706 lines
33 KiB
Plaintext
706 lines
33 KiB
Plaintext
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*************************************************************
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Geant4 version Name: global-V08-00-04 (30-June-2006)
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Copyright : Geant4 Collaboration
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Reference : NIM A 506 (2003), 250-303
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WWW : http://cern.ch/geant4
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*************************************************************
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PhotInPrimaryGeneratorAction::Constructor: part=gamma, E=100
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Visualization Manager instantiating...
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Visualization Manager initialising...
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Registering graphics systems...
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PhotInVisManager::RegisterGraphicsSystems: chosen graphics systems
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Current available graphics systems are:
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ASCIITree (ATree)
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DAWNFILE (DAWNFILE)
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GAGTree (GAGTree)
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G4HepRepFile (HepRepFile)
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G4HepRep (HepRepXML)
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RayTracer (RayTracer)
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VRML1FILE (VRML1FILE)
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VRML2FILE (VRML2FILE)
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You have successfully registered the following graphics systems.
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Current available graphics systems are:
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ASCIITree (ATree)
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DAWNFILE (DAWNFILE)
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GAGTree (GAGTree)
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G4HepRepFile (HepRepFile)
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G4HepRep (HepRepXML)
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RayTracer (RayTracer)
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VRML1FILE (VRML1FILE)
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VRML2FILE (VRML2FILE)
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Registering model factories...
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G4VisManager: No model factories registered with G4VisManager.
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G4VisManager::RegisterModelFactories() should be overridden in derived
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class. See G4VisExecutive for an example.
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You have successfully registered the following model factories.
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Registered model factories:
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None
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Registered models:
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None
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Registered filter factories:
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None
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Registered filters:
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None
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PhotInPrimaryGeneratorAction::SetDetector: is called
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/run/verbose 1
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##/tracking/verbose 6
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/run/initialize
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PhotInPhysicsList::ConstructProcess: is called
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PhotInPhysList::ConstructProcess: Part=B+
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PhotInPhysList::ConstructProcess: Part=B-
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PhotInPhysList::ConstructProcess: Part=B0
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PhotInPhysList::ConstructProcess: Part=Bs0
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PhotInPhysList::ConstructProcess: Part=D+
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PhotInPhysList::ConstructProcess: Part=D-
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PhotInPhysList::ConstructProcess: Part=D0
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PhotInPhysList::ConstructProcess: Part=Ds+
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PhotInPhysList::ConstructProcess: Part=Ds-
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PhotInPhysList::ConstructProcess: Part=GenericIon
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PhotInPhysList::ConstructProcess: Part=He3
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PhotInPhysList::ConstructProcess: Part=J/psi
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PhotInPhysList::ConstructProcess: Part=N(1440)+
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PhotInPhysList::ConstructProcess: Part=N(1440)0
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PhotInPhysList::ConstructProcess: Part=N(1520)+
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PhotInPhysList::ConstructProcess: Part=N(1520)0
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PhotInPhysList::ConstructProcess: Part=N(1535)+
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PhotInPhysList::ConstructProcess: Part=N(1535)0
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PhotInPhysList::ConstructProcess: Part=N(1650)+
