std::vector<G4double> pin = PEX;
std::vector<G4double> pin = PEX;
pin[0] += 0.001 * EEXS;
G4bool try_again = true;
G4bool fission_open = true;
@@ -154,9 +154,9 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
G4double E0 = getE0(A);
G4double parlev = getPARLEVDEN(A, Z);
G4double u1 = parlev * A;
G4std::pair<G4std::vector<G4double>, G4std::vector<G4double> > parms = paraMaker(Z);
G4std::vector<G4double> AK = parms.first;
G4std::vector<G4double> CPA = parms.second;
std::pair<std::vector<G4double>, std::vector<G4double> > parms = paraMaker(Z);
std::vector<G4double> AK = parms.first;
std::vector<G4double> CPA = parms.second;
G4double DM0 = bindingEnergy(A, Z);
G4int i(0);
@@ -281,15 +281,15 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
// new photon escape
G4InuclElementaryParticle particle(10);
G4double pmod = 0.001 * S;
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double P1 = pmod * COS_SIN.second;
mom[1] = P1 * cos(FI);
mom[2] = P1 * sin(FI);
mom[3] = pmod * COS_SIN.first;
mom[0] = pmod;
G4std::vector<G4double> mom_at_rest(4);
std::vector<G4double> mom_at_rest(4);
for (G4int i = 1; i < 4; i++) mom_at_rest[i] = -mom[i];
mom_at_rest[0] = sqrt(mom_at_rest[1] * mom_at_rest[1] +
@@ -297,14 +297,14 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
mom_at_rest[3] * mom_at_rest[3] +
nuc_mass * nuc_mass);
G4std::vector<G4double> part_mom =
std::vector<G4double> part_mom =
toTheNucleiSystemRestFrame.backToTheLab(mom);
part_mom[0] = sqrt(part_mom[1] * part_mom[1] +
part_mom[2] * part_mom[2] +
part_mom[3] * part_mom[3]);
G4std::vector<G4double> ex_mom =
std::vector<G4double> ex_mom =
toTheNucleiSystemRestFrame.backToTheLab(mom_at_rest);
ex_mom[0] = sqrt(ex_mom[1] * ex_mom[1] +
@@ -377,14 +377,14 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
G4double mass = particle.getMass();
// generate particle momentum
G4double pmod = sqrt((2.0 * mass + S) * S);
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double P1 = pmod * COS_SIN.second;
mom[1] = P1 * cos(FI);
mom[2] = P1 * sin(FI);
mom[3] = pmod * COS_SIN.first;
G4std::vector<G4double> mom_at_rest(4);
std::vector<G4double> mom_at_rest(4);
for (G4int i = 1; i < 4; i++) mom_at_rest[i] = -mom[i];
G4double new_nuc_mass = dummy_nuc.getNucleiMass(A1[icase],
@@ -396,13 +396,13 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
mom[0] = sqrt(mom[1] * mom[1] + mom[2] * mom[2] +
mom[3] * mom[3] + mass * mass);
G4std::vector<G4double> part_mom =
std::vector<G4double> part_mom =
toTheNucleiSystemRestFrame.backToTheLab(mom);
part_mom[0] = sqrt(part_mom[1] * part_mom[1] +
part_mom[2] * part_mom[2] +
part_mom[3] * part_mom[3] +
mass * mass);
G4std::vector<G4double> ex_mom =
std::vector<G4double> ex_mom =
toTheNucleiSystemRestFrame.backToTheLab(mom_at_rest);
ex_mom[0] = sqrt(ex_mom[1] * ex_mom[1] +
ex_mom[2] * ex_mom[2] +
@@ -428,14 +428,14 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
G4double mass = nuclei.getMass();
// generate particle momentum
G4double pmod = sqrt((2.0 * mass + S) * S);
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double P1 = pmod * COS_SIN.second;
mom[1] = P1 * cos(FI);
mom[2] = P1 * sin(FI);
mom[3] = pmod * COS_SIN.first;
G4std::vector<G4double> mom_at_rest(4);
std::vector<G4double> mom_at_rest(4);
for (G4int i = 1; i < 4; i++) mom_at_rest[i] = -mom[i];
G4double new_nuc_mass = dummy_nuc.getNucleiMass(A1[icase],
@@ -448,13 +448,13 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
mom[2] * mom[2] +
mom[3] * mom[3] +
mass * mass);
G4std::vector<G4double> part_mom =
std::vector<G4double> part_mom =
toTheNucleiSystemRestFrame.backToTheLab(mom);
part_mom[0] = sqrt(part_mom[1] * part_mom[1] +
part_mom[2] * part_mom[2] +
part_mom[3] * part_mom[3] +
mass * mass);
G4std::vector<G4double> ex_mom =
std::vector<G4double> ex_mom =
toTheNucleiSystemRestFrame.backToTheLab(mom_at_rest);
ex_mom[0] = sqrt(ex_mom[1] * ex_mom[1] +
ex_mom[2] * ex_mom[2] +
@@ -492,13 +492,13 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
}
G4CollisionOutput foutput = theFissioner->collide(0, &nuclei);
G4std::vector<G4InuclNuclei> nuclea = foutput.getNucleiFragments();
std::vector<G4InuclNuclei> nuclea = foutput.getNucleiFragments();
if (nuclea.size() == 2) { // fission o'k
// convert back to the lab
for(G4int i = 0; i < 2; i++) {
G4std::vector<G4double> mom = nuclea[i].getMomentum();
std::vector<G4double> mom = nuclea[i].getMomentum();
mom = toTheNucleiSystemRestFrame.backToTheLab(mom);
nuclea[i].setMomentum(mom);
nuclea[i].setEnergy();
@@ -537,7 +537,7 @@ G4CollisionOutput G4EquilibriumEvaporator::collide(G4InuclParticle* bullet,
}
G4std::vector<G4double> pnuc(4);
std::vector<G4double> pnuc(4);
for (G4int i = 1; i < 4; i++) pnuc[i] = pin[i] - ppout[i];
source/processes/hadronic/models/cascade/cascade/src/G4FissionStore.cc
+1 -1
View File
@@ -41,7 +41,7 @@ G4FissionConfiguration G4FissionStore::generateConfiguration(G4double amax,
const G4double small = -30.0;
G4double totProb = 0.0;
G4std::vector<G4double> probs(configurations.size());
std::vector<G4double> probs(configurations.size());
// G4cout << " amax " << amax << " ic " << configurations.size() << G4endl;
source/processes/hadronic/models/cascade/cascade/src/G4Fissioner.cc
+9 -9
View File
@@ -77,8 +77,8 @@ G4CollisionOutput G4Fissioner::collide(G4InuclParticle* bullet,
TEM += DTEM;
G4std::vector<G4double> AL1(2, -0.15);
G4std::vector<G4double> BET1(2, 0.05);
std::vector<G4double> AL1(2, -0.15);
std::vector<G4double> BET1(2, 0.05);
G4FissionStore fissionStore;
G4double R12 = pow(A1, one_third) + pow(A2, one_third);
@@ -88,7 +88,7 @@ G4CollisionOutput G4Fissioner::collide(G4InuclParticle* bullet,
G4double X3 = 1.0 / pow(A1, one_third);
G4double X4 = 1.0 / pow(A2, one_third);
Z1 = G4int(getZopt(A1, A2, Z, X3, X4, R12)) - 1.0;
G4std::vector<G4double> EDEF1(2);
std::vector<G4double> EDEF1(2);
G4double Z2 = Z - Z1;
G4double VPOT, VCOUL;
@@ -140,11 +140,11 @@ G4CollisionOutput G4Fissioner::collide(G4InuclParticle* bullet,
G4double mass2 = nuclei2.getMass();
G4double EK = config.ekin;
G4double pmod = sqrt(0.001 * EK * mass1 * mass2 / mass_in);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double Fi = randomPHI();
G4double P1 = pmod * COS_SIN.second;
G4std::vector<G4double> mom1(4);
G4std::vector<G4double> mom2(4);
std::vector<G4double> mom1(4);
std::vector<G4double> mom2(4);
mom1[1] = P1 * cos(Fi);
mom1[2] = P1 * sin(Fi);
@@ -220,14 +220,14 @@ G4double G4Fissioner::getZopt(G4double A1,
}
void G4Fissioner::potentialMinimization(G4double& VP,
G4std::vector<G4double> & ED,
std::vector<G4double> & ED,
G4double& VC,
G4double AF,
G4double AS,
G4double ZF,
G4double ZS,
G4std::vector<G4double>& AL1,
G4std::vector<G4double>& BET1,
std::vector<G4double>& AL1,
std::vector<G4double>& BET1,
G4double& R12) const {
if (verboseLevel > 3) {
source/processes/hadronic/models/cascade/cascade/src/G4IntraNucleiCascader.cc
+13 -13
View File
@@ -28,9 +28,9 @@
#include "G4ParticleLargerEkin.hh"
#include "G4NucleiModel.hh"
#include "G4CascadParticle.hh"
#include "g4std/algorithm"
#include <algorithm>
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
G4IntraNucleiCascader::G4IntraNucleiCascader()
: verboseLevel(1) {
@@ -64,7 +64,7 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
G4InuclNuclei* bnuclei = dynamic_cast<G4InuclNuclei*>(bullet);
G4InuclElementaryParticle* bparticle = dynamic_cast<G4InuclElementaryParticle*>(bullet);
G4NucleiModel model(tnuclei);
G4std::vector<G4double> momentum_in = bullet->getMomentum();
std::vector<G4double> momentum_in = bullet->getMomentum();
momentum_in[0] += tnuclei->getMass();
@@ -82,9 +82,9 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
itry++;
model.reset();
G4std::vector<G4CascadParticle> cascad_particles;
std::vector<G4CascadParticle> cascad_particles;
G4ExitonConfiguration theExitonConfiguration;
G4std::vector<G4InuclElementaryParticle> output_particles;
std::vector<G4InuclElementaryParticle> output_particles;
G4double afin = tnuclei->getA();
G4double zfin = tnuclei->getZ();
@@ -104,7 +104,7 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
afin += ab;
zfin += zb;
G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
all_particles = model.initializeCascad(bnuclei, tnuclei);
cascad_particles = all_particles.first;
@@ -131,7 +131,7 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
};
};
G4std::vector<G4CascadParticle> new_cascad_particles;
std::vector<G4CascadParticle> new_cascad_particles;
G4int iloop = 0;
while (!cascad_particles.empty() && !model.empty()) {
@@ -194,7 +194,7 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
for (G4int i = 0; i < G4int(new_cascad_particles.size()); i++)
cascad_particles.push_back(new_cascad_particles[i]);
G4std::pair<G4int, G4int> holes = model.getTypesOfNucleonsInvolved();
std::pair<G4int, G4int> holes = model.getTypesOfNucleonsInvolved();
theExitonConfiguration.incrementHoles(holes.first);
@@ -210,12 +210,12 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
<< " output_particles " << output_particles.size() << G4endl;
}
G4std::vector<G4double> momentum_out(4, 0.0);
std::vector<G4double> momentum_out(4, 0.0);
particleIterator ipart;
for (ipart = output_particles.begin(); ipart != output_particles.end(); ipart++) {
G4std::vector<G4double> mom = ipart->getMomentum();
std::vector<G4double> mom = ipart->getMomentum();
for (G4int j = 0; j < 4; j++) momentum_out[j] += mom[j];
@@ -253,7 +253,7 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
}
if (goodCase(afin, zfin, Eex, ekin_in)) { // ok, exitation energy > cut
G4std::sort(output_particles.begin(), output_particles.end(), G4ParticleLargerEkin());
std::sort(output_particles.begin(), output_particles.end(), G4ParticleLargerEkin());
