1 | <HTML> |
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2 | <HEAD> |
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3 | <TITLE>Geant4 9.3 Release Notes</TITLE> |
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5 | <BODY BGCOLOR='F0F0F0'> |
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6 | |
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7 | <P> </P> |
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8 | <BR> |
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9 | <P> </P> |
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10 | |
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11 | <P ALIGN="Center"> |
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12 | <FONT SIZE="+4" COLOR="#238E23"> |
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13 | <B>Geant4 9.3 Release Notes</B> |
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14 | </FONT> |
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15 | |
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16 | <TABLE WIDTH="100%"> |
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17 | <TR><TD ALIGN="Right"> |
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18 | <FONT SIZE="-1" COLOR="#5C3317"> |
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19 | <B><I>December 18<SUP>th</SUP>, 2009</I></B> |
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20 | </FONT> |
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21 | </TD></TR> |
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22 | </TABLE> |
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23 | |
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24 | <BR><BR> |
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25 | <HR ALIGN="Center" SIZE="7%"> |
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26 | <P> |
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27 | The code and binary libraries for the supported systems are available |
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28 | through our <A TARGET="ext" HREF="http://cern.ch/geant4/support/download.shtml">Source |
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29 | Code Web page</A>. |
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30 | </P> |
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31 | <P> |
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32 | <I>We are grateful for the efforts of Geant4 users who have provided |
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33 | detailed feedback or comprehensive reports of issues. |
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34 | We thank in particular those who have contributed corrections, |
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35 | improvements or developments included in this release. </I> |
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36 | </P> |
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37 | <P> |
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38 | Please refer to the |
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39 | <A TARGET="ext" HREF="http://cern.ch/geant4/support/userdocuments.shtml">Geant4 |
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40 | User Documentation</A> for further information about using Geant4. |
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41 | </P> |
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42 | |
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43 | <H2><I>Contents</I></H2> |
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44 | <OL> |
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45 | <LI><A HREF="#1.">Supported and Tested Platforms</A></LI> |
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46 | <LI><A HREF="#2.">CLHEP and AIDA</A></LI> |
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47 | <LI><A HREF="#3.">Items for migration of the user code</A></LI> |
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48 | <LI><A HREF="#4.">New Developments and Capabilities</A></LI> |
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49 | <LI><A HREF="#5.">Expected effects on physics and performance</A></LI> |
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50 | <LI><A HREF="#6.">Known Run-Time Problems and Limitations</A></LI> |
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51 | <LI><A HREF="#7.">Compilation Warnings</A></LI> |
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52 | <LI><A HREF="#8.">Known Run-Time Warnings</A></LI> |
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53 | <LI><A HREF="#9.">Geant4 Software License</A></LI> |
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54 | <LI><A HREF="#10.">Detailed list of changes and fixes</A></LI> |
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55 | </OL> |
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56 | |
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57 | <P> </P> |
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58 | <A NAME="1."></a> |
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59 | <HR> |
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60 | |
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61 | <!-- ============================================== --> |
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62 | |
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63 | <H2>1. Supported and Tested Platforms</H2> |
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64 | |
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65 | Official platforms: |
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66 | <UL> |
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67 | <LI>Linux, gcc-4.1.2 and gcc-4.3.2 (SLC5).<BR> |
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68 | Tested on 32 and 64 bit architectures (Intel or AMD) with |
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69 | Scientific Linux CERN 4 (SLC4) (based on RedHat Linux Enterprise 4) and |
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70 | Scientific Linux CERN 5 (SLC5) (based on RedHat Linux Enterprise 5). |
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71 | Geant4 has also been successfully compiled on other RedHat versions as |
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72 | well as Debian and Suse.</LI> |
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73 | <LI>MacOSX 10.5 with gcc-4.0.1 and 10.6 with gcc-4.2.1</LI> |
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74 | <LI>Windows/XP and CygWin Tools with: Visual C++ 9.0 (Visual Studio 2008)</LI> |
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75 | </UL> |
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76 | |
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77 | More verified configurations: |
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78 | <UL> |
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79 | <LI>Linux, gcc-4.4.2, gcc-4.3.2, gcc-3.4.6 (SLC4)</LI> |
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80 | <LI>Linux, Intel-icc 11.1</LI> |
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81 | </UL> |
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82 | |
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83 | Platforms configured but neither tested nor supported: |
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84 | <UL> |
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85 | <LI>AIX 4.3.2, xlC 6.0</LI> |
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86 | <LI>DEC V4.0, cxx C++ V6.1-027</LI> |
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87 | <LI>HP 10.20, aCC C++ B3910B A.01.23</LI> |
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88 | <LI>MacOSX 10.4, gcc-3.3</LI> |
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89 | <LI>SGI V6.5.5, CC 7.2.1</LI> |