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PhotInPhysList::ConstructProcess: Part=N(1650)0
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PhotInPhysList::ConstructProcess: Part=N(1675)+
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PhotInPhysList::ConstructProcess: Part=N(1675)0
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PhotInPhysList::ConstructProcess: Part=N(1680)+
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PhotInPhysList::ConstructProcess: Part=N(1680)0
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PhotInPhysList::ConstructProcess: Part=N(1700)+
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PhotInPhysList::ConstructProcess: Part=N(1700)0
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PhotInPhysList::ConstructProcess: Part=N(1710)+
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PhotInPhysList::ConstructProcess: Part=N(1710)0
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PhotInPhysList::ConstructProcess: Part=N(1720)+
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PhotInPhysList::ConstructProcess: Part=N(1720)0
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PhotInPhysList::ConstructProcess: Part=N(1900)+
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PhotInPhysList::ConstructProcess: Part=N(1900)0
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PhotInPhysList::ConstructProcess: Part=N(1990)+
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PhotInPhysList::ConstructProcess: Part=N(1990)0
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PhotInPhysList::ConstructProcess: Part=N(2090)+
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PhotInPhysList::ConstructProcess: Part=N(2090)0
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PhotInPhysList::ConstructProcess: Part=N(2190)+
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PhotInPhysList::ConstructProcess: Part=N(2190)0
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PhotInPhysList::ConstructProcess: Part=N(2220)+
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PhotInPhysList::ConstructProcess: Part=N(2220)0
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PhotInPhysList::ConstructProcess: Part=N(2250)+
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PhotInPhysList::ConstructProcess: Part=N(2250)0
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PhotInPhysList::ConstructProcess: Part=a0(1450)+
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PhotInPhysList::ConstructProcess: Part=a0(1450)-
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PhotInPhysList::ConstructProcess: Part=a0(1450)0
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PhotInPhysList::ConstructProcess: Part=a0(980)+
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PhotInPhysList::ConstructProcess: Part=a0(980)-
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PhotInPhysList::ConstructProcess: Part=a0(980)0
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PhotInPhysList::ConstructProcess: Part=a1(1260)+
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PhotInPhysList::ConstructProcess: Part=a1(1260)-
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PhotInPhysList::ConstructProcess: Part=a1(1260)0
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PhotInPhysList::ConstructProcess: Part=a2(1320)+
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PhotInPhysList::ConstructProcess: Part=a2(1320)-
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PhotInPhysList::ConstructProcess: Part=a2(1320)0
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PhotInPhysList::ConstructProcess: Part=alpha
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PhotInPhysList::ConstructProcess: Part=anti_B0
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PhotInPhysList::ConstructProcess: Part=anti_Bs0
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PhotInPhysList::ConstructProcess: Part=anti_D0
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PhotInPhysList::ConstructProcess: Part=anti_N(1440)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1440)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1520)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1520)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1535)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1535)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1650)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1650)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1675)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1675)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1680)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1680)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1700)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1700)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1710)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1710)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1720)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1720)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1900)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1900)0
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PhotInPhysList::ConstructProcess: Part=anti_N(1990)+
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PhotInPhysList::ConstructProcess: Part=anti_N(1990)0
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PhotInPhysList::ConstructProcess: Part=anti_N(2090)+
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PhotInPhysList::ConstructProcess: Part=anti_N(2090)0
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PhotInPhysList::ConstructProcess: Part=anti_N(2190)+
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PhotInPhysList::ConstructProcess: Part=anti_N(2190)0
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PhotInPhysList::ConstructProcess: Part=anti_N(2220)+
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PhotInPhysList::ConstructProcess: Part=anti_N(2220)0
