- Timestamp:
- Apr 6, 2009, 12:30:29 PM (15 years ago)
- File:
-
- 1 edited
Legend:
- Unmodified
- Added
- Removed
-
trunk/source/processes/hadronic/models/pre_equilibrium/History
r819 r962 14 14 * Please list in reverse chronological order (last date on top) 15 15 --------------------------------------------------------------- 16 17 13-February 2009 V.Ivanchenko hadr-pre-V09-02-03 18 --------------------------------------------------- 19 G4PreCompoundXXX - changed the shape of probabilities (return back to 9.2) 20 for d, t, He3, alpha (JMQ) 21 22 12-February 2009 V.Ivanchenko hadr-pre-V09-02-02 23 --------------------------------------------------- 24 G4PreCompoundXXX - changed the shape of probabilities 25 for d, t, He3, alpha near the Coulomb barrier (JMQ) 26 27 11-February 2009 V.Ivanchenko hadr-pre-V09-02-01 28 --------------------------------------------------- 29 G4PreCompoundXXX - set default Opt3 back, add decrease Coulomb barrier 30 for d, t, a, he3 (JMQ) 31 32 10-February 2009 V.Ivanchenko hadr-pre-V09-02-00 33 --------------------------------------------------- 34 Some clean up of comments 35 G4PreCompoundIon - fixed probability of light ion emmision (JMQ) 36 G4PreCompoundXXX - by default Opt1 is used for d, t, a, he3, 37 Opt3 for n, p (JMQ) 38 39 09-December 2008 A.Howard hadr-pre-V09-01-15 40 --------------------------------------------------- 41 Added protection for close to zero excitation energy in 42 G4PreCompoundModel.cc (according to JMQ, MAC) to not try to de-excite. 43 44 09-December 2008 A.Howard hadr-pre-V09-01-14 45 --------------------------------------------------- 46 Added protection for close to zero excitation energy in 47 G4PreCompoundTransitions.cc (returns 0.0), prevents FPE later on. 48 49 27-November 2008 A.Howard hadr-pre-V09-01-13 50 --------------------------------------------------- 51 Added data member initialisation to G4VPreCompoundTransitions.hh 52 53 19-November 2008 A.Howard hadr-pre-V09-01-12 54 --------------------------------------------------- 55 JMQ fix to G4PreCompoundNeutron.cc for Zirconium (if (nu < 0.)nu=-nu). 56 57 30-September 2008 A.Howard hadr-pre-V09-01-11 58 --------------------------------------------------- 59 Trivial protection against negative probabilities for incident protons on 60 targets with A < Carbon. 61 62 22-September 2008 A.Howard hadr-pre-V09-01-10 63 --------------------------------------------------- 64 JMQ's latest developments - which are an extension of hadr-pre-V09-01-08 with 65 cross-section options (equivalent to the de-excitation modifications) and other 66 options (SICB, Never Go Back,...). In addition Gunter's fix to the factorials 67 is included from hadr-pre-V09-01-09. 68 Added new files: G4PreCompoundAlpha.cc G4PreCompoundDeuteron.cc 69 G4PreCompoundHe3.cc G4PreCompoundNeutron.cc G4PreCompoundProton.cc 70 G4PreCompoundTriton.cc (Classes previously existed. Now they have more 71 involved cross-section calculations). 72 73 19-September 2008 A.Howard hadr-pre-V09-01-09 74 --------------------------------------------------- 75 Including Gunter's fix (see 11-August below) on top of ref-07 76 (hadr-pre-V09-00-04), i.e. without JMQ's developments. 77 78 11-August 2008 G.Folger 79 ----------------------------------------------- 80 Rewrite algorithm in G4PreCompoundEmission::rho() to avoid frequent 81 floating point overflow when using Precompund in combination 82 with Binary Cascade. 