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90 | <LI>SUN Solaris 5.8, C++ CC-5.5.</LI> |
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91 | </UL> |
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92 | |
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93 | <P> </P> |
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94 | <A NAME="2."></A> |
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95 | <HR> |
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96 | |
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97 | <!-- ============================================== --> |
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98 | |
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99 | <H2>2. CLHEP and AIDA</H2> |
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100 | |
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101 | This release of Geant4 has been verified with |
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102 | <A TARGET="ext" HREF="http://cern.ch/clhep/">CLHEP</A>, release <B>2.0.4.5</B>. |
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103 | Use of a different CLHEP version may cause incorrect simulation results. |
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104 | <P> </P> |
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105 | Geant4 9.3 examples with histogramming co-work with analysis tools compliant |
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106 | to AIDA 3.2.1 interfaces (for details, see |
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107 | <A TARGET="ext" HREF="http://cern.ch/geant4/UserDocumentation/UsersGuides/ForApplicationDeveloper/html/apas02.html">Appendix 2</A> |
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108 | of the |
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109 | <A TARGET="ext" HREF="http://cern.ch/geant4/UserDocumentation/UsersGuides/ForApplicationDeveloper/html/">Users Guide for Application Developers</A>). |
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110 | AIDA headers can be downloaded from: |
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111 | <A TARGET="ext" HREF="http://aida.freehep.org/">http://aida.freehep.org</A> |
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112 | |
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113 | |
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114 | <P> </P> |
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115 | <A NAME="3."></A> |
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116 | <HR> |
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117 | |
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118 | <!-- ============================================== --> |
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119 | |
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120 | <H2>3. Items for migration of the user code</H2> |
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121 | |
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122 | Listed here is some relevant information on developments included in this |
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123 | release, some of which may require migrations (mainly for users of advanced |
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124 | Geant4 features) in order to upgrade from release 9.2 to release 9.3. |
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125 | Note that for all users a full re-installation of libraries (or a full |
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126 | recompilation) and a recompilation of user applications is required. |
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127 | |
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128 | <P> </P> |
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129 | <B>Run</B> |
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130 | <P> </P> |
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131 | <UL> |
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132 | <LI>A new method <TT>CheckParticleList()</TT> has been added to |
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133 | <TT>G4VUserPhysicsList</TT> to check the consistency of the list of defined |
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134 | particles before instantiating the physics processes. For example, |
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135 | <TT>e+, e-</TT> and <TT>gamma</TT> should exist if any electromagnetic |
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136 | process is simulated... A fatal exception will be thrown if any particle |
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137 | type mandatory for the simulation is missing.<BR> |
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138 | It is possible to skip this check, by making use of the method |
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139 | <TT>DisableCheckParticleList()</TT> from <TT>G4VUserPhysicsList</TT>.</LI> |
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140 | </UL> |
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141 | |
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142 | <P> </P> |
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143 | <B>Low Energy Electromagnetic physics</B> |
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144 | <P> </P> |
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145 | <UL> |
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146 | <LI>All Low Energy Electromagnetic Physics process classes have been entirely |
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147 | redesigned (migrated) in the Geant4 toolkit in order to offer to users a |
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148 | coherent approach for the modeling of electromagnetic physical interactions. |
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149 | The software design is now common to both 'standard' and 'low energy' |
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150 | electromagnetic modules. These changes affect Livermore, Penelope, |
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151 | ICRU'73 ion and Geant4-DNA Physics. Users are invited to modify their own |
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152 | physics-list(s) in order to use these new processes and models. |
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153 | The web page indicated below describe how to use these new processes and |
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154 | models, with examples of physics list implementations and new features of |
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155 | the adopted common design:<BR> |
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156 | <A HREF="https://twiki.cern.ch/twiki/bin/view/Geant4/LoweMigratedProcesses">https://twiki.cern.ch/twiki/bin/view/Geant4/LoweMigratedProcesses</A> |
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157 | Please note that it is still possible to use previous implementation of the |
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158 | low energy processes for backward compatibility, however, these models are no |
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159 | longer maintained and will be removed in the near future. A warning message |
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160 | will also be displayed when running older low energy model versions.</LI> |
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161 | </UL> |
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162 | |
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163 | <P> </P> |
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164 | <B>Standard Electromagnetic physics</B> |
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165 | <P> </P> |
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166 | <UL> |