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PhotInPhysList::ConstructProcess: Part=anti_N(2250)+
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PhotInPhysList::ConstructProcess: Part=anti_N(2250)0
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PhotInPhysList::ConstructProcess: Part=anti_b_quark
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PhotInPhysList::ConstructProcess: Part=anti_c_quark
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PhotInPhysList::ConstructProcess: Part=anti_d_quark
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PhotInPhysList::ConstructProcess: Part=anti_dd1_diquark
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PhotInPhysList::ConstructProcess: Part=anti_delta(1600)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1600)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1600)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1600)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1620)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1620)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1620)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1620)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1700)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1700)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1700)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1700)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1900)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1900)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1900)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1900)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1905)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1905)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1905)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1905)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1910)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1910)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1910)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1910)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1920)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1920)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1920)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1920)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1930)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1930)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1930)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1930)0
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PhotInPhysList::ConstructProcess: Part=anti_delta(1950)+
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PhotInPhysList::ConstructProcess: Part=anti_delta(1950)++
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PhotInPhysList::ConstructProcess: Part=anti_delta(1950)-
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PhotInPhysList::ConstructProcess: Part=anti_delta(1950)0
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PhotInPhysList::ConstructProcess: Part=anti_delta+
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PhotInPhysList::ConstructProcess: Part=anti_delta++
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PhotInPhysList::ConstructProcess: Part=anti_delta-
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PhotInPhysList::ConstructProcess: Part=anti_delta0
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PhotInPhysList::ConstructProcess: Part=anti_k(1460)0
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PhotInPhysList::ConstructProcess: Part=anti_k0_star(1430)0
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PhotInPhysList::ConstructProcess: Part=anti_k1(1270)0
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PhotInPhysList::ConstructProcess: Part=anti_k1(1400)0
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PhotInPhysList::ConstructProcess: Part=anti_k2(1770)0
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PhotInPhysList::ConstructProcess: Part=anti_k2_star(1430)0
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PhotInPhysList::ConstructProcess: Part=anti_k2_star(1980)0
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PhotInPhysList::ConstructProcess: Part=anti_k3_star(1780)0
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PhotInPhysList::ConstructProcess: Part=anti_k_star(1410)0
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PhotInPhysList::ConstructProcess: Part=anti_k_star(1680)0
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PhotInPhysList::ConstructProcess: Part=anti_k_star0
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PhotInPhysList::ConstructProcess: Part=anti_kaon0
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PhotInPhysList::ConstructProcess: Part=anti_lambda
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1405)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1520)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1600)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1670)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1690)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1800)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1810)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1820)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1830)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(1890)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(2100)
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PhotInPhysList::ConstructProcess: Part=anti_lambda(2110)
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PhotInPhysList::ConstructProcess: Part=anti_lambda_c+
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PhotInPhysList::ConstructProcess: Part=anti_neutron
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PhotInPhysList::ConstructProcess: Part=anti_nu_e
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PhotInPhysList::ConstructProcess: Part=anti_nu_mu
