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This commit is contained in:
Gabriele Cosmo
2019-04-17 10:39:02 +02:00
parent a7fdc52004
commit 28a70706e0
661 changed files with 55791 additions and 106984 deletions
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source/processes/electromagnetic/adjoint/History
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@@ -16,13 +16,16 @@ committal in the CVS repository !
* Reverse chronological order (last date on top), please *
---------------------------------------------------------
11 Mar 2019: G. Cosmo (emadjoint-V10-04-00)
-Fixed typos in printouts and comments.
06 Nov 2017: V. Ivanchenko (emadjoint-V10-03-01)
-Extended correction of occurence of FPE in G4AdjointForcedInteractionForGamma.
-Extended correction of occurrence of FPE in G4AdjointForcedInteractionForGamma.
-G4eAdjointMultipleScattering - change index of the default accourding to recent
modifications in emutils
27 Jan 2017: L. Desorgher (emadjoint-V10-03-00)
-Correction of occurence of FPE in G4AdjointForcedInteractionForGamma.
-Correction of occurrence of FPE in G4AdjointForcedInteractionForGamma.
27 Octb 2016: L. Desorgher (emadjoint-V10-02-03)
-Correction in G4AdjointForcedInteractionForGamma to avoid high weight of forced gamma
source/processes/electromagnetic/adjoint/include/G4AdjointCSManager.hh
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@@ -43,7 +43,7 @@
//-------------------------------------------------------------
// Documentation:
// Is responsible for the management of all adjoint cross sections matrices, and for the computation of the total forward and adjoint cross sections.
// Total adjoint and forward cross sections are needed to correct the weight of a particle after a tracking step or after the occurence of a reverse reaction.
// Total adjoint and forward cross sections are needed to correct the weight of a particle after a tracking step or after the occurrence of a reverse reaction.
// It is also used to sample an adjoint secondary from a given adjoint cross section matrix.
//
#ifndef G4AdjointCSManager_h
source/processes/electromagnetic/adjoint/include/G4AdjointPhotoElectricModel.hh
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@@ -39,7 +39,7 @@
//
// -January 2009. L. Desorgher
// Put a higher limit on the CS to avoid a high rate of Inverse Photo e- effect at low energy. The very high adjoint CS of the reverse
// photo electric reaction produce a high rate of reverse photo electric reaction in the inner side of a shielding for eaxmple, the correction of this occurence
// photo electric reaction produce a high rate of reverse photo electric reaction in the inner side of a shielding for eaxmple, the correction of this occurrence
// by weight correction in the StepDoIt method is not statistically sufficient at small energy. The problem is partially solved by setting an higher CS limit
// and compensating it by an extra weight correction factor. However when coupling it with other reverse processes the reverse photo-electric is still
// the source of very occasional high weight that decrease the efficiency of the computation. A way to solve this problemn is still needed but is difficult