output.addOutgoingParticles(output_particles);
outgoing_nuclei.setMomentum(momentum_out);
outgoing_nuclei.setEnergy();
@@ -285,7 +285,7 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
output_particles.push_back(last_particle);
};
G4std::sort(output_particles.begin(), output_particles.end(), G4ParticleLargerEkin());
std::sort(output_particles.begin(), output_particles.end(), G4ParticleLargerEkin());
output.addOutgoingParticles(output_particles);
return output;
@@ -296,7 +296,7 @@ G4CollisionOutput G4IntraNucleiCascader::collide(G4InuclParticle* bullet,
// special branch to avoid the cascad generation but to get the input for evaporation etc
G4std::vector<G4double> momentum_out(4, 0.0);
std::vector<G4double> momentum_out(4, 0.0);
G4InuclNuclei outgoing_nuclei(169, 69);
outgoing_nuclei.setMomentum(momentum_out);
source/processes/hadronic/models/cascade/cascade/src/G4InuclCollider.cc
+10 -10
View File
@@ -24,10 +24,10 @@
#include "G4InuclElementaryParticle.hh"
#include "G4LorentzConvertor.hh"
#include "G4ParticleLargerEkin.hh"
#include "g4std/algorithm"
#include <algorithm>
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef G4std::vector<G4InuclNuclei>::iterator nucleiIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclNuclei>::iterator nucleiIterator;
G4InuclCollider::G4InuclCollider()
: verboseLevel(2) {
@@ -122,12 +122,12 @@ G4CollisionOutput G4InuclCollider::collide(G4InuclParticle* bullet,
G4cout << " degenerated? " << convertToTargetRestFrame.trivial() << G4endl;
}
G4std::vector<G4double> bmom(4, 0.0);
std::vector<G4double> bmom(4, 0.0);
bmom[3] = convertToTargetRestFrame.getTRSMomentum();
G4InuclNuclei ntarget(at, zt);
G4std::vector<G4double> tmom(4, 0.0);
std::vector<G4double> tmom(4, 0.0);
ntarget.setMomentum(tmom);
ntarget.setEnergy();
@@ -208,14 +208,14 @@ G4CollisionOutput G4InuclCollider::collide(G4InuclParticle* bullet,
// convert to the LAB
G4bool withReflection = convertToTargetRestFrame.reflectionNeeded();
G4std::vector<G4InuclElementaryParticle> particles =
std::vector<G4InuclElementaryParticle> particles =
TRFoutput.getOutgoingParticles();
if(!particles.empty()) {
particleIterator ipart;
for(ipart = particles.begin(); ipart != particles.end(); ipart++) {
G4std::vector<G4double> mom = ipart->getMomentum();
std::vector<G4double> mom = ipart->getMomentum();
if(withReflection) mom[3] = -mom[3];
mom = convertToTargetRestFrame.rotate(mom);
@@ -223,15 +223,15 @@ G4CollisionOutput G4InuclCollider::collide(G4InuclParticle* bullet,
mom = convertToTargetRestFrame.backToTheLab(ipart->getMomentum());
ipart->setMomentum(mom);
};
G4std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
std::sort(particles.begin(), particles.end(), G4ParticleLargerEkin());
};
G4std::vector<G4InuclNuclei> nucleus = TRFoutput.getNucleiFragments();
std::vector<G4InuclNuclei> nucleus = TRFoutput.getNucleiFragments();
if(!nucleus.empty()) {
nucleiIterator inuc;
for(inuc = nucleus.begin(); inuc != nucleus.end(); inuc++) {
G4std::vector<G4double> mom = inuc->getMomentum();
std::vector<G4double> mom = inuc->getMomentum();
if(withReflection) mom[3] = -mom[3];
mom = convertToTargetRestFrame.rotate(mom);
inuc->setMomentum(mom);
source/processes/hadronic/models/cascade/cascade/src/G4InuclSpecialFunctions.cc
+5 -5
View File
@@ -134,7 +134,7 @@ G4double G4InuclSpecialFunctions::randomPHI() {
return twopi * inuclRndm();
}
G4std::pair<G4double, G4double> G4InuclSpecialFunctions::randomCOS_SIN() {
std::pair<G4double, G4double> G4InuclSpecialFunctions::randomCOS_SIN() {
G4int verboseLevel = 2;
if (verboseLevel > 3) {
@@ -143,10 +143,10 @@ G4std::pair<G4double, G4double> G4InuclSpecialFunctions::randomCOS_SIN() {
G4double CT = 1.0 - 2.0 * inuclRndm();
return G4std::pair<G4double, G4double>(CT, sqrt(1.0 - CT * CT));
return std::pair<G4double, G4double>(CT, sqrt(1.0 - CT * CT));
}
G4std::vector<G4double> G4InuclSpecialFunctions::generateWithFixedTheta(G4double ct,
std::vector<G4double> G4InuclSpecialFunctions::generateWithFixedTheta(G4double ct,
G4double p) {
G4int verboseLevel = 2;
@@ -154,10 +154,10 @@ G4std::vector<G4double> G4InuclSpecialFunctions::generateWithFixedTheta(G4double
G4cout << " >>> G4InuclSpecialFunctions::generateWithFixedTheta" << G4endl;
}
G4std::vector<G4double> momr(4);
std::vector<G4double> momr(4);
G4double phi = randomPHI();
G4double pt = p * sqrt(fabs(1.0 - ct * ct));
G4std::vector<G4double> mom1(4);
std::vector<G4double> mom1(4);
momr[1] = pt * cos(phi);
momr[2] = pt * sin(phi);
momr[3] = p * ct;
source/processes/hadronic/models/cascade/cascade/src/G4LorentzConvertor.cc
+9 -9
View File
@@ -97,13 +97,13 @@ void G4LorentzConvertor::toTheCenterOfMass() {
gapp = ga * pscm;
}
G4std::vector<G4double> G4LorentzConvertor::rotate(const G4std::vector<G4double> mom) const {
std::vector<G4double> G4LorentzConvertor::rotate(const std::vector<G4double> mom) const {
if (verboseLevel > 3) {
G4cout << " >>> G4LorentzConvertor::rotate(G4std::vector<G4double>)" << G4endl;
G4cout << " >>> G4LorentzConvertor::rotate(std::vector<G4double>)" << G4endl;
}
G4std::vector<G4double> mom_rot(4);
std::vector<G4double> mom_rot(4);
if (verboseLevel > 3) {
G4cout << " ga " << ga << " gbpp " << gbpp << " gapp " << gapp << G4endl;
@@ -134,16 +134,16 @@ G4std::vector<G4double> G4LorentzConvertor::rotate(const G4std::vector<G4double>
return mom_rot;
}
G4std::vector<G4double> G4LorentzConvertor::rotate(const G4std::vector<G4double> mom1,
const G4std::vector<G4double> mom) const {
std::vector<G4double> G4LorentzConvertor::rotate(const std::vector<G4double> mom1,
const std::vector<G4double> mom) const {
if (verboseLevel > 3) {
G4cout << " >>> G4LorentzConvertor::rotate(G4std::vector<G4double>,G4std::vector<G4double>)" << G4endl;
G4cout << " >>> G4LorentzConvertor::rotate(std::vector<G4double>,std::vector<G4double>)" << G4endl;
}
const G4double small = 1.0e-10;
G4std::vector<G4double> mom_rot(4);
std::vector<G4double> mom_rot(4);
G4double pp = 0.0;
@@ -237,7 +237,7 @@ void G4LorentzConvertor::toTheTargetRestFrame() {
gapp = ga * pscm;
}
G4std::vector<G4double> G4LorentzConvertor::backToTheLab(const G4std::vector<G4double>& mom) const {
std::vector<G4double> G4LorentzConvertor::backToTheLab(const std::vector<G4double>& mom) const {
if (verboseLevel > 3) {
G4cout << " >>> G4LorentzConvertor::backToTheLab" << G4endl;
@@ -251,7 +251,7 @@ G4std::vector<G4double> G4LorentzConvertor::backToTheLab(const G4std::vector<G4d
G4cout << " v2 " << v2 << G4endl;
}
G4std::vector<G4double> mom1(4);
std::vector<G4double> mom1(4);
if(v2 < small) {
mom1 = mom;
source/processes/hadronic/models/cascade/cascade/src/G4NonEquilibriumEvaporator.cc
+11 -11
View File
@@ -62,8 +62,8 @@ G4CollisionOutput G4NonEquilibriumEvaporator::collide(G4InuclParticle* bullet,
// initialization
G4double A = nuclei_target->getA();
G4double Z = nuclei_target->getZ();
G4std::vector<G4double> PEX = nuclei_target->getMomentum();
G4std::vector<G4double> pin = PEX;
std::vector<G4double> PEX = nuclei_target->getMomentum();
std::vector<G4double> pin = PEX;
G4double EEXS = nuclei_target->getExitationEnergy();
pin[0] += 0.001 * EEXS;
G4InuclNuclei dummy_nuc;
@@ -91,7 +91,7 @@ G4CollisionOutput G4NonEquilibriumEvaporator::collide(G4InuclParticle* bullet,
G4double AR = A - QP;
G4double ZR = Z - QPP;
G4int NEX = G4int(QEX + 0.5);
G4std::vector<G4double> ppout(4, 0.0);
std::vector<G4double> ppout(4, 0.0);
G4bool try_again = NEX > 0 ? true : false;
while (try_again) {
@@ -116,7 +116,7 @@ G4CollisionOutput G4NonEquilibriumEvaporator::collide(G4InuclParticle* bullet,
if (QEX < sqrt(2.0 * EG)) { // ok
G4std::pair<G4double, G4double> parms = paraMakerTruncated(Z);
std::pair<G4double, G4double> parms = paraMakerTruncated(Z);
G4double AK1 = parms.first;
G4double CPA1 = parms.second;
@@ -153,7 +153,7 @@ G4CollisionOutput G4NonEquilibriumEvaporator::collide(G4InuclParticle* bullet,
if (F1 > 0.0 && F2 > 0.0) {
G4double F = F2 / F1;
G4double M1 = 2.77 * MELE * PL;
G4std::vector<G4double> D(3, 0.0);
std::vector<G4double> D(3, 0.0);
D[0] = M1 * F2 * F2 * pow(F, NEX - 1) / (QEX + 1.0);
if (D[0] > 0.0) {
@@ -286,14 +286,14 @@ G4CollisionOutput G4NonEquilibriumEvaporator::collide(G4InuclParticle* bullet,
EPART *= 0.001; // to the GeV
// generate particle momentum
G4double pmod = sqrt(EPART * (2.0 * mass + EPART));
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double P1 = pmod * COS_SIN.second;
mom[1] = P1 * cos(FI);
mom[2] = P1 * sin(FI);
mom[3] = pmod * COS_SIN.first;
G4std::vector<G4double> mom_at_rest(4);
std::vector<G4double> mom_at_rest(4);
for (G4int i = 1; i < 4; i++) mom_at_rest[i] = -mom[i];
@@ -319,14 +319,14 @@ G4CollisionOutput G4NonEquilibriumEvaporator::collide(G4InuclParticle* bullet,
mom[0] = sqrt(mom[1] * mom[1] + mom[2] * mom[2] +
mom[3] * mom[3] + mass * mass);
G4std::vector<G4double> part_mom =
std::vector<G4double> part_mom =
toTheExitonSystemRestFrame.backToTheLab(mom);
part_mom[0] = sqrt(part_mom[1] * part_mom[1] +
part_mom[2] * part_mom[2] + part_mom[3] * part_mom[3] +
mass * mass);
G4std::vector<G4double> ex_mom =
std::vector<G4double> ex_mom =
toTheExitonSystemRestFrame.backToTheLab(mom_at_rest);
ex_mom[0] = sqrt(ex_mom[1] * ex_mom[1] + ex_mom[2] * ex_mom[2]
@@ -416,7 +416,7 @@ G4CollisionOutput G4NonEquilibriumEvaporator::collide(G4InuclParticle* bullet,
// the exitation energy has to be re-set properly for the energy
// conservation
G4std::vector<G4double> pnuc(4);
std::vector<G4double> pnuc(4);
for (G4int i = 1; i < 4; i++) pnuc[i] = pin[i] - ppout[i];
G4InuclNuclei nuclei(pnuc, A, Z);
source/processes/hadronic/models/cascade/cascade/src/G4NucleiModel.cc
+50 -50
View File
@@ -26,7 +26,7 @@
#include "G4LorentzConvertor.hh"
#include "G4CollisionOutput.hh"