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PhotInPhysList::ConstructProcess: Part=anti_nu_tau
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PhotInPhysList::ConstructProcess: Part=anti_omega-
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PhotInPhysList::ConstructProcess: Part=anti_omega_c0
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PhotInPhysList::ConstructProcess: Part=anti_proton
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PhotInPhysList::ConstructProcess: Part=anti_s_quark
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PhotInPhysList::ConstructProcess: Part=anti_sd0_diquark
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PhotInPhysList::ConstructProcess: Part=anti_sd1_diquark
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1385)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1385)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1385)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1660)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1660)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1660)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1670)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1670)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1670)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1750)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1750)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1750)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1775)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1775)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1775)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1915)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1915)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1915)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1940)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1940)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(1940)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma(2030)+
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PhotInPhysList::ConstructProcess: Part=anti_sigma(2030)-
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PhotInPhysList::ConstructProcess: Part=anti_sigma(2030)0
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PhotInPhysList::ConstructProcess: Part=anti_sigma+
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PhotInPhysList::ConstructProcess: Part=anti_sigma-
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PhotInPhysList::ConstructProcess: Part=anti_sigma0
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PhotInPhysList::ConstructProcess: Part=anti_sigma_c+
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PhotInPhysList::ConstructProcess: Part=anti_sigma_c++
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PhotInPhysList::ConstructProcess: Part=anti_sigma_c0
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PhotInPhysList::ConstructProcess: Part=anti_ss1_diquark
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PhotInPhysList::ConstructProcess: Part=anti_su0_diquark
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PhotInPhysList::ConstructProcess: Part=anti_su1_diquark
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PhotInPhysList::ConstructProcess: Part=anti_t_quark
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PhotInPhysList::ConstructProcess: Part=anti_u_quark
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PhotInPhysList::ConstructProcess: Part=anti_ud0_diquark
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PhotInPhysList::ConstructProcess: Part=anti_ud1_diquark
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PhotInPhysList::ConstructProcess: Part=anti_uu1_diquark
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PhotInPhysList::ConstructProcess: Part=anti_xi(1530)-
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PhotInPhysList::ConstructProcess: Part=anti_xi(1530)0
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PhotInPhysList::ConstructProcess: Part=anti_xi(1690)-
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PhotInPhysList::ConstructProcess: Part=anti_xi(1690)0
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PhotInPhysList::ConstructProcess: Part=anti_xi(1820)-
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PhotInPhysList::ConstructProcess: Part=anti_xi(1820)0
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PhotInPhysList::ConstructProcess: Part=anti_xi(1950)-
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PhotInPhysList::ConstructProcess: Part=anti_xi(1950)0
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PhotInPhysList::ConstructProcess: Part=anti_xi(2030)-
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PhotInPhysList::ConstructProcess: Part=anti_xi(2030)0
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PhotInPhysList::ConstructProcess: Part=anti_xi-
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PhotInPhysList::ConstructProcess: Part=anti_xi0
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PhotInPhysList::ConstructProcess: Part=anti_xi_c+
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PhotInPhysList::ConstructProcess: Part=anti_xi_c0
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PhotInPhysList::ConstructProcess: Part=b1(1235)+
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PhotInPhysList::ConstructProcess: Part=b1(1235)-
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PhotInPhysList::ConstructProcess: Part=b1(1235)0
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PhotInPhysList::ConstructProcess: Part=b_quark
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PhotInPhysList::ConstructProcess: Part=c_quark
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PhotInPhysList::ConstructProcess: Part=chargedgeantino
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PhotInPhysList::ConstructProcess: Part=d_quark