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167 | <LI>It is recommended to migrate user custom physics-lists by replacing |
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168 | the <TT>G4MultipleScattering</TT> physics process with the following: |
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169 | <UL> |
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170 | <LI><TT>G4eMultipleScattering</TT> for <TT>e+-</TT>;</LI> |
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171 | <LI><TT>G4MuMultipleScattering</TT> for muons;</LI> |
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172 | <LI><TT>G4hMultipleScattering</TT> for hadrons and ions.</LI> |
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173 | </UL> |
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174 | The former <TT>G4MultipleScattering</TT> still exists in the Geant4 |
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175 | distribution but will be deleted in a future release. |
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176 | <P></P> |
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177 | Nuclear stopping power is no longer part of ionization processes, and is now |
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178 | responsible only for electronic stopping power; for simulation of nuclear |
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179 | stopping, a new process <TT>G4NuclearStopping</TT> should be added to |
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180 | custom physics-lists.</LI> |
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181 | </UL> |
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182 | |
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183 | <P> </P> |
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184 | <B>Physics Lists</B> |
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185 | <P> </P> |
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186 | <UL> |
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187 | <LI>Qualification for several physics-lists have changed. Several are now declared |
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188 | obsolete. A new category of 'experimental' is used for newer physics-lists or ones with new physics options. Some physics-lists have been removed. |
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189 | See in <A HREF="#lst-notes">Section 10</A> for the details.</LI> |
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190 | </UL> |
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191 | |
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192 | <P> </P> |
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193 | <B>Visualization</B> |
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194 | <P> </P> |
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195 | <UL> |
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196 | <LI>The OpenGL Print EPS facility now always depends on the compression library, |
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197 | <TT>zlib</TT>. An internal version of this library is provided for users |
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198 | whose system does not provide the library <TT>libz</TT>. |
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199 | To use this internal version, set the environment variable |
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200 | <TT>G4LIB_USE_ZLIB</TT>. |
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201 | Users who build with the standard Geant4 <TT>Configure</TT> script should |
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202 | not have to worry about this as the environment will automatically be set up |
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203 | correctly.</LI> |
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204 | </UL> |
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205 | |
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206 | <P> </P> |
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207 | <B>Data Sets</B> |
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208 | <P> </P> |
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209 | This release introduces new versions of two data sets. |
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210 | Please see the corresponding details in |
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211 | <A href="#data-notes">Section 10</A> of this document. |
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212 | <UL> |
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213 | <LI>New data for measured optical surface reflectance, RealSurface.1.0.</LI> |
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214 | <LI>New low-energy data set, G4EMLOW.6.9.</LI> |
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215 | </UL> |
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216 | |
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217 | <P> </P> |
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218 | <A NAME="4."></A> |
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219 | <HR> |
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220 | |
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221 | <!-- ============================================== --> |
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222 | |
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223 | <H2>4. New Developments and Capabilities </H2> |
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224 | |
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225 | <B>Geometry & Field</B> |
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226 | <UL> |
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227 | <LI>A new stepper <TT>G4NystromRK4</TT> offers better computing performance in |
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228 | integrating the trajectories of charged particles in a magnetic field. |
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229 | It uses the standard Nystrom method and a novel analytical estimation of |
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230 | the integration error. This reduces greatly the number of field calls per |
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231 | integration step (from 10 to 3). It achieves comparable accuracy with |
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232 | <TT>G4ClassicalRK4</TT> in test cases. It can be used only for pure |
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233 | magnetic fields which are not time-dependent.</LI> |
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234 | <LI>A new class <TT>G4CachedMagneticField</TT> caches the value of a magnetic |
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235 | field class, in order to reduce the number of calls to an expensive field |
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236 | calculation or interpolation method. For positions within the chosen radius |
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237 | of the previous position where it evaluated the field, it returns the last |
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238 | value of the field is automatically. It can be used only for pure magnetic |
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239 | fields which are not time-dependent.</LI> |
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240 | </UL> |
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241 | |
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242 | <B>Detector description persistency</B> |
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243 | <UL> |
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244 | <LI><U>GDML</U>: it is now possible to customise the reader as well as |