typedef G4std::vector<G4InuclElementaryParticle>::iterator particleIterator;
typedef std::vector<G4InuclElementaryParticle>::iterator particleIterator;
G4NucleiModel::G4NucleiModel()
: verboseLevel(2) {
@@ -82,7 +82,7 @@ void G4NucleiModel::generateModel(G4double a,
if (a > 3.5) { // a > 3
G4std::vector<G4double> ur;
std::vector<G4double> ur;
G4int icase = 0;
@@ -115,9 +115,9 @@ void G4NucleiModel::generateModel(G4double a,
G4double tot_vol = 0.0;
G4std::vector<G4double> v;
std::vector<G4double> v;
G4std::vector<G4double> v1;
std::vector<G4double> v1;
G4int i(0);
for (i = 0; i < number_of_zones; i++) {
@@ -139,9 +139,9 @@ void G4NucleiModel::generateModel(G4double a,
// proton
G4double dd0 = 3.0 * z * oneBypiTimes4 / tot_vol;
G4std::vector<G4double> rod;
G4std::vector<G4double> pf;
G4std::vector<G4double> vz;
std::vector<G4double> rod;
std::vector<G4double> pf;
std::vector<G4double> vz;
for (i = 0; i < number_of_zones; i++) {
G4double rd = dd0 * v[i] / v1[i];
@@ -173,7 +173,7 @@ void G4NucleiModel::generateModel(G4double a,
fermi_momenta.push_back(pf);
// pion stuff (primitive)
G4std::vector<G4double> vp(number_of_zones, pion_vp);
std::vector<G4double> vp(number_of_zones, pion_vp);
zone_potentials.push_back(vp);
} else { // a < 4
@@ -181,9 +181,9 @@ void G4NucleiModel::generateModel(G4double a,
number_of_zones = 1;
zone_radii.push_back(radForSmall);
G4double vol = 1.0 / piTimes4thirds / pow(zone_radii[0], 3);
G4std::vector<G4double> rod;
G4std::vector<G4double> pf;
G4std::vector<G4double> vz;
std::vector<G4double> rod;
std::vector<G4double> pf;
std::vector<G4double> vz;
G4int i(0);
for (i = 0; i < number_of_zones; i++) {
@@ -216,7 +216,7 @@ void G4NucleiModel::generateModel(G4double a,
fermi_momenta.push_back(pf);
// pion (primitive)
G4std::vector<G4double> vp(number_of_zones, pion_vp_small);
std::vector<G4double> vp(number_of_zones, pion_vp_small);
zone_potentials.push_back(vp);
};
@@ -366,9 +366,9 @@ G4InuclElementaryParticle G4NucleiModel::generateNucleon(G4int type,
G4double pmod = fermi_momenta[type - 1][zone] * pow(inuclRndm(), one_third);
G4std::vector<G4double> mom(4);
std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
@@ -389,9 +389,9 @@ G4InuclElementaryParticle G4NucleiModel::generateQuasiDeutron(G4int type1,
G4cout << " >>> G4NucleiModel::generateQuasiDeutron" << G4endl;
}
G4std::vector<G4double> mom = generateNucleon(type1, zone).getMomentum();
G4std::vector<G4double> mom1 = generateNucleon(type2, zone).getMomentum();
G4std::vector<G4double> dmom(4);
std::vector<G4double> mom = generateNucleon(type1, zone).getMomentum();
std::vector<G4double> mom1 = generateNucleon(type2, zone).getMomentum();
std::vector<G4double> dmom(4);
for (G4int i = 1; i < 4; i++) dmom[i] = mom[i] + mom1[i];
@@ -437,7 +437,7 @@ partners G4NucleiModel::generateInteractionPartners(G4CascadParticle& cparticle)
G4int ptype = cparticle.getParticle().type();
G4int zone = cparticle.getCurrentZone();
G4double pmass = cparticle.getParticle().getMass();
G4std::vector<G4double> pmom = cparticle.getParticle().getMomentum();
std::vector<G4double> pmom = cparticle.getParticle().getMomentum();
G4double r_in;
G4double r_out;
@@ -475,7 +475,7 @@ partners G4NucleiModel::generateInteractionPartners(G4CascadParticle& cparticle)
} else { // normal case
G4std::vector<G4InuclElementaryParticle> particles;
std::vector<G4InuclElementaryParticle> particles;
G4LorentzConvertor dummy_convertor;
@@ -526,8 +526,8 @@ partners G4NucleiModel::generateInteractionPartners(G4CascadParticle& cparticle)
if (cparticle.getParticle().pion()) { // absorption possible
G4std::vector<G4InuclElementaryParticle> qdeutrons;
G4std::vector<G4double> acsecs;
std::vector<G4InuclElementaryParticle> qdeutrons;
std::vector<G4double> acsecs;
G4double tot_abs_csec = 0.0;
G4double abs_sec;
@@ -674,14 +674,14 @@ partners G4NucleiModel::generateInteractionPartners(G4CascadParticle& cparticle)
return thePartners;
}
G4std::vector<G4CascadParticle> G4NucleiModel::generateParticleFate(G4CascadParticle& cparticle,
std::vector<G4CascadParticle> G4NucleiModel::generateParticleFate(G4CascadParticle& cparticle,
G4ElementaryParticleCollider* theElementaryParticleCollider) {
if (verboseLevel > 3) {
G4cout << " >>> G4NucleiModel::generateParticleFate" << G4endl;
}
G4std::vector<G4CascadParticle> outgouing_cparticles;
std::vector<G4CascadParticle> outgouing_cparticles;
partners thePartners = generateInteractionPartners(cparticle);
@@ -706,7 +706,7 @@ G4std::vector<G4CascadParticle> G4NucleiModel::generateParticleFate(G4CascadPart
} else { // there are possible interactions
G4std::vector<G4double> old_position = cparticle.getPosition();
std::vector<G4double> old_position = cparticle.getPosition();
G4InuclElementaryParticle bullet = cparticle.getParticle();
@@ -734,14 +734,14 @@ G4std::vector<G4CascadParticle> G4NucleiModel::generateParticleFate(G4CascadPart
output.printCollisionOutput();
}
G4std::vector<G4InuclElementaryParticle> outgoing_particles =
std::vector<G4InuclElementaryParticle> outgoing_particles =
output.getOutgoingParticles();
if (passFermi(outgoing_particles, zone)) { // interaction
cparticle.propagateAlongThePath(thePartners[i].second);
G4std::vector<G4double> new_position = cparticle.getPosition();
std::vector<G4double> new_position = cparticle.getPosition();
for (G4int ip = 0; ip < G4int(outgoing_particles.size()); ip++)
outgouing_cparticles.push_back(G4CascadParticle(outgoing_particles[ip],
@@ -810,7 +810,7 @@ G4std::vector<G4CascadParticle> G4NucleiModel::generateParticleFate(G4CascadPart
return outgouing_cparticles;
}
G4bool G4NucleiModel::passFermi(const G4std::vector<G4InuclElementaryParticle>& particles,
G4bool G4NucleiModel::passFermi(const std::vector<G4InuclElementaryParticle>& particles,
G4int zone) {
if (verboseLevel > 3) {
G4cout << " >>> G4NucleiModel::passFermi" << G4endl;
@@ -852,9 +852,9 @@ void G4NucleiModel::boundaryTransition(G4CascadParticle& cparticle) {
} else {
G4std::vector<G4double> mom = cparticle.getMomentum();
std::vector<G4double> mom = cparticle.getMomentum();
G4std::vector<G4double> pos = cparticle.getPosition();
std::vector<G4double> pos = cparticle.getPosition();
G4int type = cparticle.getParticle().type();
@@ -972,7 +972,7 @@ G4CascadParticle G4NucleiModel::initializeCascad(G4InuclElementaryParticle* part
G4double rz = nuclei_radius * s1;
G4std::vector<G4double> pos(3);
std::vector<G4double> pos(3);
pos[0] = rz * cos(phi);
pos[1] = rz * sin(phi);
@@ -987,7 +987,7 @@ G4CascadParticle G4NucleiModel::initializeCascad(G4InuclElementaryParticle* part
return cpart;
}
G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4InuclNuclei* target) {
@@ -1007,8 +1007,8 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
const G4double s4max = 7.0;
const G4int itry_max = 100;
G4std::vector<G4CascadParticle> casparticles;
G4std::vector<G4InuclElementaryParticle> particles;
std::vector<G4CascadParticle> casparticles;
std::vector<G4InuclElementaryParticle> particles;
// first decide whether it will be cascad or compound final nuclei
@@ -1033,15 +1033,15 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
if(itryg > 0) particles.resize(0);
// nucleons coordinates and momenta in nuclei rest frame
G4std::vector<G4std::vector<G4double> > coordinates;
G4std::vector<G4std::vector<G4double> > momentums;
std::vector<std::vector<G4double> > coordinates;
std::vector<std::vector<G4double> > momentums;
if (ab < 3.0) { // deutron, simplest case
G4double r = 2.214 - 3.4208 * log(1.0 - 0.981 * inuclRndm());
G4double s = 2.0 * inuclRndm() - 1.0;
G4double r1 = r * sqrt(1.0 - s * s);
G4std::vector<G4double> coord1(3);
std::vector<G4double> coord1(3);
G4double phi = randomPHI();
coord1[0] = r1 * cos(phi);
coord1[1] = r1 * sin(phi);
@@ -1077,8 +1077,8 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4cout << " p nuc " << p << G4endl;
}
G4std::vector<G4double> mom(4);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::vector<G4double> mom(4);
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double FI = randomPHI();
G4double P1 = p * COS_SIN.second;
mom[1] = P1 * cos(FI);
@@ -1093,7 +1093,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4int ia = int(ab + 0.5);
G4std::vector<G4double> coord1(3);
std::vector<G4double> coord1(3);
G4bool badco = true;
@@ -1123,7 +1123,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
if (sqrt(s) * exp(-s) > u && s < s3max) {
s = r0forAeq3 * sqrt(s);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
u = s * COS_SIN.second;
G4double phi = randomPHI();
coord1[0] = u * cos(phi);
@@ -1215,7 +1215,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
if (sqrt(s) * exp(-s) * (1.0 + b * s) > u && s < s4max) {
s = r0forAeq4 * sqrt(s);
G4std::pair<double, double> COS_SIN = randomCOS_SIN();
std::pair<double, double> COS_SIN = randomCOS_SIN();
u = s * COS_SIN.second;
G4double phi = randomPHI();
coord1[0] = u*cos(phi);
@@ -1291,7 +1291,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4cout << " can not generate the nucleons coordinates for a " << ab <<
G4endl;
return G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
return std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
(casparticles, particles);
} else { // momentums
@@ -1299,7 +1299,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4double p;
G4double u;
G4double x;
G4std::vector<G4double> mom(4);
std::vector<G4double> mom(4);
//G4bool badp = True;
G4int i(0);
@@ -1313,7 +1313,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
if(x > inuclRndm()) {
p = sqrt(0.01953 * u);
G4std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
std::pair<G4double, G4double> COS_SIN = randomCOS_SIN();
G4double pt = p * COS_SIN.second;