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PhotInPhysList::ConstructProcess: Part=dd1_diquark
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PhotInPhysList::ConstructProcess: Part=delta(1600)+
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PhotInPhysList::ConstructProcess: Part=delta(1600)++
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PhotInPhysList::ConstructProcess: Part=delta(1600)-
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PhotInPhysList::ConstructProcess: Part=delta(1600)0
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PhotInPhysList::ConstructProcess: Part=delta(1620)+
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PhotInPhysList::ConstructProcess: Part=delta(1620)++
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PhotInPhysList::ConstructProcess: Part=delta(1620)-
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PhotInPhysList::ConstructProcess: Part=delta(1620)0
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PhotInPhysList::ConstructProcess: Part=delta(1700)+
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PhotInPhysList::ConstructProcess: Part=delta(1700)++
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PhotInPhysList::ConstructProcess: Part=delta(1700)-
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PhotInPhysList::ConstructProcess: Part=delta(1700)0
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PhotInPhysList::ConstructProcess: Part=delta(1900)+
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PhotInPhysList::ConstructProcess: Part=delta(1900)++
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PhotInPhysList::ConstructProcess: Part=delta(1900)-
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PhotInPhysList::ConstructProcess: Part=delta(1900)0
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PhotInPhysList::ConstructProcess: Part=delta(1905)+
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PhotInPhysList::ConstructProcess: Part=delta(1905)++
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PhotInPhysList::ConstructProcess: Part=delta(1905)-
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PhotInPhysList::ConstructProcess: Part=delta(1905)0
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PhotInPhysList::ConstructProcess: Part=delta(1910)+
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PhotInPhysList::ConstructProcess: Part=delta(1910)++
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PhotInPhysList::ConstructProcess: Part=delta(1910)-
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PhotInPhysList::ConstructProcess: Part=delta(1910)0
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PhotInPhysList::ConstructProcess: Part=delta(1920)+
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PhotInPhysList::ConstructProcess: Part=delta(1920)++
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PhotInPhysList::ConstructProcess: Part=delta(1920)-
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PhotInPhysList::ConstructProcess: Part=delta(1920)0
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PhotInPhysList::ConstructProcess: Part=delta(1930)+
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PhotInPhysList::ConstructProcess: Part=delta(1930)++
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PhotInPhysList::ConstructProcess: Part=delta(1930)-
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PhotInPhysList::ConstructProcess: Part=delta(1930)0
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PhotInPhysList::ConstructProcess: Part=delta(1950)+
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PhotInPhysList::ConstructProcess: Part=delta(1950)++
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PhotInPhysList::ConstructProcess: Part=delta(1950)-
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PhotInPhysList::ConstructProcess: Part=delta(1950)0
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PhotInPhysList::ConstructProcess: Part=delta+
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PhotInPhysList::ConstructProcess: Part=delta++
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PhotInPhysList::ConstructProcess: Part=delta-
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PhotInPhysList::ConstructProcess: Part=delta0
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PhotInPhysList::ConstructProcess: Part=deuteron
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PhotInPhysList::ConstructProcess: Part=e+
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PhotInPhysList::ConstructProcess: Part=e-
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PhotInPhysList::ConstructProcess: Part=eta
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PhotInPhysList::ConstructProcess: Part=eta(1295)
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PhotInPhysList::ConstructProcess: Part=eta(1475)
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PhotInPhysList::ConstructProcess: Part=eta2(1645)
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PhotInPhysList::ConstructProcess: Part=eta2(1870)
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PhotInPhysList::ConstructProcess: Part=eta_prime
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PhotInPhysList::ConstructProcess: Part=f0(1370)
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PhotInPhysList::ConstructProcess: Part=f0(1500)
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PhotInPhysList::ConstructProcess: Part=f0(1710)
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PhotInPhysList::ConstructProcess: Part=f0(600)
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PhotInPhysList::ConstructProcess: Part=f0(980)
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PhotInPhysList::ConstructProcess: Part=f1(1285)
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PhotInPhysList::ConstructProcess: Part=f1(1420)
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PhotInPhysList::ConstructProcess: Part=f2(1270)
