| [575] |
0.34 |
304 | 3,744 | 88 | 2,655 | 1 | 1 |
G4ExcitedMesonConstructor::CreateDecayTable(G4String const&, int, int, int) |
| 0.34 |
3,744 | 3,744 | 84 | 84 | 1 | 1 |
G4ExcitedMesonConstructor::Add2PiRhoMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.24 |
2,592 | 2,592 | 216 | 216 | 1 | 1 |
G4ExcitedMesonConstructor::AddPiRhoMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.21 |
2,304 | 2,304 | 159 | 159 | 1 | 1 |
G4ExcitedMesonConstructor::AddKKStarMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.21 |
2,304 | 2,304 | 366 | 366 | 1 | 1 |
G4ExcitedMesonConstructor::AddKRhoMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.21 |
2,304 | 2,304 | 54 | 54 | 1 | 1 |
G4ExcitedMesonConstructor::AddKStar2PiMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.21 |
2,304 | 2,304 | 332 | 332 | 1 | 1 |
G4ExcitedMesonConstructor::AddKStarPiMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.21 |
2,304 | 2,304 | 51 | 51 | 1 | 1 |
G4ExcitedMesonConstructor::AddKTwoPiMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.18 |
2,016 | 2,016 | 45 | 45 | 1 | 1 |
G4ExcitedMesonConstructor::Add3PiMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.16 |
1,728 | 1,728 | 51 | 51 | 1 | 1 |
G4ExcitedMesonConstructor::Add2PiOmegaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.16 |
1,728 | 1,728 | 156 | 156 | 1 | 1 |
G4ExcitedMesonConstructor::Add4PiMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.13 |
1,440 | 1,440 | 102 | 102 | 1 | 1 |
G4ExcitedMesonConstructor::Add2PiMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.11 |
1,152 | 1,152 | 144 | 144 | 1 | 1 |
G4ExcitedMesonConstructor::Add2KMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.11 |
1,152 | 1,152 | 127 | 127 | 1 | 1 |
G4ExcitedMesonConstructor::Add2KPiMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.11 |
1,152 | 1,152 | 21 | 21 | 1 | 1 |
G4ExcitedMesonConstructor::AddKEtaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.08 |
864 | 864 | 33 | 33 | 1 | 1 |
G4ExcitedMesonConstructor::AddPiA2Mode(G4DecayTable*, G4String const&, double, int, int) |
| 0.05 |
576 | 576 | 53 | 53 | 1 | 1 |
G4ExcitedMesonConstructor::Add2PiEtaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15673488} |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15673727} |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15673908} |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15674149} |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15674410} |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15674650} |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15674810} |
| 0.03 |
288 | 288 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15675050} |
| 0.03 |
288 | 288 | 5 | 5 | 1 | 1 |
@{SimplifiedCalo+15675616} |
| 0.03 |
288 | 288 | 5 | 5 | 1 | 1 |
@{SimplifiedCalo+15675788} |
| 0.03 |
288 | 288 | 5 | 5 | 1 | 1 |
@{SimplifiedCalo+15676042} |
| 0.03 |
288 | 288 | 5 | 5 | 1 | 1 |
@{SimplifiedCalo+15676194} |
| 0.03 |
288 | 288 | 6 | 6 | 1 | 1 |
G4ExcitedMesonConstructor::Add2EtaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.03 |
288 | 288 | 54 | 54 | 1 | 1 |
G4ExcitedMesonConstructor::AddPiEtaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.03 |
288 | 288 | 15 | 15 | 1 | 1 |
G4ExcitedMesonConstructor::AddPiF0Mode(G4DecayTable*, G4String const&, double, int, int) |
| 0.03 |
288 | 288 | 17 | 17 | 1 | 1 |
G4ExcitedMesonConstructor::AddPiF2Mode(G4DecayTable*, G4String const&, double, int, int) |
| 0.03 |
288 | 288 | 35 | 35 | 1 | 1 |
G4ExcitedMesonConstructor::AddPiOmegaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.03 |
288 | 288 | 18 | 18 | 1 | 1 |
G4ExcitedMesonConstructor::AddRhoEtaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.03 |
288 | 288 | 6 | 6 | 1 | 1 |
G4ExcitedMesonConstructor::AddRhoGammaMode(G4DecayTable*, G4String const&, double, int, int) |
| 0.01 |
132 | 132 | 20 | 20 | 1 | 1 |
@{SimplifiedCalo+15673978} |
| 0.01 |
132 | 132 | 20 | 20 | 1 | 1 |
@{SimplifiedCalo+15674211} |
| 0.01 |
132 | 132 | 23 | 23 | 1 | 1 |
@{SimplifiedCalo+15675838} |
| 0.01 |
128 | 128 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15675940} |
| 0.01 |
112 | 5,016 | 12 | 9,554 | 1 | 130 |
G4PhaseSpaceDecayChannel::G4PhaseSpaceDecayChannel(G4String const&, double, int, G4String const&, G4String const&, G4String const&, G4String const&) |
| 0.01 |
112 | 112 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15673558} |
| 0.01 |
112 | 112 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15673789} |
| 0.01 |
112 | 112 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15674480} |
| 0.01 |
112 | 112 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15674712} |
| 0.01 |
112 | 112 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15674880} |
| 0.01 |
112 | 112 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15675112} |
| 0.01 |
112 | 112 | 20 | 20 | 1 | 1 |
@{SimplifiedCalo+15675666} |
| 0.01 |
112 | 112 | 20 | 20 | 1 | 1 |
@{SimplifiedCalo+15676092} |
| 0.01 |
112 | 112 | 20 | 20 | 1 | 1 |
@{SimplifiedCalo+15676244} |
| 0.00 |
24 | 408 | 85 | 410 | 1 | 57 |
G4DecayTable::G4DecayTable() |
| 0.00 |
20 | 20 | 1 | 1 | 1 | 1 |
G4ExcitedMesonConstructor::AddKTwoPiMode(G4DecayTable*, _ZN25G4E const&, long long, char, int) |
| 0.00 |
16 | 16 | 16 | 16 | 1 | 1 |
@{SimplifiedCalo+15674313} |
| 0.00 |
16 | 16 | 2 | 2 | 1 | 1 |
_ZN25G4ExcitedMesonConstructor10Add4PiModeEP12G4DecayTableRK_ZN25G4Excit |
| 0.00 |
8 | 688 | 3 | 1,394 | 1 | 123 |
G4DecayTable::Insert(G4VDecayChannel*) |
| 0.00 |
8 | 8 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15673661} |
| 0.00 |
8 | 8 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15674083} |
| 0.00 |
8 | 8 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15674584} |
| 0.00 |
8 | 8 | 4 | 4 | 1 | 1 |
@{SimplifiedCalo+15674984} |