G4double phi = randomPHI();
mom[1] = pt * cos(phi);
@@ -1328,7 +1328,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
if(itry == itry_max) {
G4cout << " can not generate proper momentum for a " << ab << G4endl;
return G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
return std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
(casparticles, particles);
};
@@ -1360,7 +1360,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
G4double s1 = sqrt(inuclRndm());
G4double phi = randomPHI();
G4double rz = (nuclei_radius + rb) * s1;
G4std::vector<double> global_pos(3);
std::vector<double> global_pos(3);
global_pos[0] = rz * cos(phi);
global_pos[1] = rz * sin(phi);
global_pos[2] = -(nuclei_radius + rb) * sqrt(1.0 - s1 * s1);
@@ -1372,7 +1372,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
};
// all nucleons at rest
G4std::vector<G4InuclElementaryParticle> raw_particles;
std::vector<G4InuclElementaryParticle> raw_particles;
G4int ia = int(ab + 0.5);
G4int iz = int(zb + 0.5);
@@ -1390,7 +1390,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
particleIterator ipart;
for (ipart = raw_particles.begin(); ipart != raw_particles.end(); ipart++) {
G4std::vector<G4double> mom =
std::vector<G4double> mom =
toTheBulletRestFrame.backToTheLab(ipart->getMomentum());
ipart->setMomentum(mom);
};
@@ -1398,7 +1398,7 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
// fill cascad particles and outgoing particles
for(G4int ip = 0; ip < G4int(raw_particles.size()); ip++) {
G4std::vector<G4double> mom = raw_particles[ip].getMomentum();
std::vector<G4double> mom = raw_particles[ip].getMomentum();
G4double pmod = sqrt(mom[1] * mom[1] + mom[2] * mom[2] + mom[3] * mom[3]);
G4double t0 = -(mom[1] * coordinates[ip][0] + mom[2] * coordinates[ip][1] +
mom[3] * coordinates[ip][2]) / pmod;
@@ -1477,6 +1477,6 @@ G4NucleiModel::initializeCascad(G4InuclNuclei* bullet,
for(ip = 0; ip < G4int(particles.size()); ip++) particles[ip].printParticle();
}
return G4std::pair<G4std::vector<G4CascadParticle>, G4std::vector<G4InuclElementaryParticle> >
return std::pair<std::vector<G4CascadParticle>, std::vector<G4InuclElementaryParticle> >
(casparticles, particles);
}
source/processes/hadronic/models/cascade/cascade/src/G4RegionModel.cc
-189
View File
@@ -1,189 +0,0 @@
//
// ********************************************************************
// * DISCLAIMER *
// * *
// * The following disclaimer summarizes all the specific disclaimers *
// * of contributors to this software. The specific disclaimers,which *
// * govern, are listed with their locations in: *
// * http://cern.ch/geant4/license *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. *
// * *
// * This code implementation is the intellectual property of the *
// * GEANT4 collaboration. *
// * By copying, distributing or modifying the Program (or any work *
// * based on the Program) you indicate your acceptance of this *
// * statement, and all its terms. *
// ********************************************************************
#include "G4RegionModel.hh"
const G4double G4RegionModel::radius0 = 1.0E-15;
const G4double G4RegionModel::BE = 7;
G4RegionModel::G4RegionModel(const G4int numberOfLayers, const G4int A, const G4int Z)
{
//count the radiuses, densities and fermi momenta with A and Z
G4double r = radius0*pow(A, 1/3);
if(numberOfLayers==1){
radius.push_back(r);
G4double rho = A / (4/3*pi*pow(r,3));
density.push_back(rho);
G4double protonMass = G4Proton::Proton()->GetPDGMass();
G4double neutronMass = G4Neutron::Neutron()->GetPDGMass();
G4double protonDensity = Z / (4/3*pi*pow(r,3));
G4double neutronDensity = (A-Z) / (4/3*pi*pow(r,3));
protonFermiEnergy.push_back(GetFermiEnergy(protonDensity, protonMass));
neutronFermiEnergy.push_back(GetFermiEnergy(neutronDensity, neutronMass));
protonFermiMomentum.push_back(GetFermiMomentum(protonDensity, protonMass));
neutronFermiMomentum.push_back(GetFermiMomentum(neutronDensity, neutronMass));
G4double fermiEP = *protonFermiEnergy.begin();
G4double fermiEN = *neutronFermiEnergy.begin();
protonPotentialEnergy.push_back(-(fermiEP + BE));
neutronPotentialEnergy.push_back(-(fermiEN + BE));
}
else{
if(numberOfLayers==3){
radius.push_back(0.1*r);
radius.push_back(0.2*r);
radius.push_back(0.9*r);
}
}
}
G4RegionModel::~G4RegionModel(){}
/*
void G4RegionModel::Init(const G4int numberOfLayers, const G4int A, const G4int Z){
//count the radiuses, densities and fermi momenta with A and Z
G4double r = radius0*pow(A, 1/3);
if(numberOfLayers==1){
radius.push_back(r);
G4double rho = A / (4/3*pi*pow(r,3));
density.push_back(rho);
G4double protonMass = G4Proton::Proton()->GetPDGMass()/MeV;
G4double neutronMass = G4Neutron::Neutron()->GetPDGMass()/MeV ;
G4double protonDensity = Z / (4/3*pi*pow(r,3));
G4double neutronDensity = (A-Z) / (4/3*pi*pow(r,3));
protonFermiEnergy.push_back(GetFermiEnergy(protonDensity, protonMass));
neutronFermiEnergy.push_back(GetFermiEnergy(neutronDensity, neutronMass));
protonFermiMomentum.push_back(GetFermiMomentum(protonDensity, protonMass));
neutronFermiMomentum.push_back(GetFermiMomentum(neutronDensity, neutronMass));
G4double fermiEP = *protonFermiEnergy.begin();
G4double fermiEN = *neutronFermiEnergy.begin();
protonPotentialEnergy.push_back(-(fermiEP + BE));
neutronPotentialEnergy.push_back(-(fermiEN + BE));
}
else{
if(numberOfLayers==3){
radius.push_back(0.1*r);
radius.push_back(0.2*r);
radius.push_back(0.9*r);
}
}
}
*/
//--------------------------------------------------------------
G4double G4RegionModel::GetDensity(G4double r){
iterator j=density.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
return 0;
}
G4double G4RegionModel::GetPotentialEnergy(G4double r, G4int particle){
if(particle == 0){ //proton
iterator j=protonPotentialEnergy.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
return 0;
}
if(particle == 1){ //neutron
iterator j=neutronPotentialEnergy.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
return 0;
}
return 0;
}
G4double G4RegionModel::GetMaximumNucleonMomentum(G4double r,
G4int nucleon){
if(nucleon == 0){
iterator j=protonFermiMomentum.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
}
if(nucleon==1){
iterator j=neutronFermiMomentum.begin();
for(iterator i=radius.begin(); i<radius.end(); i++){
if(r <= *i) return *j;
j++;
}
}
G4Exception("G4RegionModel::GetMaximumNucleonMomentum - return value undefined");
return 0;
}
G4double G4RegionModel::GetFermiMomentum(G4double aDensity,
G4double aMass){
return sqrt(2*aMass*GetFermiEnergy(aDensity, aMass));
}
G4double G4RegionModel::GetFermiEnergy(G4double aDensity,
G4double aMass){
//G4double hbar = 1.0E-6;
return (pow(hbar_Planck,2)/(2*aMass)*pow((3*pi2*aDensity),2/3));
}
source/processes/hadronic/models/cascade/cascade/src/G4WatcherGun.cc
+3 -3
View File
@@ -38,9 +38,9 @@ void G4WatcherGun::setWatchers() {
G4cout << " >>> G4WatcherGun::setWatchers" << G4endl;
}
G4std::vector<G4double> as;
G4std::vector<G4double> cs;
G4std::vector<G4double> errs;
std::vector<G4double> as;
std::vector<G4double> cs;
std::vector<G4double> errs;
// specific stuff to monitor the difference with fortran
// particle type
source/processes/hadronic/models/cascade/cascade/src/bindingEnergyExact.cc
+1 -1
View File
@@ -22,7 +22,7 @@
#include "G4InuclSpecialFunctions.hh"
#include "g4std/iostream"
#include <iostream>
G4double G4InuclSpecialFunctions::bindingEnergyExact(G4double A,
G4double Z) {
source/processes/hadronic/models/cascade/cascade/src/paraMaker.cc
+6 -6
View File
@@ -22,7 +22,7 @@
#include "G4InuclSpecialFunctions.hh"
G4std::pair<G4std::vector<G4double>, G4std::vector<G4double> > G4InuclSpecialFunctions::paraMaker(G4double Z) {
std::pair<std::vector<G4double>, std::vector<G4double> > G4InuclSpecialFunctions::paraMaker(G4double Z) {
G4int verboseLevel = 1;
if (verboseLevel > 3) {
@@ -37,8 +37,8 @@ G4std::pair<G4std::vector<G4double>, G4std::vector<G4double> > G4InuclSpecialFun
const G4double CP[5] = {0.50, 0.28, 0.20, 0.15, 0.10};
const G4double AA[5] = {0.68, 0.82, 0.91, 0.97, 0.98};
const G4double CA[5] = {0.10, 0.10, 0.10, 0.08, 0.06};
G4std::vector<G4double> AK(6);
G4std::vector<G4double> CPA(6);
std::vector<G4double> AK(6);
std::vector<G4double> CPA(6);
AK[0] = 0.0;
CPA[0] = 0.0;
G4double AK2 = 0.0;
@@ -87,10 +87,10 @@ G4std::pair<G4std::vector<G4double>, G4std::vector<G4double> > G4InuclSpecialFun
AK[4] = AK6 - 0.06;
CPA[4] = 4.0 * CP6 / 3.0;
return G4std::pair<G4std::vector<G4double>, G4std::vector<G4double> >(AK, CPA);
return std::pair<std::vector<G4double>, std::vector<G4double> >(AK, CPA);
}
G4std::pair<G4double, G4double> G4InuclSpecialFunctions::paraMakerTruncated(G4double Z) {
std::pair<G4double, G4double> G4InuclSpecialFunctions::paraMakerTruncated(G4double Z) {
G4int verboseLevel = 1;
if (verboseLevel > 3) {
@@ -126,5 +126,5 @@ G4std::pair<G4double, G4double> G4InuclSpecialFunctions::paraMakerTruncated(G4do
};
};
return G4std::pair<G4double, G4double>(AK2, CP2);
return std::pair<G4double, G4double>(AK2, CP2);
}
source/processes/hadronic/models/cascade/doc/GNUmakefile
-12
View File
@@ -1,12 +0,0 @@
all: # :::
grep ":::" GNUmakefile
man: # ::: Make manual.
make clean; latex manCascade; bibtex manCascade; latex manCascade; latex manCascade; dvips manCascade.dvi -o manCascade.ps; gv manCascade.ps
pub: # ::: Make publication.
make clean; latex pubCascade; bibtex pubCascade; latex pubCascade; latex pubCascade; dvips pubCascade.dvi -o pubCascade.ps; gv pubCascade.ps
clean: # ::: clean directory
rm -f \#*.*\# \#*\# \#* .*~ .#* *.*~ *~ *.o; rm -f core tmp.txt *.blg *.bbl *.toc *.log *.aux *.dvi
source/processes/hadronic/models/cascade/doc/README
-4
View File
@@ -1,4 +0,0 @@
Main document is manCascade.tex.