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PhotInPhysList::ConstructProcess: Part=f2(1810)
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PhotInPhysList::ConstructProcess: Part=f2(2010)
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PhotInPhysList::ConstructProcess: Part=f2_prime(1525)
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PhotInPhysList::ConstructProcess: Part=gamma
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PhotInPhysList::ConstructProcess: Part=geantino
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PhotInPhysList::ConstructProcess: Part=gluon
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PhotInPhysList::ConstructProcess: Part=h1(1170)
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PhotInPhysList::ConstructProcess: Part=h1(1380)
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PhotInPhysList::ConstructProcess: Part=k(1460)+
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PhotInPhysList::ConstructProcess: Part=k(1460)-
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PhotInPhysList::ConstructProcess: Part=k(1460)0
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PhotInPhysList::ConstructProcess: Part=k0_star(1430)+
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PhotInPhysList::ConstructProcess: Part=k0_star(1430)-
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PhotInPhysList::ConstructProcess: Part=k0_star(1430)0
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PhotInPhysList::ConstructProcess: Part=k1(1270)+
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PhotInPhysList::ConstructProcess: Part=k1(1270)-
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PhotInPhysList::ConstructProcess: Part=k1(1270)0
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PhotInPhysList::ConstructProcess: Part=k1(1400)+
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PhotInPhysList::ConstructProcess: Part=k1(1400)-
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PhotInPhysList::ConstructProcess: Part=k1(1400)0
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PhotInPhysList::ConstructProcess: Part=k2(1770)+
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PhotInPhysList::ConstructProcess: Part=k2(1770)-
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PhotInPhysList::ConstructProcess: Part=k2(1770)0
|
|
PhotInPhysList::ConstructProcess: Part=k2_star(1430)+
|
|
PhotInPhysList::ConstructProcess: Part=k2_star(1430)-
|
|
PhotInPhysList::ConstructProcess: Part=k2_star(1430)0
|
|
PhotInPhysList::ConstructProcess: Part=k2_star(1980)+
|
|
PhotInPhysList::ConstructProcess: Part=k2_star(1980)-
|
|
PhotInPhysList::ConstructProcess: Part=k2_star(1980)0
|
|
PhotInPhysList::ConstructProcess: Part=k3_star(1780)+
|
|
PhotInPhysList::ConstructProcess: Part=k3_star(1780)-
|
|
PhotInPhysList::ConstructProcess: Part=k3_star(1780)0
|
|
PhotInPhysList::ConstructProcess: Part=k_star(1410)+
|
|
PhotInPhysList::ConstructProcess: Part=k_star(1410)-
|
|
PhotInPhysList::ConstructProcess: Part=k_star(1410)0
|
|
PhotInPhysList::ConstructProcess: Part=k_star(1680)+
|
|
PhotInPhysList::ConstructProcess: Part=k_star(1680)-
|
|
PhotInPhysList::ConstructProcess: Part=k_star(1680)0
|
|
PhotInPhysList::ConstructProcess: Part=k_star+
|
|
PhotInPhysList::ConstructProcess: Part=k_star-
|
|
PhotInPhysList::ConstructProcess: Part=k_star0
|
|
PhotInPhysList::ConstructProcess: Part=kaon+
|
|
PhotInPhysList::ConstructProcess: Part=kaon-
|
|
PhotInPhysList::ConstructProcess: Part=kaon0
|
|
PhotInPhysList::ConstructProcess: Part=kaon0L
|
|
PhotInPhysList::ConstructProcess: Part=kaon0S
|
|
PhotInPhysList::ConstructProcess: Part=lambda
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1405)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1520)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1600)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1670)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1690)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1800)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1810)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1820)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1830)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(1890)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(2100)
|
|
PhotInPhysList::ConstructProcess: Part=lambda(2110)
|
|
PhotInPhysList::ConstructProcess: Part=lambda_c+
|
|
PhotInPhysList::ConstructProcess: Part=mu+
|
|
PhotInPhysList::ConstructProcess: Part=mu-
|
|
PhotInPhysList::ConstructProcess: Part=neutron
|
|
PhotInPhysList::ConstructProcess: Part=nu_e
|
|
PhotInPhysList::ConstructProcess: Part=nu_mu
|
|
PhotInPhysList::ConstructProcess: Part=nu_tau
|
|
PhotInPhysList::ConstructProcess: Part=omega
|
|
PhotInPhysList::ConstructProcess: Part=omega(1420)
|
|
PhotInPhysList::ConstructProcess: Part=omega(1650)
|
|
PhotInPhysList::ConstructProcess: Part=omega-
|
|
PhotInPhysList::ConstructProcess: Part=omega3(1670)
|
|
PhotInPhysList::ConstructProcess: Part=omega_c0
|
|
PhotInPhysList::ConstructProcess: Part=opticalphoton
|
|
PhotInPhysList::ConstructProcess: Part=phi
|
|
PhotInPhysList::ConstructProcess: Part=phi(1680)
|
|
PhotInPhysList::ConstructProcess: Part=phi3(1850)
|
|
PhotInPhysList::ConstructProcess: Part=pi(1300)+
|
|
PhotInPhysList::ConstructProcess: Part=pi(1300)-
|
|
PhotInPhysList::ConstructProcess: Part=pi(1300)0
|
|
PhotInPhysList::ConstructProcess: Part=pi+
|
|
PhotInPhysList::ConstructProcess: Part=pi-
|
|
PhotInPhysList::ConstructProcess: Part=pi0
|
|
PhotInPhysList::ConstructProcess: Part=pi2(1670)+
|
|
PhotInPhysList::ConstructProcess: Part=pi2(1670)-
|
|
PhotInPhysList::ConstructProcess: Part=pi2(1670)0
|
|
PhotInPhysList::ConstructProcess: Part=proton
|
|
PhotInPhysList::ConstructProcess: Part=rho(1450)+
|
|
PhotInPhysList::ConstructProcess: Part=rho(1450)-
|
|
PhotInPhysList::ConstructProcess: Part=rho(1450)0
|
|
PhotInPhysList::ConstructProcess: Part=rho(1700)+
|
|
PhotInPhysList::ConstructProcess: Part=rho(1700)-
|
|