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245 | the writer to treat ad-hoc user extensions to the GDML schema. |
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246 | The GDML writer now also supports dumping of optical surface |
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247 | properties associated with surfaces and materials.</LI> |
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248 | </UL> |
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249 | |
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250 | <B>Low Energy Electromagnetic physics</B> |
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251 | <UL> |
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252 | <LI>Software migration: as explained in section 3, all low energy |
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253 | electromagnetic processes and models are now adopting the same design |
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254 | as for the Standard Electromagnetic Physics, for a coherent approach |
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255 | of the modeling of electromagnetic physical interactions.</LI> |
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256 | <LI>Livermore Physics: new <TT>G4LivermorePolarizedPhotoElectricModel</TT> and |
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257 | <TT>G4LivermorePolarizedGammaConversionModel</TT> are available for the |
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258 | simulation of polarized photon interactions.</LI> |
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259 | <LI>ICRU'73 ion model : the upper energy limit of ICRU'73 stopping power tables |
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260 | was extended to <TT>1 GeV/nucleon</TT> (compared to <TT>10 MeV/nucleon</TT> |
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261 | in the previous release). Revised tables were included for <TT>G4_WATER, |
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262 | G4_WATER_VAPOR, G4_Cu, G4_NYLON-6-6</TT> (all tables provided by |
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263 | P. Sigmund/Univ. of Southern Denmark).</LI> |
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264 | <LI>Geant4-DNA Physics: |
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265 | <UL> |
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266 | <LI>Energy range coverage of several Geant4-DNA Physics models has been |
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267 | extended: electron elastic Champion's model from <TT>7.4 eV</TT> up to |
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268 | <TT>10 MeV</TT>; electron ionization Born's model from <TT>11 eV</TT> |
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269 | up to <TT>1 MeV</TT>; proton excitation Born's model up to |
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270 | <TT>100 MeV</TT>; proton ionization Born's model up to <TT>100 MeV</TT>.</LI> |
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271 | <LI>Geant4-DNA models are valid for liquid water only and use now the |
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272 | <TT>G4_WATER</TT> NIST material as liquid water material definition. |
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273 | Users should define liquid water as <TT>G4_WATER</TT> in their |
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274 | application(s).</LI> |
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275 | </UL></LI> |
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276 | <LI>Data set: G4EMLOW version 6.9 is required.</LI> |
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277 | </UL> |
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278 | |
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279 | <B>Standard Electromagnetic physics</B> |
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280 | <UL> |
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281 | <LI>The set of multiple-scattering models has been expanded: |
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282 | <UL> |
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283 | <LI><TT>G4UrbanMscModel92</TT> is the default model for <TT>e+/e-</TT> |
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284 | equivalent to the Urban model included in the previous release 9.2. |
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285 | It is used as the default and in the <TT>Option1</TT> electromagnetic |
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286 | physics constructors for physics-lists.</LI> |
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287 | <LI><TT>G4UrbanMscModel93</TT> is a tuned version of the Urban model used |
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288 | for <TT>e+/e-</TT> in all other physics constructors of physics-lists |
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289 | (<TT>Option2, Option3, Livermore, Penelope</TT>).</LI> |
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290 | <LI><TT>G4GoudsmitSaundersonMscModel</TT> is a new model for <TT>e+/e-</TT> |
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291 | based on formalism developed for Penelope and EGSnrc.</LI> |
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292 | </UL> |
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293 | A new relativistic model <TT>G4PairProductionRelModel</TT> is available |
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294 | for gamma conversion into <TT>e+e-</TT> pair. In this model, the LPM effect |
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295 | is taken into account. The model is suggested for use in high-energy |
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296 | astrophysics applications.</LI> |
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297 | </UL> |
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298 | |
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299 | <B>Hadronic physics</B> |
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300 | <UL> |
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301 | <LI>Improved and extended the <TT>FTF</TT> model. |
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302 | Improved its pion absorption on nucleons, introduced Reggeon cascade stage, and added excitation energy calculation. Tuned the model parameters of nuclear de-excitation and |
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303 | implemented charge-exchange for <TT>pn->np</TT> in elastic and |
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304 | inelastic interactions.</LI> |
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305 | <LI>The validity of the pion-nuclear cross-sections in |
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306 | <TT>G4PiNuclearCrossSections</TT>, and the nucleon-nuclear cross-sections |
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307 | in <TT>G4NeutronInelasticCrossSections</TT> and |
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308 | <TT>G4ProtonInelasticCrossSections</TT> has been extended to <TT>100 TeV,</TT> |
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309 | by assuming a constant cross-section at very high energies.</LI> |
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310 | <LI>Glauber-Gribov cross-sections for ion-ion collisions are now available in |
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311 | the class <TT>G4GGNuclNuclCrossSection</TT>, |
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312 | spanning from <TT>0.1 MeV</TT> to <TT>100 TeV</TT>.</LI> |
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313 | <LI>The nucleon-nucleon and pion-nucleon partial cross-sections used in the |