Create documentation with 'gmake' or
full release (ps, html and pdf-versions)
with 'gmake release'.
source/processes/hadronic/models/cascade/doc/espcrc2.sty
-226
View File
@@ -1,226 +0,0 @@
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%
%
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%
% IMPORTANT NOTICE:
%
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%
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%
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%
% If you receive only this file from someone, complain!
%
%
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\def\filedate{24 November 1993}
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source/processes/hadronic/models/cascade/doc/evaporationUml.eps
-852
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\title{HETC/INUCL++ manual - System for Modelling Hadronic Intranuclear Processes}
\author{Aatos Heikkinen, Nikita Stepanov
\address{ Helsinki Institute of Physics,
P.O.Box 9,\\
FIN-00014 University of Helsinki, Finland }
}
\begin{document}
\begin{abstract}
HETC/INUCL is a simulation package and a model of intermediate energy nuclear
reactions.
INUCL consists of cascade, fission models, pre-equilibrium, and evaporation
This manual describes the models used in INUCL++.
This documet works as an manual, status report and working document for INUCL project. In accordance with this, we represent results acieved with INUCL. Comparison with measurement is made.
We also descripe staus of Geant4 installation on INUCL software \cite{titarenko99a}.
\end{abstract}
\maketitle
% uncomment main sections when needed
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% declarations for front matter
%\title{HETC/INUCL++ manual - System for Modelling Hadronic Intranuclear Processes}
%\author{Aatos Heikkinen, Nikita Stepanov
%\address{ Helsinki Institute of Physics,
%P.O.Box 9,\\
%FIN-00014 University of Helsinki, Finland }
% }
%\begin{document}
%\begin{abstract}
%HETC/INUCL is a simulation package and a model of intermediate energy nuclear
%reactions.
%INUCL consists of cascade, fission models, pre-equilibrium, and evaporation
%This manual describes the models used in INUCL++.
%This documet works as an manual, status report and working document for INUCL project. In accordance with this, we represent results acieved with INUCL. Comparison with measurement is made.
%We also descripe staus of Geant4 installation on INUCL software \cite{titarenko99a}.
%\end{abstract}
%\maketitle
\section{VOCABULARY}
\begin{itemize}
\item {\it NR} Nuclear reaction
\item {\it quasi-elastic reaction} NR where nucleon can be knocked out of its nuclear.
\item {\it T-nucleus} Target nucleus
\end{itemize}
\section{INTRODUCTION TO INTERMEDIATE-ENERGY NUCLEAR PHYSICS}
Fig :::. Schematic nucleon structure.
The central nucleon is shown as collection of three constituent quarks interacting via the color force.
Closer views show a more complex picture.
At higher energies ($~200~MeV$) energy is high enough to momentarily exite a nucleon into the exited dalta-resonant state ($\Delta$-resonance).
\subsection{Classification of Cross-Sections of NRS}
Let us denote an incident particle and a nucleus under investigation by the symbols $a$ and $A$, respectively.
Following final states following from $a + A$ are possible \cite{iljinov94}:
\begin{itemize}
\item $a + A$ : elastic scattering
\item $a^{*} + A$ : scattering with an exitation of the $a$ particle
\item $a + A^{*}$ : scattering with an exitation of the nucleus
\item $a^{*} + A^{*}$ : scattering in which both the particle and the nucleus are exited
\item $a^{'} + A^{'}$ : reaction involving the production of a new particle and a new nucleus
\item $a^{'} + a^{''} + A^{'}$ : reaction involving the production of two new particles and a new nucleus
\end{itemize}
\subsection{Quantum Formulation of Collision Problem}
\subsubsection{Reaction Channels}
Consider a collision of two complex particles. ::: \cite{iljinov94}
\subsubsection{Transition Probabilities and S-Matrix}
In accordance with general priciples of quantum theory, the probability
::: \cite{iljinov94}
\subsubsection{S-Matrix and Cross-SectionsScattering Amplitude}
::: \cite{iljinov94}
\subsection{Nuclear Structure Phase Diagram}
THe atomic nucleus with its $A$ nucleons is governed by a large number of degrees of freedom.
\subsection{Nuclear density}
Nuclear charge densities are usually well described using present-day effective two-body forces; it is also clear that saturation of the charge dencity indeed occurs.
The central density barely varies when the nucleon number changes.
\subsection{Nuclear radius}
\subsection{Mass formula}
A parametrization of the nuclear binding energy in the groud state,
was first discussed by Bethe, Bacher and Weizs\"{a}cker.
Parametrization conatains volume, surface, Coulomb and symmetry correction terms (we neglegt here typical shell model correction terms) and reads
$$B(E, A) = a_{\nu} A - a_{s} A^{2/3} - a_{c} Z(Z-1)A^{-1/3} -$$
\begin{equation}
a_{A}\frac{(A-2Z)^2}{A}
\end{equation}
Nuclear charge radius turns out to be a rather well-defined quantity.
\subsection{Symmetry consepts in Nuclear Physics}
The nuclear two-body force obeys quite a large number of basic invariances.
Forexample invariance under interchange of the spatial coordinates, translation invariance, Galilean invariance, space reflection symmetry, time reversal invariance, rotation invariance in coordinate space and rotation invariance in charge space (isospin).
The symmetry consept (1932) of isospin symmetry,
describing the charge independence of the nuclear forces by means of the isospin consept with the SU(2) group as the underlying mathematical group was suggested by Heisenberg.
This (simplest of all dynamical symmetries) expresses the invariance of the Hamiltonian under the exchange of all proton and neutron coordinates \cite{heyde98}.
\subsection{Quantum effects}
On the level of the nucleons themselves, invariance of the total nuclear wave functions under the exchange of identical nucleons affects the possible models realized.
The Pauli principle implies antisymmetry for the total fermionic wave function and this has very definite consequences for the types of collective motion that can be set up inside the nucleus.
\subsection{INC-Model}
Widely used semiclassical miscroscopic description of a collision between a particle and a nucleus,
was proposed by Serber \cite{serber47} and Goldberger \cite{goldberger48}.
\section{INTRODUCTION TO INUCL}
\subsection{BACKGROUND}
Originally the INUCL code was published in 1983 \cite{stepanov}.
This code, written with Fortran has been used in [:::] \cite{:::}.
Comprison of results between INCUL and LAHET, CEM95, HETC, CASCADE,
YIELDX, and ALICE code are presented in Refs. \cite{titarenko99a}.
Year 2000 a aroject to implement INUCL into Geant4 hadronic physic
module using C++ wal launched.
New now works also as standalone c++ software called INUCL++.
\subsection{SUMMARY OF INUCL MODEL FEATURES}
\begin{itemize}
\item Originally INUCL was designed as a particle - nucleus interaction simulation block for the particle - target interaction simulation program PHOENIX. It produces an exclusive approach to simulating events with reasonable performance.
\item INUCL is based on N. Stepanov Ph.D. thesis, ITEP, Moscow, 1990.
Also, contribution Vladimir D. Kazaritsky.
\item Now we have standalone F77 based INUCL code and INUCL++ written in C++.
INUCL++ is now written using Geant4 coding style and integration to hadronic models in in progress. Problem: speed is five times slower.
\end{itemize}
\subsubsection{INUCL models}
\begin{itemize}
\item Intranuclear cascade
\item Precompound decay (exiton master equation)
\item Evaporation (Weisskopf - Ewing)
\item Fission (phenomenological model, incorporating some features of the fission statistical model)
\end{itemize}
\subsubsection{Particles treated}
\begin{itemize}
\item Range of targets allowed arbitrary.
\item Range of projectiles allowed p, n, pi and nuclei.
\item From a few Mev to 10 GeV for n, p, pi and up to about 100 MeV / nucleon for nuclei.
\end{itemize}
\subsubsection{Cross sections}
\begin{itemize}
\item Total inelastic cross section has to be taken from outside to normalize all data.
\item Total reaction cross-sections [mbarn] were calculated by J.R. Letaw's formulae
%$45 A^0.7 (1+0.016 sin(5.3-2.63 log10(A)))^(1-0.62 exp(-E / 200) sin(10.9 E^(-0.28)))$
\item Ref.: S. Pearlstein, The Astrophysical Journal, 346: 1049-1060, 1989 November 15
\item Fermi energy calculated in a local density approximation.
\end{itemize}
Nuclear density distribution are derived from the Re(Vopt( r)) distribution. In cascade part, nucleus is divided into a finite number of zones with constant density.
%nuclear radius parameterization: By the definition R(A) is derived from eq. Den(R(A)) = 0.01*Den max
\subsubsection{Nucleon nucleon cross-sections}
\begin{itemize}
\item Parametrizations based on the experimental data (ED) are used.
\item They are energy and isospin dependent.
\item The parameterizations described in ([1] Barashenkov V.S., Toneev V.D. High Energy interactions of particles and nuclei with nuclei. Moscow, 1972
%(in Russian, but there is an English translation)) are used.
\item Pauli exclusion in the INC: Simulated particle-particle interaction is accepted only for secondary nucleons which have $E_n > E_f$.
\item Nuclear density effects are recalculated after each step
\item Cascade is stopped when all the particles, which can escape the nucleus, do it. Then conformity with the energy - conservation law is checked and the given event is accepted, if $E_{exitation} > E_{cut} \approx $a few $MeV$.
\item For nucleons binding energies are calculated using mass formula. For pions Vopt is taken to be constant (about 7 MeV).
\end{itemize}
%What criteria for p-h excitation? is the next phase precompound or compound'? Only pions. The next phase is precompound. Initial conditions are defined during the cascad phase: p -number of "particles", i.e. nucleons, which can not escape the nucleus and have too small interaction probability; h - number of "holes" = number of nuclear nucleons involved in the cascade; energy - momentum of the exiton system derived from the conservation law.
