Geant4 11.2.2
Toolkit for the simulation of the passage of particles through matter
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G4HyperAlpha.cc
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1//
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25//
26// Author: 2021 Alberto Ribon
27//
28//----------------------------------------------------------------------------
29
30#include "G4HyperAlpha.hh"
31
32#include "G4DecayTable.hh"
33#include "G4ParticleTable.hh"
36#include "G4String.hh"
37#include "G4SystemOfUnits.hh"
38#include "G4Types.hh"
39#include "G4VDecayChannel.hh"
40
41G4HyperAlpha* G4HyperAlpha::theInstance = nullptr;
42
44{
45 if (theInstance != nullptr) return theInstance;
46 const G4String name = "hyperalpha";
47 // search in particle table
49 auto anInstance = static_cast<G4Ions*>(pTable->FindParticle(name));
50 if (anInstance == nullptr) {
51 // create particle
52 //
53 // Arguments for constructor are as follows
54 // name mass width charge
55 // 2*spin parity C-conjugation
56 // 2*Isospin 2*Isospin3 G-parity
57 // type lepton number baryon number PDG encoding
58 // stable lifetime decay table
59 // shortlived subType anti_encoding
60 // excitation
61
62 // clang-format off
63 anInstance = new G4Ions( name, 3921.87*MeV, 2.501e-12*MeV, +2.0*eplus,
64 0, +1, 0,
65 0, 0, 0,
66 "nucleus", 0, +4, 1010020040,
67 false, 0.2631*ns, nullptr,
68 false, "static", -1010020040,
69 0.0, 0 );
70 // clang-format on
71
72 // Magnetic Moment
73 G4double mN = eplus * hbar_Planck / 2.0 / (proton_mass_c2 / c_squared);
74 anInstance->SetPDGMagneticMoment(2.97896248 * mN);
75
76 // create Decay Table
77 auto table = new G4DecayTable;
78 // create decay channels
79 /*
80 // The decay "mode[1]" produces the secondary "Li4" whose corresponding anti-particle
81 // is not existing in Geant4: we therefore skip it for the time being, to keep the
82 // symmetry with the decays of anti_hyperalpha.
83 const G4double half_br_lambda_to_p_pim = 0.5*0.639;
84 const G4double half_br_lambda_to_n_piz = 0.5*0.358;
85 G4VDecayChannel** mode = new G4VDecayChannel*[4];
86 // lambda -> proton + pi- , with 50% probability of capturing the proton
87 mode[0] = new G4PhaseSpaceDecayChannel( "hyperalpha", half_br_lambda_to_p_pim, 3,
88 "He3", "proton", "pi-" );
89 mode[1] = new G4PhaseSpaceDecayChannel( "hyperalpha", half_br_lambda_to_p_pim, 2,
90 "Li4", "pi-" );
91 // lambda -> neutron + pi0 , with 50% probability of capturing the neutron
92 mode[2] = new G4PhaseSpaceDecayChannel( "hyperalpha", half_br_lambda_to_n_piz, 3,
93 "He3", "neutron", "pi0" );
94 mode[3] = new G4PhaseSpaceDecayChannel( "hyperalpha", half_br_lambda_to_n_piz, 2,
95 "alpha", "pi0" );
96 for ( G4int index = 0; index < 4; ++index ) table->Insert( mode[index] );
97 */
98 // Replacement decay for the time being
99 const G4double br_lambda_to_p_pim = 0.639;
100 const G4double half_br_lambda_to_n_piz = 0.5 * 0.358;
101 auto mode = new G4VDecayChannel*[3];
102 // lambda -> proton + pi- , with 0% probability of capturing the proton
103 mode[0] =
104 new G4PhaseSpaceDecayChannel("hyperalpha", br_lambda_to_p_pim, 3, "He3", "proton", "pi-");
105 // lambda -> neutron + pi0 , with 50% probability of capturing the neutron
106 mode[1] = new G4PhaseSpaceDecayChannel("hyperalpha", half_br_lambda_to_n_piz, 3, "He3",
107 "neutron", "pi0");
108 mode[2] =
109 new G4PhaseSpaceDecayChannel("hyperalpha", half_br_lambda_to_n_piz, 2, "alpha", "pi0");
110 for (G4int index = 0; index < 3; ++index)
111 table->Insert(mode[index]);
112 //---
113 delete[] mode;
114 anInstance->SetDecayTable(table);
115 }
116 theInstance = static_cast<G4HyperAlpha*>(anInstance);
117 return theInstance;
118}
119
124
double G4double
Definition G4Types.hh:83
int G4int
Definition G4Types.hh:85
static G4HyperAlpha * HyperAlpha()
static G4HyperAlpha * HyperAlphaDefinition()
static G4HyperAlpha * Definition()
G4Ions()=default
G4ParticleDefinition * FindParticle(G4int PDGEncoding)
static G4ParticleTable * GetParticleTable()