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314 | Bertini cascade were reviewed and the incorrect cross-sections found below |
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315 | <TT>1 GeV</TT> were fixed. This results in slightly improved agreement |
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316 | with data below <TT>1 GeV</TT>.</LI> |
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317 | <LI>The CHIPS model has been extended with hadronic interactions covering all energies for all hadronic particles; in addition hadron- and |
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318 | lepton-nuclear reactions are extended to high energies (~TeV). |
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319 | It can be used by choosing the new <TT>CHIPS</TT> physics-list. |
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320 | CHIPS ion-ion elastic scattering model is also now available.</LI> |
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321 | <LI>An option was added to allow models for elastic scattering to be treated in a similar way to inelastic models. Models can now be assigned to the |
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322 | process class <TT>G4WHadronElasticProcess</TT>.</LI> |
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323 | <LI><TT>G4NeutronRadCapture</TT> is a simplified new model which produces a |
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324 | single photon after neutron capture. 4-momentum is conserved in the |
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325 | reaction.</LI> |
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326 | <LI>Improved probabilities and channels in the <TT>G4GEM</TT> model bring it |
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327 | into closer agreement with data.</LI> |
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328 | <LI>Unit conversion errors were corrected in fission and Fermi break-up models.</LI> |
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329 | </UL> |
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330 | |
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331 | <B>Optical physics</B> |
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332 | <UL> |
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333 | <LI>Measured angular reflectivity distributions for common surface treatments |
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334 | and reflectors have been incorporated as look-up tables (LUT).</LI> |
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335 | </UL> |
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336 | |
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337 | <P> </P> |
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338 | <B>Physics Lists</B> |
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339 | <UL> |
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340 | <LI>New electromagnetic physics constructors combining standard and |
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341 | low-energy electromagnetic models are available: |
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342 | <TT>G4EmLivermorePhysics, G4EmPenelopePhysics, G4EmDNAPhysics, |
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343 | G4EmLivermorePolarizedPhysics</TT>.</LI> |
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344 | <LI>New default builder for optical photon physics has been added: |
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345 | <TT>G4OpticalPhysics</TT> together with its messenger, |
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346 | <TT>G4OpticalPhysicsMessenger</TT>.</LI> |
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347 | <LI>All lists based on <TT>FTF</TT> and <TT>CHIPS</TT> modelling |
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348 | use the improved versions of <TT>FTF</TT> and <TT>CHIPS</TT>.</LI> |
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349 | <LI>Newly added physics lists: |
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350 | <UL> |
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351 | <LI><TT>CHIPS</TT>, a physics-lists which uses the CHIPS model for nuclear interactions of all energies and particles..</LI> |
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352 | <LI><TT>QGSP_INCL_ABLA</TT>, a list using INCL/ABLA. It is mainly |
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353 | intended for use with energies less than <TT>3 GeV</TT>. This is |
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354 | useful for e.g. spallation studies and Accelerator Driven Systems (ADS) |
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355 | applications.</LI> |
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356 | </UL></LI> |
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357 | <LI>Other new physics-lists, already present in 9.3-Beta: |
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358 | <UL> |
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359 | <LI>Some are based on existing lists, with different transitions between |
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360 | models:<BR> |
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361 | <TT>FTFP_BERT_TRV</TT>, lower the transition energy from |
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362 | BERTini to FTFP in the range from <TT>6-8 GeV</TT>.</LI> |
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363 | <LI>Others offer options for EM physics:<BR> |
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364 | <TT>FTFP_BERT_EMV, FTFP_BERT_EMX, QGSP_BERT_EMX, QGSP_BIC_EMY</TT>.</LI> |
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365 | </UL></LI> |
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366 | <LI>Attempts to reduce usage of LEP in the intermediate energy range: |
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367 | <UL> |
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368 | <LI><TT>QGSP_BERT_NOLEP</TT>, using QGSP starting from <TT>8.5 GeV</TT>;</LI> |
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369 | <LI><TT>QGSP_FTFP_BERT</TT>, using FTFP in the energy range between BERT |
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370 | and QGSP.</LI> |
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371 | </UL></LI> |
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372 | </UL> |
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373 | |
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374 | <B>Visualization, Graphical Representations & Interfaces</B> |
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375 | <UL> |
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376 | <LI>Improved ability of visualization system to render Boolean solids. |
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377 | Certain cases involving very near co-planar faces used to result in |
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378 | incorrect visualization (though not incorrect tracking). |
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379 | An existing mechanism to deal with this has been improved; this mechanism |
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380 | used to shift slightly the position of one solid in a chosen direction. |
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381 | Now it attempts shifts in different directions by varying small amounts |
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382 | until one is found that does not give an error. The system still can not |
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383 | handle every situation. However it results in far fewer visualization |
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384 | inaccuracies than were seen previously in such difficult cases.</LI> |