\subsubsection{Precompound phase}
%, describe the PE model used, parameters, i.e., partial state densities, transition rates?
\begin{itemize}
\item Main parameters are taken from (Ribansky I. et al, Nucl.Phys.,1973, A205, p.545 (level densities); Kolbach.C., Z.Phys.,1978, A287, p.319 (matrix elements)).
%(Only N -> N, N -> N + 2, N -> N -2, N -> N - 1 channels are treated.)
\item The angular distribution is isotropic in the frame of rest of the exiton system.
\end{itemize}
%Describe parameters used: level densities, inverse cross-sections or transmission coefficient, choice of optical model parameters if relevant (or reference to source), range of excitations allowed, inclusive or exclusive results? Weisskopf-Ewing evaporation in competition with fission. Emissions of n,p,d,t,He3,He4,gamma is allowed. Level densities derived from exp.data are used. Angular momentum and spin dependence are not included. Other parameters are the same as in ([1], see 5a.) Fermi breakup is allowed onlyin some extreme cases, i.e. for light nuclei and E(exitation) > 3.*Eb. Only the total nuleus decay into neutrons and protons is treated.
\begin{verbatim}
particles p, n, pi, D, T, He3, He4,\gamma
(INUCLN with neutrino 31.3.98)
pion aborption
interaction crosssections
(all data for (N, N) and (pi, N) interactions (dn/dsigma, d3sigma/d3p,
partial multiplicity for npi<=5 error 10-20\%)
pre-equilibrium exiton model
\end{verbatim}
\section{INUCL MANUAL PAGES}
\subsection{Reaction initial state simulation}
\subsubsection{Projectiles and enery range of model}
The GEANT4 INCUL model is cpable to predict final states :::
The allowed allowed bombarding kinetic enery is recommended to be more than
$20~MeV$ in the laboratory frame.
The upper limit of initial kinetic energy is approximately $10~GeV$.
\subsubsection{Nucleus initialization}
\begin{itemize}
\item {\bf Nucleon radii}:
\item {\bf The initial momenta of the nucleons}:
\item {\bf Nucleon binding energy}:
\end{itemize}
\subsection{Random choice of the impact parameter}
The impact parameter $b$ is randomly selected according to
\subsection{Hadron propagation}
\subsection{Selection of particle collisions and particle decays}
\subsection{Hadron interation cross sections}
\subsection{Hadron collision simulation}
\subsubsection{Two-body hadron scattering}
\subsubsection{Angular distribution of two-body hadron scatterings}
\subsubsection{$\pi$-absorption simulation}
\subsection{Resonance decay simulation}
\subsection{Phenomenological potentials}
\subsubsection{The nucleon potential}
\subsection{Pauli blocking simulation}
\subsection{Residual nucleus parameters in the hadron-nucleus collision}
\subsection{Calculation of a residual nucleus exitation energy}
\subsection{Staus of this document}
8.6.02 created by A. Heikkinen
\section{INTRANUCLEAR CASCADE MODEL}
\subsection{NUCLEON DENCITY IN THE ATOM}
Halo nucleus such as $^{11}Li$ are not modelled.
\subsection{IMPULSE DISTRIBUTION}
\subsection{DISTRIBUTION OF POTENTIAL ENERGY}
\subsection{QUANTUM EFFECTS}
Pauli exclusion principle
\subsection{DESCRIPTION OF INC}
\section{FISSION}
\section{PRE-EQUILIBRIUM}
\section{EVAPORATION}
Exited nuclei cools further trough the emission of gamma radiation.
If simulation is detailed,
the emitted gamma rays contain information about the cooling route
and region the nucleus is passing trough.
\section{FROM INUCL TO INUCL++}
\subsection{DESIGN AND ANALYSIS}
We desided to make separate INUCL++ implementations one as an stand
alone with spesific cross-section data and particle definition, and
another iplementation that re-uses Geant4 classes.
So, requirements for the INUCL++ came mainly from Geant4.
Coding style and organization should follow those used in Geant4.
Interace-classes to Geant4 hadronic models define the separation of
cascade, fission, pre-equilibrium, and evaporation. Thus INUCL++
implementation in Geant4 consists of four separate modules.
\subsection{IMPLEMENTATION}
\subsection{TESTING}
Extensive testing :::
Speed comparison :::
\section{INUCL++ AS A STANDALONE PROGRAM}
\section{INUCL++ IN GEANT4}
\section{RESULTS}
We have rewritten INUCL into C++ and tested the performance.
Here we combine INUCL models and HETC INC.
We give here summary of results. Each configuration consists of N=1000 events simulated with same energy etc. parameters.
\subsection{Particle multiplicities}
Multiplities for collisions between $p$ projectile ( $0.5~GeV< E <5.0~GeV$) and aluminium $Al$, iron $Fe$ and lead $Pb$ tragets (at rest) are listed in Figs. \ref{pAlMultiplicity} - \ref{pPbPionMultiplicity}.
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pAlMultiplicity.eps} }
\caption{Particle multiplicities for $(p, ^{27}Al$).}
\label{pAlMultiplicity}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pFeMultiplicity.eps} }
\caption{Particle multiplicities for $(p, ^{56}Fe$).}
\label{pFeMultiplicity}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbMultiplicity.eps} }
\caption{Particle multiplicities for $(p, ^{82}Pb$).}
\label{pPbMultiplicity}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbPionMultiplicity.eps} }
\caption{Pion multiplicities.}
\label{pPbPionMultiplicity}
\end{center}
\end{figure}
\subsection{Particle energies}
Figs. \ref{pPbProtonEnergy} - \ref{p500MeVPbProtonEnergy} give an summary of cascade products energy-levels.
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbProtonEnergy.eps} }
\caption{Average proton energies.}
\label{pPbProtonEnergy}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbNeutronEnergy.eps} }
\caption{Average neutron energies.}
\label{pPbNeutronEnergy}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbNucleonExitation.eps} }
\caption{Average nucleon exitation energy.}
\label{pPbNucleonExitation}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC p50MeVPbProtonEnergy.eps} }
\caption{Proton energy spectrum, when projectile particle (p) had an energy of $0.05~GeV$.}
\label{p50MeVPbProtonEnergy}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC p500MeVPbProtonEnergy.eps} }
\caption{Proton energy spectrum, when projectile particle (p) had an energy of $0.5~GeV$.}
\label{p500MeVPbProtonEnergy}
\end{center}
\end{figure}
\bibliographystyle{unsrt} % Options plain, unsrt, alpha, abbrv
%\bibstyle{plain}
%\begin{thebibliography}{99}
\bibliography{\AATOS texts/references/references.bib}
%\end{thebibliography}
\begin{appendix}
\section{PROJECT plan}
\begin{itemize}
\item we will continue testing INUCL++ against previous verison.
\item we reorganize the code is sutch mannet that integratin to Geant4
is smooth
\item before year 2002 will provide INUCL++ as a stanalone program,
or as an hadronic cascaded modules
(INC, pre-equilibrium, evaporation, fission) in Geant4.
\end{itemize}
\section{UML DIAGRAMS}
Preliminary suggestion for Inucl class interface to Geant4 cascade, pre-equilibrium
and evaporation modules.
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC cascadeUml.eps} }
\caption{General class structure for Inucl INC model.}
\label{massPb}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{preEquilibriumUml.eps} }
\caption{General class structure for Inucl pre-equilibrium model.}
\label{massPb}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{evaporationUml.eps} }
\caption{General class structure for Inucl evaporation/fission model.}
\label{massPb}
\end{center}
\end{figure}
\section{DOWNLOADING INUCL++}
INUCL++ is downloadable from INUCL homepage at
http://cern.ch/aatos.heikkinen/inucl
\scriptsize
\begin{verbatim}
\end{verbatim}
\normalsize
\section{OVERVIEW OF GEANT4 INUCL ACTIVITIES 2001-2002 }
\subsection{General}
Inside LHC Programme Software and Physics project Geant4 activities are under catecory {\it Simulation and event recosntruction}.
In 2001 HIP joined as participating institute the worl wide Geant4 collaboration with the major responsibility for development and maintenance of the nuclear evaporation and intra-nuclear cascade processes.
Two major codes HETC and INUCL are to be implemented and developed for Geant4 hadronic processes.
The conversion of the hadronic evaporation processes of HETC code to Geant4 was completed in 2001 and good progress was made in the Object-Oriented implementation of the intra-nuclear cascade processes.
For another important nuclear Maonte Carlo code, INUCL, an object oriented model was prepared, containing models for intra-nuclear cascade, pre-equilibrium state, fission and evaporation.
Year 2002 started with implementation of INUCL++ as a standalone software.
A preliminary version of architecture using INUCL++ intra-nuclear model. It also integrates HETC cascades and utilites Geant4 hadronic models frameworks.
\subsection{ABOUT GEANT4}
Geant4 represents one of the largest and most ambitious projects of geographically-distributed software development and large-scale object-oriented systems.
\subsection{COLLABORATION TSB AND CB WORK}
In 2001 HIP joined as participating institute the worl wide Geant4 collaboration with the major responsibility for development and maintenance of the nuclear evaporation and intra-nuclear cascade processes.
Our contribution in TSB and CB will be focused in near future to initiatives and coordination of hadronic cascade framework inside Geant4 hadronic framework.
\subsection{INCUL}
\subsubsection{INTORODUCTION TO INUCL}
INUCL++ is an object oriented implementation of Monte Carlo transport code INUCL for computing the properties of high-energy hadronic cascades in matter.
The functionality of INUCL++ is divided into intranuclear cascade, pre-equilibrium, fission, and evaporation parts.
The stand-alone version INUCL++ is comparable to codes such as HETC and LAHET \cite{titarenko99}.
\subsubsection{INUCL++}
We have made independent version INUCL++ using OO methods.
Architecture of INUCL++ intra-nuclear model plays an important role in our Geant4 work, since we use it also for HETC cascades modelling and as an platform to form a general framework for cascading model.
\subsection{PLANS FOR YEAR 2002}
\begin{itemize}
\item INUCL cascade model introduced to Geant4
\item We also aim to have significant progress on pre-equilibrium, fission models.
\end{itemize}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{massPb.eps2} }
\caption{::: Pb from 1 GeV .}
\label{massPb}
\end{center}
\end{figure}
\subsection{HIP Geant4 activities 2001-2002}
General:
\begin{itemize}
\item In 2001 HIP joined as participating institute the world wide Geant4 collaboration
\item Responsibility for development and maintenance of the nuclear evaporation and intra-nuclear cascade processes.
\item Two major codes HETC and INUCL are to be implemented and developed for Geant4 hadronic processes.
\end{itemize}
Research activities:
\begin{itemize}
\item Participation to Geant4 TSB and CB meetings
\item The conversion of the hadronic evaporation processes of HETC code to Geant4 was completed in 2001
\item Good progress was made in the Object-Oriented implementation of the intra-nuclear cascade processes
\item An object oriented model of INUCL was prepared, containing models for intra-nuclear cascade, pre-equilibrium state, fission and evaporation
\item Implementation of INUCL++ as a standalone software was finalized
\item Prototype for cascading framework was prepared using experience gained from INUCL OO design
\end{itemize}
Future plans:
\begin{itemize}
\item INUCL cascade model introduced to Geant4
\item Fully integration of HETC intra nuclear cascade -model and Geant4.