PhotInPhysList::ConstructProcess: Part=rho(1700)0
|
|
PhotInPhysList::ConstructProcess: Part=rho+
|
|
PhotInPhysList::ConstructProcess: Part=rho-
|
|
PhotInPhysList::ConstructProcess: Part=rho0
|
|
PhotInPhysList::ConstructProcess: Part=rho3(1690)+
|
|
PhotInPhysList::ConstructProcess: Part=rho3(1690)-
|
|
PhotInPhysList::ConstructProcess: Part=rho3(1690)0
|
|
PhotInPhysList::ConstructProcess: Part=s_quark
|
|
PhotInPhysList::ConstructProcess: Part=sd0_diquark
|
|
PhotInPhysList::ConstructProcess: Part=sd1_diquark
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1385)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1385)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1385)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1660)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1660)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1660)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1670)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1670)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1670)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1750)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1750)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1750)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1775)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1775)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1775)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1915)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1915)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1915)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1940)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1940)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(1940)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma(2030)+
|
|
PhotInPhysList::ConstructProcess: Part=sigma(2030)-
|
|
PhotInPhysList::ConstructProcess: Part=sigma(2030)0
|
|
PhotInPhysList::ConstructProcess: Part=sigma+
|
|
PhotInPhysList::ConstructProcess: Part=sigma-
|
|
PhotInPhysList::ConstructProcess: Part=sigma0
|
|
PhotInPhysList::ConstructProcess: Part=sigma_c+
|
|
PhotInPhysList::ConstructProcess: Part=sigma_c++
|
|
PhotInPhysList::ConstructProcess: Part=sigma_c0
|
|
PhotInPhysList::ConstructProcess: Part=ss1_diquark
|
|
PhotInPhysList::ConstructProcess: Part=su0_diquark
|
|
PhotInPhysList::ConstructProcess: Part=su1_diquark
|
|
PhotInPhysList::ConstructProcess: Part=t_quark
|
|
PhotInPhysList::ConstructProcess: Part=tau+
|
|
PhotInPhysList::ConstructProcess: Part=tau-
|
|
PhotInPhysList::ConstructProcess: Part=triton
|
|
PhotInPhysList::ConstructProcess: Part=u_quark
|
|
PhotInPhysList::ConstructProcess: Part=ud0_diquark
|
|
PhotInPhysList::ConstructProcess: Part=ud1_diquark
|
|
PhotInPhysList::ConstructProcess: Part=uu1_diquark
|
|
PhotInPhysList::ConstructProcess: Part=xi(1530)-
|
|
PhotInPhysList::ConstructProcess: Part=xi(1530)0
|
|
PhotInPhysList::ConstructProcess: Part=xi(1690)-
|
|
PhotInPhysList::ConstructProcess: Part=xi(1690)0
|
|
PhotInPhysList::ConstructProcess: Part=xi(1820)-
|
|
PhotInPhysList::ConstructProcess: Part=xi(1820)0
|
|
PhotInPhysList::ConstructProcess: Part=xi(1950)-
|
|
PhotInPhysList::ConstructProcess: Part=xi(1950)0
|
|
PhotInPhysList::ConstructProcess: Part=xi(2030)-
|
|
PhotInPhysList::ConstructProcess: Part=xi(2030)0
|
|
PhotInPhysList::ConstructProcess: Part=xi-
|
|
PhotInPhysList::ConstructProcess: Part=xi0
|
|
PhotInPhysList::ConstructProcess: Part=xi_c+
|
|
PhotInPhysList::ConstructProcess: Part=xi_c0
|
|
PhotInPhysicsList::SetCuts: default cut length : 1 mm
|
|
/run/dumpRegion
|
|
|
|
Region <DefaultRegionForTheWorld> -- appears in <World> world volume
|
|
Materials : Vac
|
|
Production cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|
|
|
Region <Region0> -- appears in <World> world volume
|
|
Materials : Aluminium Scintillator
|
|
Production cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|
|
|
Region <Region1> -- appears in <World> world volume
|
|
Materials : Aluminium Scintillator
|
|
Production cuts : gamma 1 cm e- 1 cm e+ 1 cm
|
|
|
|
Region <Region2> -- appears in <World> world volume
|
|
Materials : Aluminium Scintillator
|
|
Production cuts : gamma 10 cm e- 10 cm e+ 10 cm
|
|
/PhotIn/projParticle pi+
|
|
PhotInPrimaryGeneratorAction::SetProjectileName:Before Name=pi+, oldName=gamma
|
|
PhotInPrimaryGeneratorAction::SetProjectileName: After Name=pi+
|
|
/PhotIn/projEnergy 100.
|
|
PhotInPrimaryGeneratorAction::SetProjectileEnergy: before E=100
|
|
PhotInPrimaryGeneratorAction::SetProjectileEnergy: before E=100
|
|
/run/beamOn 1
|
|
|
|
conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z;
|
|
sampling secondary e+e- according to the Bethe-Heitler model
|
|
tables are built for gamma
|
|
Lambda tables from 1.022 MeV to 100 GeV in 100 bins.
|
|
|
|
compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV
|
|
Sampling according Klein-Nishina model
|
|
tables are built for gamma
|
|
Lambda tables from 100 eV to 100 GeV in 90 bins.
|
|
|
|
phot: Total cross sections from Sandia parametrisation.
|
|
|
|
msc: Model variant of multiple scattering for e-
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
eIoni: tables are built for e-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Delta cross sections from Moller+Bhabha, good description from 1 KeV to 100 GeV.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
eBrem: tables are built for e-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Total cross sections from a parametrisation based on the EEDL data library.
|
|
Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
|
|
|
|
eIoni: tables are built for e+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Delta cross sections from Moller+Bhabha, good description from 1 KeV to 100 GeV.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
eBrem: tables are built for e+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Total cross sections from a parametrisation based on the EEDL data library.