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385 | <LI>Visualization attributes can now be individually set for each volume within |
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386 | a nested parameterization.</LI> |
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387 | <LI>Rich Trajectories and Rich Trajectory Points now include additional |
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388 | information such as the complete volume path of the starting and ending |
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389 | volume including all replica and copy numbers, etc.</LI> |
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390 | <LI>A new command, <TT>/vis/viewer/set/targetPoint</TT>, sets a specific point |
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391 | to be the center of the view. Helps with doing extreme zoom in to a |
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392 | specific point.</LI> |
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393 | <LI><B>gMocrenFile</B>: First Beta release of this new visualization driver to |
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394 | output data in the <TT>gdd</TT> format used by the gMocren volume |
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395 | visualization tool. <TT>gMocrenFile</TT> can include volume data from |
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396 | sensitive detector volumes, or from command-based scoring meshes, in |
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397 | addition to detector geometry and trajectories. Use new command |
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398 | <TT>/vis/scene/add/psHits</TT> to add scorer hits to gMocren output. |
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399 | For details, see the Application Developers Guide and the |
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400 | <A HREF="http://geant4.kek.jp/gMocren/">gMocren web site</A>.</LI> |
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401 | <LI><TT>G4UIExecutive</TT>: a new utility class for automatic instantiation of |
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402 | a user session selected according to defined environment variables |
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403 | <TT>G4UI_USE_*</TT>.</LI> |
---|
404 | <LI><B>Qt</B>: Continued improvements to this new driver. The <TT>Qt</TT> |
---|
405 | visualization driver and the associated <TT>Qt</TT> User Interface now work |
---|
406 | well on almost all platforms and with both Qt3 and Qt4 (but still considered |
---|
407 | a Beta release due to a few rare combinations of commands on certain |
---|
408 | platforms that can cause crashes).</LI> |
---|
409 | <LI>PostScript printing: vector and bitmapped printing through the UI command |
---|
410 | <TT>/vis/ogl/printEPS</TT> is now fully functional for all OpenGL viewers |
---|
411 | (previously only for OGLIX and OGLSX). Related new commands are |
---|
412 | <TT>/vis/ogl/set/printSize</TT> and <TT>/vis/ogl/set/printFilename</TT>.</LI> |
---|
413 | <LI><B>HepRepFile</B>: new UI commands of the form <TT>/vis/heprep</TT> allow |
---|
414 | easy control of output file name and output directory, whether a file name |
---|
415 | should be reused (rather than having a sequential suffix appended at each |
---|
416 | new file) and whether culled geometry volumes should be included. |
---|
417 | Also fixed a bug in representation of <TT>G4Tubs</TT> which had caused |
---|
418 | wrong visualization for cases in which the tube was at an unusual angle.</LI> |
---|
419 | </UL> |
---|
420 | |
---|
421 | <P> </P> |
---|
422 | <A NAME="5."></A> |
---|
423 | <HR> |
---|
424 | <!-- ============================================== --> |
---|
425 | |
---|
426 | <H2>5. Expected effects on physics and performance</H2> |
---|
427 | |
---|
428 | <B>Geometry</B> |
---|
429 | <UL> |
---|
430 | <LI>The new ad-hoc memory allocation system for touchables in navigation has |
---|
431 | shown an average CPU speed improvement of ~5% and a reduction of overall |
---|
432 | memory allocation and fragmentation for reasonably complex detector setups.</LI> |
---|
433 | </UL> |
---|
434 | |
---|
435 | <B>Low-energy Electromagnetic physics</B> |
---|
436 | <UL> |
---|
437 | <LI>Computing performance of low energy models has been significantly |
---|
438 | improved thanks to new implementations for data loading and interpolation |
---|
439 | methods, transparent to the user's application.<BR> |
---|
440 | No significant changes on the physics outcomes are expected due to the |
---|
441 | new software design of process and model classes, or from these new |
---|
442 | implementations of data loading and interpolation methods.</LI> |
---|
443 | </UL> |
---|
444 | |
---|
445 | <B>Standard Electromagnetic physics and cuts</B> |
---|
446 | <UL> |
---|
447 | <LI>Initialization of the physics-tables is now considerably faster, |
---|
448 | being measured up to a factor 3, depending on the application |
---|
449 | complexity.</LI> |
---|
450 | <LI>A more precise Spline interpolation for the physics-tables, provides |
---|
451 | accuracy of the order of 0.1%.</LI> |
---|
452 | <LI>A new method <TT>ResetConverters()</TT> has been added to |
---|
453 | <TT>G4ProductionCutTable</TT>. This method, if called once initialised |
---|
454 | the run, allows to reduce the memory footprint by clearing temporary |
---|
455 | loss tables and range vectors used at initialisation.</LI> |
---|
456 | </UL> |
---|
457 | |
---|
458 | <B>Hadronic physics</B> |
---|
459 | <UL> |
---|
460 | <LI>Improvements in the de-excitation code (<TT>G4CompetitiveFission</TT>, |
---|
461 | <TT>G4FermiBreakup</TT>, etc.) produce better agreement with IAEA benchmark |
---|
462 | data below <TT>200 MeV</TT>.</LI> |
---|
463 | <LI>Bug-fixes in <TT>G4GEM</TT> evaporation code remove odd-even <TT>A</TT> |
---|
464 | (in fragment mass) discrepancies with triple differential benchmark data.</LI> |
---|
465 | <LI>Bertini cascade now generates 10% less memory churn (creation and deletion |
---|
466 | of objects) and is about 6% faster as a result.</LI> |
---|
467 | <LI>Improved low energy partial cross-sections in Bertini cascade give slightly |
---|
468 | better agreement with low energy benchmark data (<TT>< 1 GeV</TT>).</LI> |
---|
469 | <LI>Improvements in INCL/ABLA code allow <TT>QGSP_INCL_ABLA</TT> physics list to |
---|
470 | run much longer (several thousand events) without crashing.</LI> |
---|
471 | <LI>Improvements in the <TT>FTF</TT> high energy model, allow the model to be |
---|
472 | used successfully down to <TT>3-5 GeV</TT> incident particle energy.</LI> |
---|
473 | </UL> |
---|
474 | |
---|
475 | <P> </P> |
---|
476 | <A NAME="6."></A> |
---|
477 | <HR> |
---|
478 | |
---|
479 | <!-- ============================================== --> |
---|
480 | |
---|
481 | <H2>6. Known Run-Time Problems and Limitations</H2> |
---|
482 | <UL> |
---|
483 | <LI>Reports have been made of particle tracks stuck at a volume boundary or at |
---|
484 | an interface between volumes. This occurs infrequently, on the order of one |
---|
485 | step per 10^11, but can effect large productions. The behaviour involved |
---|
486 | particles which do not progress but move in very small steps, and as a |
---|
487 | result the simulation of this track never finishes. |
---|
488 | <UL> |
---|
489 | <LI>A partial solution is implemented in this release, which uses an |
---|
490 | existing mechanism to identify better these stuck tracks. It is able to |
---|
491 | find all such tracks in the setups reported, using a large multiple of |
---|
492 | the value of the geometrical tolerance for the setup. Users should pay |
---|
493 | attention that the value is chosen well for their setup in case they |
---|
494 | encounter a similar problem (using the existing functionality for |