\item Significant progress on HETC and INUCL pre-equilibrium and fission models.
\item Introduction of general cascade framework to Geant4 hadronic models
\end{itemize}
\section{SAMPLE RUN RESULT}
\scriptsize
\begin{verbatim}
Number of events 100000
average multiplicity 21.5523
average proton number 3.53569
average neutron number 14.5048
average nucleon Ekin 0.0321547
average proton Ekin 0.0848587
average neutron Ekin 0.0193075
average pion number 0.3036
average pion Ekin 0.132491
average pi+ 0.1165
average pi- 0.058
average pi0 0.1291
average A 126.891
average Z 53.1615
average Exitation Energy 0.0258312
average num of fragments 1.69988
fission prob. 0.0117 c.sec 20.592
=====================================================
********** Izotop analysis ******************
++++++++++++++++++++++++++++++++++++++++++++++++++++++++
**** izotop Z **** 0
A 1 exp.cs 33520 err 12.4
sim. cs 30536.4 err 23.1827
ratio 0.910989 err 0.000769346
simulated production rate 17.3502
A 0 exp.cs 217.4 err 1.22
sim. cs 256.749 err 2.12574
ratio 1.181 err 0.0118124
simulated production rate 0.14588
not found in simulations 0
not found in exper: 0
simulated production rate 17.3502
simulated production rate 0.14588
matched 2 CHSQ 58.3536
raw chsq 13620.6
average ratio 1.04599 err 0.00629088
lhood 1.14436
exper. cs 33737.4 err 13.62
inucl. cs 30793.1 err 25.3085
++++++++++++++++++++++++++++++++++++++++++++++++++++++++
++++++++++++++++++++++++++++++++++++++++++++++++++++++++
**** izotop Z **** 1
A 1 exp.cs 7645 err 6.08
sim. cs 6801.24 err 10.9408
ratio 0.889632 err 0.00159645
simulated production rate 3.86434
A 0 exp.cs 109.4 err 0.96
sim. cs 226.195 err 1.99525
ratio 2.0676 err 0.0257258
simulated production rate 0.12852
not found exper.: A 2 exp.cs 658.7 err 4.2
not found exper.: A 3 exp.cs 338.6 err 3.1
not found in simulations 2
not found in exper: 0
simulated production rate 3.86434
simulated production rate 0.12852
matched 2 CHSQ 40.3162
raw chsq 6501.58
average ratio 1.47862 err 0.0136611
lhood 1.68244
exper. cs 8751.7 err 14.34
inucl. cs 7027.43 err 12.9361
\end{verbatim}
\normalsize
\section{WORKING DOCUMENT}
\subsection{15.7.2002}
\subsection{11.7.2002}
Now platform is ready. G4 and subcodes are organized and compiles. It is time to do actual interface.
Plan for today work 13-15 and 17-20. Build solid understanding of interface. And build it using tests.
\begin{itemize}
\item to do: ApplyYout self seciton CascadeInterfaceen, koncretic conversion between system nucleust and particles, study more interfacing, write towards working interface
\item KineticTrack is starting point for us.
\item Study G4VIntraNuclearTransport (base class G4HadronicInteraction, G4KineticTrack, G4VParticleChange, G4ReactionProductVector) class. And kinetic model. G4TheoFSGenerator steers the collaboration between hadronic generator and intra-nuclear transport
\item Methods in CascadeInteface : {\tt G4VParticleChange* ApplyYourself(const G4Track\& aTrack, G4Nucleus\& theNucleus);
G4ReactionProductVector* Propagate(G4KineticTrackVector* theSecondaries, G4V3DNucleus* theNucleus);} G4ReactionProductVector ok also for G4VParticleChange
\item For use of ApplyYourself see G4PreCompoundModel
\item
\end{itemize}
\subsection{10.7.2002}
\begin{itemize}
\item {\bf}: localised files (inucl cascade code at {\tt html/inucl/inucl++/demo},
hetc code at {\tt html/geant4/geant4/source/processes/ hadronic/models/cascade/cascade},
documentation {\tt html/inucl/doc}).
There is also another g4 version at {\tt html/geant4/geant4.3.1 })
\item studied g4 hadronic cascade interface.
\item {\bf all code and documentation in one place} {\tt html/geant4/geant4/source/processes/ hadronic/models/cascade/cascade}
\item general plan: {\bf thursday} put cascade code to g4 installation (+), make compile (+), study interface structure (+), make small testing (+),
{\bf friday} create real interface,
{\bf sunday} create inteface, and test basics (modify test13 hadronic testing)
{\bf monday morning at 8} co g4 at cern, pack {\tt hadronic/models/cascade}, replace cascade files, add new ones, and commit. Mail hpw. Start holiday at 10 am.
\item cascading basic structure: {\tt G4Collider (base),
G4ElementaryParticlCollider,
G4IntraNucleiCollider (:G4Collider, has G4ElementaryParticlCollider, ),
G4NucleiModel (initializes cascade,zones, boundary trasitions, fermi energy, density, potential),
G4InucleNuclei/G4HETCNuclei (A, Z, kinetic energy, mass formula, exiton configuration) }
\item change G4vector to vector:
\item {\tt G4InuclCollider} does the lining of different models inside collision with method command {\tt collide(bull, targ)}
\item {\tt G4IntraNucleiCascader} does the actual cascading. I starts by setting elementary particel cascader {\tt G4IntraNucleiCascader* incascader-> setElementaryParticleCollider( G4ElementaryParticleCollider*)}
\item The actual cascading is then done: {\tt theIntraNucleiCascader-> collide(\&nbullet, \&ntarget);}
\item finally, laboratory frame change, and some other organizational things happen
\item g4 inc base class is defined in models/generator/ management/include/ G4VIntraNuclearTransportModel.hh
\item INC model is set by G4TheoFSGenerator (: public G4HadronicInteraction) by method: {\tt void SetTransport( G4VIntraNuclearTransportModel *const value);}
\end{itemize}
\subsection{10.6.2002}
\begin{itemize}
\item {\bf compilation}: made compilation faster (now takes 45 seconds) by tunig compiler setting and include-statements
\item {\bf sample run}: result from original C++ test are saved to this document as sample run.
\item {\bf compilation}: fixed writing errors, so code now compiles
\item {\bf manual pages}: tempalte for manual pages copied to this document from GEANT4 ninematic model manual
\end{itemize}
\subsection{7.6.2002}
\begin{itemize}
\item {\bf document template}: Added new style and collected material to this documet. Rethinking chapter organization.
\item {\bf picture rezise}: {\tt convert x.ps x.eps2}
\item {\bf new references}: Some text added fron new sources
\end{itemize}
\end{appendix}
%\end{document}
% end of file
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/DeviceCMYK setcolorspace
<<
/ImageType 1
/Width columns
/Height rows
/BitsPerComponent 8
/Decode [0 1 0 1 0 1 0 1]
/ImageMatrix [columns 0 0 rows neg 0 rows]
compression 0 gt
{ /DataSource pixel_stream }
{ /DataSource pixel_stream /RunLengthDecode filter } ifelse
>> image
} ifelse
} bind def
/PseudoClassImage
{
%
% Display a PseudoClass image.
%
% Parameters:
% colors: number of colors in the colormap.
%
currentfile buffer readline pop
token pop /colors exch def pop
colors 0 eq
{
%
% Image is grayscale.
%
/DeviceGray setcolorspace
<<
/ImageType 1
/Width columns
/Height rows
/BitsPerComponent 1
/Decode [0 1]
/ImageMatrix [columns 0 0 rows neg 0 rows]
compression 0 gt
{ /DataSource pixel_stream }
{
/DataSource pixel_stream
<<
/K -1
/Columns columns
/Rows rows
>> /CCITTFaxDecode filter
} ifelse
>> image
}
{
%
% Parameters:
% colormap: red, green, blue color packets.
%
/colormap colors 3 mul string def
currentfile colormap readhexstring pop pop
[ /Indexed /DeviceRGB colors 1 sub colormap ] setcolorspace
<<
/ImageType 1
/Width columns
/Height rows
/BitsPerComponent 8
/Decode [0 255]
/ImageMatrix [columns 0 0 rows neg 0 rows]
compression 0 gt
{ /DataSource pixel_stream }
{ /DataSource pixel_stream /RunLengthDecode filter } ifelse
>> image
} ifelse
} bind def
/DisplayImage
{
%
% Display a DirectClass or PseudoClass image.
%
% Parameters:
% x & y translation.
% x & y scale.
% label pointsize.
% image label.
% image columns & rows.
% class: 0-DirectClass or 1-PseudoClass.
% colorspace: 0-RGB or 1-CMYK.
% compression: 0-RunlengthEncodedCompression or 1-NoCompression.
% hex color packets.