|
|
Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
|
|
|
|
annihil: Heilter model of formula of annihilation into 2 photons
|
|
tables are built for e+
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
|
|
annihil: Heilter model of formula of annihilation into 2 photons
|
|
tables are built for e+
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
|
|
msc: Model variant of multiple scattering for proton
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
hIoni: tables are built for proton
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Scaling relation is used to proton dE/dx and range
|
|
Bether-Bloch model for Escaled > 2 MeV, ICRU49 parametrisation for protons below.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
msc: Model variant of multiple scattering for GenericIon
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
hIoni: tables are built for anti_proton
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Scaling relation is used to proton dE/dx and range
|
|
Bether-Bloch model for Escaled > 2 MeV, ICRU49 parametrisation for protons below.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
msc: Model variant of multiple scattering for mu+
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
muIoni: tables are built for mu+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
|
|
radiative corrections for E > 1 GeV
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
muBrems: tables are built for mu+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
muPairProd: tables are built for mu+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
muIoni: tables are built for mu-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
|
|
radiative corrections for E > 1 GeV
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
muBrems: tables are built for mu-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
muPairProd: tables are built for mu-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Parametrised model
|
|
|
|
hIoni: tables are built for pi+
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Scaling relation is used to proton dE/dx and range
|
|
Bether-Bloch model for Escaled > 0.297504 MeV, ICRU49 parametrisation for protons below.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
msc: Model variant of multiple scattering for pi-
|
|
Lambda tables from 100 eV to 100 TeV in 120 bins.
|
|
Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
|
|
|
|
hIoni: tables are built for pi-
|
|
dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
|
|
Lambda tables from threshold to 100 TeV in 120 bins.
|
|
Scaling relation is used to proton dE/dx and range
|
|
Bether-Bloch model for Escaled > 0.297504 MeV, ICRU49 parametrisation for protons below.
|
|
Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
|
|
|
|
========= Table of registered couples ==============================
|
|
|
|
Index : 0 used in the geometry : Yes recalculation needed : No
|
|
Material : Vac
|
|
Range cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|
Energy thresholds : gamma 990 eV e- 990 eV e+ 990 eV
|
|
Region(s) which use this couple :
|
|
DefaultRegionForTheWorld
|
|
|
|
Index : 1 used in the geometry : Yes recalculation needed : No
|
|
Material : Aluminium
|
|
Range cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|
Energy thresholds : gamma 6.88731 keV e- 596.68 keV e+ 568.011 keV
|
|
Region(s) which use this couple :
|
|
Region0
|
|
|
|
Index : 2 used in the geometry : Yes recalculation needed : No
|
|
Material : Scintillator
|
|
Range cuts : gamma 1 mm e- 1 mm e+ 1 mm
|
|
Energy thresholds : gamma 2.36895 keV e- 355.791 keV e+ 347.138 keV
|
|
Region(s) which use this couple :
|
|
Region0
|
|
|
|
Index : 3 used in the geometry : Yes recalculation needed : No
|
|
Material : Aluminium
|
|
Range cuts : gamma 1 cm e- 1 cm e+ 1 cm
|
|
Energy thresholds : gamma 20.4949 keV e- 4.54874 MeV e+ 4.2772 MeV
|
|
Region(s) which use this couple :
|
|
Region1
|
|
|
|
Index : 4 used in the geometry : Yes recalculation needed : No
|
|
Material : Scintillator
|
|
Range cuts : gamma 1 cm e- 1 cm e+ 1 cm
|
|
Energy thresholds : gamma 5.69883 keV e- 2.20017 MeV e+ 2.06883 MeV
|
|
Region(s) which use this couple :
|
|
Region1
|
|
|
|
Index : 5 used in the geometry : Yes recalculation needed : No
|
|
Material : Aluminium
|
|
Range cuts : gamma 10 cm e- 10 cm e+ 10 cm
|
|
Energy thresholds : gamma 79.141 keV e- 56.7407 MeV e+ 54.0144 MeV
|
|
Region(s) which use this couple :
|
|
Region2
|
|
|
|
Index : 6 used in the geometry : Yes recalculation needed : No
|
|
Material : Scintillator
|
|
Range cuts : gamma 10 cm e- 10 cm e+ 10 cm
|
|
Energy thresholds : gamma 18.8645 keV e- 23.386 MeV e+ 22.2624 MeV
|
|
Region(s) which use this couple :
|
|
Region2
|
|
|
|
====================================================================
|
|
|
|
Start Run processing.
|
|
PhotInPrimaryGeneratorAction::GeneratePrimaries: pi+,E=100
|
|
PhotInPrimaryGeneratorAction::GeneratePrimaries: part&E're redefined
|