---|
495 | setting this value).</LI> |
---|
496 | <LI>The treatment for these stuck tracks is to abandon the relevant track. |
---|
497 | This results in the track being killed by the <TT>G4Transportation</TT> |
---|
498 | process. A warning is issued (if compiled in verbose mode, the default) |
---|
499 | in the case that the energy of the track is above a threshold energy. |
---|
500 | Its default value is <TT>100 MeV</TT>. This value should be chosen by |
---|
501 | a user in order to get warning for all particles of energy important to |
---|
502 | your simulation. A new value can be assigned using the |
---|
503 | <TT>SetThresholdWarningEnergy</TT> method of |
---|
504 | <TT>G4Transportation</TT>.</LI> |
---|
505 | </UL></LI> |
---|
506 | </UL> |
---|
507 | For a complete list of outstanding run-time problems and to submit any |
---|
508 | problem you may find while running this version of Geant4, please refer |
---|
509 | to the |
---|
510 | <A TARGET="ext" HREF="http://cern.ch/geant4/problemreport">Geant4 Problem |
---|
511 | Reporting System</A>. |
---|
512 | |
---|
513 | <P> </P> |
---|
514 | <A NAME="7."></A> |
---|
515 | <HR> |
---|
516 | |
---|
517 | <!-- ============================================== --> |
---|
518 | |
---|
519 | <H2>7. Compilation Warnings</H2> |
---|
520 | |
---|
521 | There may be a few compilation warnings on some platforms. |
---|
522 | We do not believe that any of these lead to incorrect run-time behaviour. |
---|
523 | |
---|
524 | <P> </P> |
---|
525 | <A NAME="8."></A> |
---|
526 | <HR> |
---|
527 | |
---|
528 | <!-- ============================================== --> |
---|
529 | |
---|
530 | <H2>8. Known Run-Time Warnings</H2> |
---|
531 | |
---|
532 | The following message may be written to standard output at the end of a program: |
---|
533 | <PRE> |
---|
534 | G4Transportation: Statistics for looping particles |
---|
535 | Sum of energy of loopers killed: |
---|
536 | Max energy of loopers killed: |
---|
537 | </PRE> |
---|
538 | It provides the total energy (in <TT>MeV</TT>) of tracks killed due to |
---|
539 | excessive number of steps ('looping') during the simulation, and the maximum |
---|
540 | energy of such a track. Such behaviour can be due to looping in magnetic fields |
---|
541 | or being abandoned due to being stuck at geometrical boundaries, as mentioned |
---|
542 | in <A href="#6.">Section 6</A>. |
---|
543 | <P></P> |
---|
544 | In case either of these reported energies is significant, we recommend |
---|
545 | increasing the verbosity of <TT>G4Transportation</TT> to obtain information for |
---|
546 | each track killed. A user can change the threshold energy above which particles |
---|
547 | are killed more reluctantly (only after significant additional effort) using |
---|
548 | the method <TT>SetThresholdImportantEnergy</TT> of <TT>G4Transportation</TT>. |
---|
549 | The default value is <TT>250 MeV</TT>. |
---|
550 | |
---|
551 | <P> </P> |
---|
552 | <A NAME="9."></A> |
---|
553 | <HR> |
---|
554 | |
---|
555 | <!-- ============================================== --> |
---|
556 | |
---|
557 | <H2>9. Geant4 Software License</H2> |
---|
558 | |
---|
559 | A Software License applies to the Geant4 code. |
---|
560 | Users must accept this license in order to use it. The details and the list of |
---|
561 | copyright holders is available at |
---|
562 | <A href="http://cern.ch/geant4/license">http://cern.ch/geant4/license</A> |
---|
563 | and also in the text file <TT>LICENSE</TT> distributed with the source code. |
---|
564 | |
---|
565 | <P> </P> |
---|
566 | <A NAME="10."></A> |
---|
567 | <HR> |
---|
568 | |
---|
569 | <!-- ============================================== --> |
---|
570 | |
---|
571 | <H2>10. Detailed list of changes and fixes</H2> |
---|
572 | |
---|
573 | These are the main new features/fixes included in this release since the |
---|
574 | last patched public release (for more detailed lists of fixes/additions, |
---|
575 | please refer to the corresponding History files provided in most packages): |
---|
576 | |
---|
577 | <P> </P> |
---|
578 | |
---|
579 | <A NAME="conf-notes"> |
---|
580 | <H3><I>Configuration</I></H3></A> |
---|
581 | <UL> |
---|
582 | <LI>Configure script: |
---|
583 | <UL> |
---|
584 | <LI>New simplified layout for queries and updated some defaults.</LI> |
---|
585 | <LI>Fixed detection of QtCore library; addressing problem report |
---|
586 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1079">#1079</A>. |
---|
587 | Removed of -s switch to sed in Qt.U to fix problem with Qt setup.</LI> |
---|
588 | <LI>Added flag to allow running with query options on non-interactive |
---|
589 | terminal. Resolves issue reported in Hypernews Install-and-Config #1213.</LI> |
---|
590 | <LI>Added new data set for <TT>G4REALSURFACEDATA</TT> variable and updated |
---|
591 | <TT>G4LEDATA</TT> data set version.</LI> |
---|
592 | <LI>Corrected text for installation of <TT>g3tog4</TT> module; <TT>cernlib</TT> |
---|
593 | is not required.</LI> |
---|
594 | <LI>Removed query on analysis; now <TT>G4ANALYSIS_USE</TT> flag has to be set |
---|
595 | explicitely by the user, if necessary.</LI> |
---|
596 | <LI>Added force build of <TT>zlib</TT> when WIN32 GL or Inventor vis drivers |
---|
597 | are built.</LI> |
---|
598 | </UL></LI> |
---|
599 | <LI>Added <TT>G4OPTDEBUG</TT> option for hybrid optimized-debug build also to |
---|
600 | <TT>Darwin-g++</TT> and <TT>WIN32-g++</TT> configurations.</LI> |
---|
601 | <LI>Corrected inclusion of -lz for zlib in architecture.gmk; corrected also |
---|
602 | inclusion of the G4zlib library in link list in binmake.gmk for |
---|
603 | the case of global libraries.</LI> |
---|
604 | <LI>binmake.gmk: added include paths to new CHIPS modules.</LI> |
---|
605 | <LI>G4VIS_USE.gmk: fixed dependency issues on WIN32-VC for <TT>gl2ps</TT> utility |
---|
606 | library in visualization. Added new gMocren include path. |
---|
607 | Removed references to obsolete GAGTREE driver.</LI> |
---|
608 | <LI>Darwin-g++.gmk: added paths to <TT>$QTHOME/include</TT> and <TT>$QTHOME/lib</TT> |
---|
609 | to setup for Qt4 configuration.</LI> |
---|
610 | <LI>WIN32-VC.gmk: added <TT>gd32.lib use32.lib</TT> to <TT>OGLLIBS</TT> to fix |
---|
611 | problems of linking when <TT>G4LIB_BUILD/USE_WIN32_SESSION</TT> is not set.</LI> |
---|
612 | </UL> |
---|
613 | |
---|
614 | <A NAME="digits-notes"> |
---|
615 | <H3><I>Digitization & Hits</I></H3></A> |
---|
616 | <UL> |
---|
617 | <LI>Corrected counting of flux and current passing through curved surfaces |
---|
618 | (affecting cylinder and sphere surface scorers).</LI> |
---|
619 | <LI>Added missing virtual keyword for qualification of <TT>CheckROVolume()</TT> and |
---|
620 | <TT>FindROTouchable()</TT> methods in <TT>G4VReadOutGeometry</TT>.</LI> |
---|
621 | <LI>Added a few accessors for visualization to <TT>G4VScoringMesh</TT>.</LI> |
---|
622 | </UL> |
---|
623 | |
---|
624 | <A NAME="emstd-notes"> |
---|
625 | <H3><I>Electromagnetic Processes</I></H3></A> |
---|
626 | <UL> |
---|
627 | <LI><B>Adjoint</B> |
---|
628 | <UL> |
---|
629 | <LI>New revised electromagnetic processes for "Reverse MonteCarlo" technique. |
---|
630 | All e- processes have been improved and adjoint proton and ion ionisation |
---|
631 | have been added. The use of adjoint cross section matrices can be now |
---|
632 | limited only to e- Ionisation and Ion ionisation.</LI> |
---|
633 | </UL></LI> |
---|
634 | <LI><B>High Energy</B> |
---|
635 | <UL> |
---|
636 | <LI>Simplified initialisation in <TT>G4mplIonisationModel</TT> and |
---|
637 | <TT>G4eeToHadronsMultiModel</TT>.</LI> |
---|
638 | <LI><TT>G4AnnihiToMuPair</TT>: added method <TT>CrossSectionPerVolume()</TT>; |
---|
639 | added integral option to <TT>PostStepDoIt()</TT>, providing more precise |
---|