%
gsave
currentfile buffer readline pop
token pop /x exch def
token pop /y exch def pop
x y translate
currentfile buffer readline pop
token pop /x exch def
token pop /y exch def pop
currentfile buffer readline pop
token pop /pointsize exch def pop
/Helvetica findfont pointsize scalefont setfont
x y scale
currentfile buffer readline pop
token pop /columns exch def
token pop /rows exch def pop
currentfile buffer readline pop
token pop /class exch def pop
currentfile buffer readline pop
token pop /colorspace exch def pop
currentfile buffer readline pop
token pop /compression exch def pop
class 0 gt { PseudoClassImage } { DirectClassImage } ifelse
grestore
} bind def
%%EndProlog
%%Page: 1 1
%%PageBoundingBox: 0 0 611 791
userdict begin
%%BeginData:
DisplayImage
0 0
612 792
12
612 792
1
0
0
144
ffffff
787878
4b4b4b
585858
393939
474747
484848
666666
bbbbbb
8a8a8a
414141
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999999
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000000
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2b2b2b
727272
7c7c7c
c0c0c0
a4a4a4
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source/processes/hadronic/models/cascade/doc/preEquilibriumUml.eps
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source/processes/hadronic/models/cascade/evaporation/doc/evaporation.mdl
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source/processes/hadronic/models/cascade/evaporation/doc/evaporation.mdl.eps
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source/processes/hadronic/models/cascade/evaporation/include/G4BertiniEvaporation.hh
+3 -3
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@@ -53,12 +53,12 @@ public:
private:
G4int verboseLevel;
G4std::vector< G4BertiniEvaporationChannel * > channelVector;
void fillResult( G4std::vector< G4DynamicParticle * > secondaryParticleVector,
std::vector< G4BertiniEvaporationChannel * > channelVector;
void fillResult( std::vector< G4DynamicParticle * > secondaryParticleVector,
G4FragmentVector * aResult );
void splitBe8( const G4double E,
const G4ThreeVector boost,
G4std::vector< G4DynamicParticle * > & secondaryParticleVector);
std::vector< G4DynamicParticle * > & secondaryParticleVector);
void isotropicCosines( G4double & u, G4double & v,G4double & w );
};
source/processes/hadronic/models/cascade/evaporation/src/G4BEChargedChannel.cc
+4 -4
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@@ -64,9 +64,9 @@ void G4BEChargedChannel::calculateProbability()
G4double levelParam = getLevelDensityParameter();
G4double s = 2 * sqrt( levelParam * ( excitationEnergy - getThresh() - correction ) );
G4double constant = A / 2 * ( 2 * spin + 1 ) * ( 1 + coulombFactor() );
G4double eye1 = ( pow( s, 2 ) - 3 * s + 3 ) / ( 4 * pow( levelParam, 2 ) ) * exp( s );
G4double eye1 = ( pow( s, 2. ) - 3 * s + 3 ) / ( 4 * pow( levelParam, 2. ) ) * exp( s );
emissionProbability = constant * pow( residualA, 0.6666666 ) * eye1;
emissionProbability = constant * pow( G4double(residualA), 0.6666666 ) * eye1;
if ( verboseLevel >= 6 )
G4cout << "G4BEChargedChannel : calculateProbability for " << getName() << G4endl
@@ -100,8 +100,8 @@ G4double G4BEChargedChannel::sampleKineticEnergy()
// randExp2 = RandExponential::shoot( 1 );
// levelParam = getLevelDensityParameter();
// s = 2 * sqrt( levelParam * ( excitationEnergy - getThresh() - correction ) );
// kineticEnergyAv = 2 * ( pow( s, 3 ) - 6.0 * pow( s, 2 ) + 15.0 * s - 15.0 ) /
// ( ( 2.0 * pow( s, 2 ) - 6.0 * s + 6.0 ) * levelParam );
// kineticEnergyAv = 2 * ( pow( s, 3. ) - 6.0 * pow( s, 2. ) + 15.0 * s - 15.0 ) /
// ( ( 2.0 * pow( s, 2. ) - 6.0 * s + 6.0 ) * levelParam );
// kineticEnergy = 0.5 * ( randExp1 + randExp2 ) * kineticEnergyAv + getThresh() - getQ();
source/processes/hadronic/models/cascade/evaporation/src/G4BENeutronChannel.cc
+7 -7
View File
@@ -75,12 +75,12 @@ void G4BENeutronChannel::calculateProbability()
const G4double levelParam = getLevelDensityParameter();
const G4double s = 2 * sqrt( levelParam * ( excitationEnergy - getThresh() - correction ) );
const G4double temp = ( pow( s, 2 ) - 3 * s + 3 ) / ( 4 * pow( levelParam, 2 ) )
+ beta() * ( s - 1 ) / ( 2 * levelParam );
// const G4double temp = ( pow( s, 2. ) - 3 * s + 3 ) / ( 4 * pow( levelParam, 2. ) )
// + beta() * ( s - 1 ) / ( 2 * levelParam );
const G4double eye0 = exp( s ) * ( s - 1 ) / ( 2 * levelParam );
const G4double eye1 = ( pow( s, 2 ) - 3*s +3 ) * exp( s ) / ( 4 * pow( levelParam, 2 ) ) ;
const G4double eye1 = ( pow( s, 2. ) - 3*s +3 ) * exp( s ) / ( 4 * pow( levelParam, 2. ) ) ;
emissionProbability = pow( residualA, 0.666666 ) * alpha() * ( eye1 + beta() * eye0 );
emissionProbability = pow( G4double(residualA), 0.666666 ) * alpha() * ( eye1 + beta() * eye0 );
if ( verboseLevel >= 6 )
G4cout << "G4BENeutronChannel : calculateProbability " << G4endl
@@ -122,9 +122,9 @@ G4double G4BENeutronChannel::sampleKineticEnergy()
// levelParam = getLevelDensityParameter();
// s = 2 * sqrt( levelParam * ( excitationEnergy - getThresh() - correction ) );
// eye0 = 0.5 * ( s - 1 ) * exp( s ) / levelParam;
// eye1 = ( pow( s, 2 ) - 3*s + 3 ) * exp( s ) / ( 4 * pow( levelParam, 2 ) );
// kineticEnergyAv = 2 * ( pow( s, 3 ) - 6.0 * pow( s, 2 ) + 15.0 * s - 15.0 ) /
// ( ( 2.0 * pow( s, 2 ) - 6.0 * s + 6.0 ) * levelParam );
// eye1 = ( pow( s, 2. ) - 3*s + 3 ) * exp( s ) / ( 4 * pow( levelParam, 2. ) );
// kineticEnergyAv = 2 * ( pow( s, 3. ) - 6.0 * pow( s, 2. ) + 15.0 * s - 15.0 ) /
// ( ( 2.0 * pow( s, 2. ) - 6.0 * s + 6.0 ) * levelParam );
// kineticEnergyAv = ( kineticEnergyAv + beta() ) / ( 1.0 + beta() * eye0
// / eye1 );
source/processes/hadronic/models/cascade/evaporation/src/G4BertiniEvaporation.cc
+6 -6
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@@ -70,7 +70,7 @@ void G4BertiniEvaporation::setVerboseLevel( const G4int verbose )
verboseLevel = verbose;
// Update verbose level to all evaporation channels.
G4std::vector< G4BertiniEvaporationChannel * >::iterator iChannel = channelVector.begin();
std::vector< G4BertiniEvaporationChannel * >::iterator iChannel = channelVector.begin();
for ( ; iChannel != channelVector.end() ; *iChannel++ )
( *iChannel )->setVerboseLevel( verboseLevel );
}
@@ -89,7 +89,7 @@ G4FragmentVector * G4BertiniEvaporation::BreakItUp( G4LayeredNucleus & nucleus )
G4double mRes; // Mass of residual nucleus.
G4ThreeVector nucleusMomentumVector;
G4DynamicParticle *pEmittedParticle;
G4std::vector< G4DynamicParticle * > secondaryParticleVector;
std::vector< G4DynamicParticle * > secondaryParticleVector;
G4FragmentVector * result = new G4FragmentVector;
// Read properties of the nucleus.
@@ -115,7 +115,7 @@ G4FragmentVector * G4BertiniEvaporation::BreakItUp( G4LayeredNucleus & nucleus )
// Initialize evaporation channels and calculate sum of emission
// probabilities.
G4std::vector< G4BertiniEvaporationChannel * >::iterator iChannel = channelVector.begin();
std::vector< G4BertiniEvaporationChannel * >::iterator iChannel = channelVector.begin();
totalProbability = 0;
for ( ; iChannel != channelVector.end() ; *iChannel++ )
{
@@ -177,7 +177,7 @@ G4FragmentVector * G4BertiniEvaporation::BreakItUp( G4LayeredNucleus & nucleus )
const G4int zRes = nucleusZ - pSelectedChannel->getParticleZ();
const G4int aRes = nucleusA - pSelectedChannel->getParticleA();
const G4double eBind = G4NucleiProperties::GetBindingEnergy( aRes, zRes ); // Binding energy of the nucleus.
// const G4double eBind = G4NucleiProperties::GetBindingEnergy( aRes, zRes ); // Binding energy of the nucleus.
mRes = G4NucleiProperties::GetAtomicMass( aRes, zRes ); // Mass of the target nucleus
// In HETC88:
// eBind = Z * (-0.78244) + A * 8.36755 - cameron ( A , Z );
@@ -328,7 +328,7 @@ G4FragmentVector * G4BertiniEvaporation::BreakItUp( G4LayeredNucleus & nucleus )
void G4BertiniEvaporation::splitBe8( const G4double E,
const G4ThreeVector boostToLab,
G4std::vector< G4DynamicParticle * > & secondaryParticleVector )
std::vector< G4DynamicParticle * > & secondaryParticleVector )
{
G4double kineticEnergy;
G4double u;
@@ -376,7 +376,7 @@ void G4BertiniEvaporation::splitBe8( const G4double E,
}
void G4BertiniEvaporation::fillResult( G4std::vector<G4DynamicParticle *> secondaryParticleVector,
void G4BertiniEvaporation::fillResult( std::vector<G4DynamicParticle *> secondaryParticleVector,
G4FragmentVector * aResult )
{
// Fill the vector pParticleChange with secondary particles stored in vector.
source/processes/hadronic/models/cascade/evaporation/src/G4BertiniEvaporationChannel.cc
+2 -2
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@@ -159,7 +159,7 @@ G4double G4BertiniEvaporationChannel::getCoulomb()
// In HETC88 this factor was 0.88235, perhaps due to different r0
G4double coulomb = factor * particleZ * qmFactor() * residualZ /
( pow( residualA, 0.33333333 ) + rho ) * MeV;
( pow( G4double(residualA), 0.33333333 ) + rho ) * MeV;
if ( verboseLevel >= 10 )
G4cout << " G4BertiniEvaporationChannel::getThresh() " << G4endl
@@ -192,7 +192,7 @@ G4double G4BertiniEvaporationChannel::getLevelDensityParameter()
G4double y0 = 1.5;
G4double temp = ( residualA - 2.0 * residualZ ) / residualA;
G4double smallA = residualA * ( 1.0 + y0 * pow( temp, 2 ) ) / b0 / MeV;
G4double smallA = residualA * ( 1.0 + y0 * pow( temp, 2. ) ) / b0 / MeV;
// In HETC98 b0 = b0(E).
source/processes/hadronic/models/cascade/pre_compound/GNUmakefile
+1 -3
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@@ -1,4 +1,4 @@
# $Id: GNUmakefile,v 1.2 1999/11/24 14:14:59 miheikki Exp $
# $Id: GNUmakefile,v 1.3 2003/06/18 13:24:26 gcosmo Exp $
# -----------------------------------------------------------
# GNUmakefile for hadronic library. Gabriele Cosmo, 18/9/96.
# -----------------------------------------------------------
@@ -11,8 +11,6 @@ endif
include $(G4INSTALL)/config/architecture.gmk
G4TMPDIR = $(G4TMP)/$(G4SYSTEM)/$(name)
CPPFLAGS += -I$(G4BASE)/global/management/include \
-I$(G4BASE)/global/HEPRandom/include \
-I$(G4BASE)/global/HEPGeometry/include \
source/processes/hadronic/models/cascade/pre_compound/include/G4PreEquilibrium.hh
+4 -4
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@@ -21,8 +21,8 @@
// ********************************************************************
//
//
// $Id: G4PreEquilibrium.hh,v 1.9 2001/07/11 10:03:54 gunter Exp $
// GEANT4 tag $Name: geant4-05-01 $
// $Id: G4PreEquilibrium.hh,v 1.10 2003/06/16 17:03:58 gunter Exp $
// GEANT4 tag $Name: geant4-05-02 $
//
// Hadronic Process: Pre-equilibrium HETC
// Joseph L. Chuma, TRIUMF, 24-Mar-2000
@@ -33,7 +33,7 @@
#include "globals.hh"
#include "G4DynamicParticle.hh"
#include "G4Nucleus.hh"
#include "g4std/vector"
#include <vector>
class G4PreEquilibrium
{
@@ -70,7 +70,7 @@
G4int ip4; // values from 0 to N
};
#define G4Vector G4std::vector
#define G4Vector std::vector
typedef G4Vector< G4DynamicParticle* > DPvector;
typedef G4Vector< G4double > Dvector;
typedef G4Vector< G4int > Ivector;
source/processes/hadronic/models/cascade/pre_compound/src/G4PreEquilibrium.cc
+1 -1
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@@ -22,7 +22,7 @@
//
//
// $Id: G4PreEquilibrium.cc,v 1.9 2001/07/11 10:03:55 gunter Exp $
// GEANT4 tag $Name: geant4-05-01 $
// GEANT4 tag $Name: geant4-05-02 $
//
// Hadronic Process: Pre-equilibrium HETC
// Joseph L. Chuma, TRIUMF, 24-Mar-2000