83 84 85 24 July 2008 J. M. Quesada hadr-pre-V09-01-08 86 --------------------------------------------------- 87 Minor fixes and Coulomb barrier just for Wellisch's proton cross section 88 (OPT=2) 89 90 91 23 July 2008 V.Ivanchenko hadr-pre-V09-01-07 92 --------------------------------------------------- 93 Fixed mistake in tagging 94 95 23 July 2008 V.Ivanchenko hadr-pre-V09-01-06 96 --------------------------------------------------- 97 Return back Coulomb barrier initialisation (J.M.Quesada) 98 99 27 June 2008 V.Ivanchenko hadr-pre-V09-01-05 100 --------------------------------------------------- 101 Fixed G4PreCompoundNucleon and G4PreCompoundIon for 102 Coulomb barrier, added protections for zero cross sections, 103 OPT=2 is used (J.M.Quesada) 104 105 05 June 2008 J. M. Quesada hadr-pre-V09-01-04 106 --------------------------------------------------- 107 Bug fixed in OPT=1 (Chatterjee) charged particle cross sections. 108 Unphysical values at very low emission energies have been corrected (set 109 to 0); OPT=1 ( OPT=2 in previous tag) 110 111 112 15-May 2008 J. M.Quesada hadr-pre-V09-01-03 113 ----------------------------------------------- 114 The retrieval of transition probabilities in G4PreCompoundModel.cc 115 (for protection against unphysically crossing the landa_+=landa_- condition) 116 was misplaced. Now it has been placed inside the preequilibrium transitions 117 loop. 118 119 8-May 2008 J. M.Quesada hadr-pre-V09-01-02 120 ----------------------------------------------- 121 Protection against non physical situation has been set: Equilibrium exciton number 122 Neq (when reached, equilibrium regime starts) should correspond to equal transition 123 probabilities "back" and "forth". Nevertheless, for heavy target (Neq is big even 124 for low incident energies) after first emission this condition (equal trans. prob.) 125 is reached far before reaching corresponding Neq of the residual. Unless this "jump" 126 to equilibrium is forced in this case, preequilibrium will be 127 spuriously prolonged (as a side effect, with huge CPU consumption). 128 G4PreCompoundModel and G4PreCompoundTransitions classes have been modified. 129 130 131 1-May 2008 J. M.Quesada hadr-pre-V09-01-01 132 ----------------------------------------------- 133 - First trial with cvs. 00 skipped by mistake. 134 New inverse cross sections: 135 OPT=1 Chetterjee's parameterization to reaction cross sections from optical potential global fittings. 136 OPT=2 as OPT=1 but for protons the Wellisch's parameterization for protons is used (DEFAULT) 137 OPT=3 Kalbach's modifications of Chatterjee's parameterization of cross sections 138 OPT=4 as OPT=3 but for protons the Wellisch's parameterization for protons is used 139 140 Coulomb barrier has been suppressed as it enters through inverse cross sections. Also methods related to former Dostrovski's cross sections (alpha , beta and C parameters) have been suppressed. In all particle header files: 141 G4PreCompoundNucleon.hh ,G4PreCompoundNeutron.hh,G4PreCompoundProton.hh, G4PreCompoundIon.hh, G4PreCompoundDeuteron.hh, G4PreCompoundTriton.hh ,G4PreCompoundHe3.hh , G4PreCompoundAlpha.hh 142 143 144 Soft cutoff transition from equilibrium to equilibrium has been suppressed (unphysical and not necessary anymore).In G4PreCompoundModel. 145 146 New transition probabilities : 147 OPT=1 Gudima's formulae 148 OPT=2 Machner parameterization of matrix elements for transitions (DEFAULT) 149 150 Level density is set to A/10 (Gudima's prescription). 151 152 Several bugs fixed (average xs in nucleon-nucleon xs in G4PreCompundTransitions.cc and emission probability formula in G4PreCompoundIon.cc ) . 16 153 17 154 25-October 2007 A.Howard hadr-pre-V09-00-04
Note: See TracChangeset
for help on using the changeset viewer.