640 | simulation near cross-section threshold.</LI> |
---|
641 | <LI><TT>G4eeTo3PiModel</TT>: fixed vector product in matrix element. </LI> |
---|
642 | <LI>Some code cleanup: improved comments, avoid inlined virtual methods.</LI> |
---|
643 | </UL></LI> |
---|
644 | <LI><B>Low Energy</B> |
---|
645 | <UL> |
---|
646 | <LI>Added <TT>G4PenelopeBremsstrahlungModel</TT>, namely Bremsstrahlung |
---|
647 | according to Penelope model, now inheriting from <TT>G4VEmModel</TT>. |
---|
648 | Completed migration to standard-EM design for all Penelope |
---|
649 | processes.</LI> |
---|
650 | <LI>Added <TT>G4RayleighScattering</TT> process (inheriting from |
---|
651 | <TT>G4VEmProcess</TT>) describing Rayleigh scattering. Removed |
---|
652 | <TT>G4Rayleigh</TT> to avoid duplication.</LI> |
---|
653 | <LI>Added <TT>G4LivermoreIonisationModel</TT>, first implementation of |
---|
654 | low-energy ionisation in the new design. Updated Livermore photon |
---|
655 | processes classes for handling of compound materials; added gamma |
---|
656 | particle and energy range test in cross section computation.<BR> |
---|
657 | Updated public interface of <TT>G4eIonisationCrossSectionHandler</TT> |
---|
658 | in order to facilitate migration from <TT>G4LowEnergyIonisation</TT> |
---|
659 | to <TT>G4LivermoreIonisationModel</TT>. |
---|
660 | Set default angular generator in <TT>G4LivermorePhotoElectric</TT> |
---|
661 | as Sauter-Gavrila.</LI> |
---|
662 | <LI>First fully tested version of <TT>G4LivermoreBremsstrahlungModel</TT>, |
---|
663 | completing migration of Livermore processes to new design.</LI> |
---|
664 | <LI>General cleanup of new model classes for Livermore and Penelope |
---|
665 | processes.</LI> |
---|
666 | <LI>Fixed bug in <TT>G4PenelopeRayleigh</TT> (calculation of <TT>mfp</TT> |
---|
667 | for compounds), and in momentum normalization in |
---|
668 | <TT>G4PenelopeBremsstrahlungModel</TT>. Fix in |
---|
669 | <TT>G4PenelopePhotoElectricModel</TT> to avoid misleading warnings.</LI> |
---|
670 | <LI>Added proton case in <TT>G4CrossSectionExcitationMillerGreenPartial</TT>.</LI> |
---|
671 | <LI>Design update, bug fixes and models update for atomic shell hadronic |
---|
672 | cross-sections calculation.</LI> |
---|
673 | <LI>Cleared annoying printout from <TT>G4AugerData</TT> transition table.</LI> |
---|
674 | <LI>Added <TT>ActivateAuger()</TT> method to Penelope Compton and |
---|
675 | Ionisation, so that all Penelope models have now the same interface.</LI> |
---|
676 | <LI>Added protections in <TT>G4eIonisationSpectrum</TT> and |
---|
677 | <TT>G4eIonisationParameters</TT>, addressing problem report |
---|
678 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1042">#1042</A>.</LI> |
---|
679 | <LI>Revision of <TT>G4IonParametrisedLossModel</TT>. Added |
---|
680 | <TT>G4IonDEDXHandler</TT>, a new handler class used by the revised |
---|
681 | model class. Added <TT>G4VIonDEDXScalingAlgorithm</TT>, used by the |
---|
682 | handler; removed <TT>G4IonParametrisedLossTable</TT>. Moved from |
---|
683 | original ICRU'73 classes to new class <TT>G4IonStoppingData</TT>, |
---|
684 | capable of reading stopping power data files stored in the data |
---|
685 | set; with the new tables the upper energy limit of ICRU'73 stopping |
---|
686 | powers is increased to <TT>1 GeV/nucleon</TT>. Added modifier for |
---|
687 | energy loss limit parameter. Changed default energy loss limit to |
---|
688 | smaller value (from 0.15 to 0.01) to avoid approximate loss |
---|
689 | description in case of large steps. Removed nuclear stopping from |
---|
690 | model since dedicated process is available in standard EM package. |
---|
691 | Minor fixes applied in energy loss computation. Bug fix avoiding |
---|
692 | wrong ion ranges in case different cuts are used for a given |
---|
693 | material in different regions. Added <TT>UpdateRangeCache()</TT> |
---|
694 | method, removed <TT>GetRange()</TT> method.</LI> |
---|
695 | <LI>Added new scaling algorithm <TT>G4IonDEDXScalingICRU73</TT>, to |
---|
696 | obtain heavy ion stopping powers for ions not covered by ICRU'73 |
---|
697 | report (scaled from existing ICRU'73 data). Included algorithm in |
---|
698 | ion model, extending the applicability of the model to very heavy |
---|
699 | ions.</LI> |
---|
700 | <LI>Geant4-DNA processes and models: |
---|
701 | <UL> |
---|
702 | <LI>New migrated processes and models.</LI> |
---|
703 | <LI>Added ability for DNA charge change processes to kill particle |
---|
704 | without total energy deposit.</LI> |
---|
705 | <LI>Increased energy range validity of <TT>e-</TT> elastic Champion |
---|
706 | model up to <TT>10 MeV</TT>.</LI> |
---|
707 | <LI>Extended high energy coverage of proton ionisation |
---|
708 | (<TT>G4DNABornIonisationModel</TT>) and excitation |
---|
709 | (G4DNABornExcitationModel); decreased temporarily high energy |
---|
710 | coverage of electron ionisation from <TT>30 keV</TT> to |
---|
711 | <TT>20 keV</TT>.</LI> |
---|
712 | <LI>Added <TT>G4_WATER</TT> NIST material and verbose condition |
---|
713 | to all Geant4-DNA models.</LI> |
---|
714 | <LI>Bug fix in <TT>G4DNABornIonisationModel</TT> for energy deposit.</LI> |
---|
715 | <LI>Improved energy limit display.</LI> |
---|
716 | <LI>Modified low energy limit of <TT>e-</TT> elastic Champion model |
---|
717 | to be used with new data set. Extended coverage of <TT>e-</TT> |
---|
718 | ionisation model as well.</LI> |
---|
719 | <LI>Fixed cross section computation bug in |
---|
720 | <TT>G4DNAScreenedRutherfordElasticModel</TT> and |
---|
721 | <TT>G4DNAChampionElasticModel</TT>.</LI> |
---|
722 | <LI>Added vapor water shell constants to |
---|
723 | <TT>G4DNARuddIonisationModel</TT>.</LI> |
---|
724 | <LI>Added message to obsolete non-migrated Geant4-DNA cross section |
---|
725 | and final state classes, and non-migrated Livermore and Penelope |
---|
726 | classes.</LI> |
---|
727 | </UL></LI> |
---|
728 | <LI>Modified classes <TT>G4VeLowEnergyLoss, G4eLowEnergyLoss</TT> and |
---|
729 | <TT>G4hLowEnergyLoss</TT> according to updates in |
---|
730 | <TT>G4PhysicsVector</TT>.</LI> |
---|
731 | <LI>New implementation for data loading and interpolation methods; |
---|
732 | <TT>LoadData()</TT> method now loads the data from the <TT>G4EMLOW</TT> |
---|
733 | dataset and, then calculates the respective logarithmic values |
---|
734 | during initialization. Both data formats (original and logarithmic) |
---|
735 | are loaded to EM datasets and used later by interpolation methods |
---|
736 | to perform faster calculations. <TT>LoadNonLogData()</TT> method |
---|
737 | implements the old version for data loading and interpolation.</LI> |
---|
738 | <LI>Requires new data set G4EMLOW-6.9.</LI> |
---|
739 | </UL></LI> |
---|
740 | <LI><B>Muons</B> |
---|
741 | <UL> |
---|
742 | <LI><TT>G4MuIonisation</TT>: fixed initialisation for allowing to configure |
---|
743 | external model of fluctuations. Simplified initialisation in |
---|
744 | <TT>G4MuBetheBlochModel</TT>, <TT>G4MuBremsstrahlungModel</TT> |
---|
745 | and <TT>G4MuPairProductionModel</TT>.</LI> |
---|
746 | <LI><TT>G4EnergyLossForExtrapolator</TT>: removed hidden bin to use full scale of |
---|
747 | of <TT>G4PhysicsVector</TT>; set <TT>linLossLimit</TT> to 0.01.</LI> |
---|
748 | <LI><TT>G4MuBetheBlochModel</TT>: compute density effect correction using new |
---|
749 | method of <TT>G4IonisParamMat</TT> class, allowing to apply revised |
---|
750 | parameterization of the density effect.</LI> |
---|
751 | <LI><TT>G4MuMultipleScattering</TT>: use <TT>G4UrbanMscModel90</TT> by |
---|
752 | default.</LI> |
---|
753 | <LI>Some code cleanup: improved comments, avoid inlined virtual methods. </LI> |
---|
754 | </UL></LI> |
---|
755 | <LI><B>Polarisation</B> |
---|
756 | <UL> |
---|
757 | <LI>Bug fix in <TT>G4PolarizationHelper::GetSpinInPRF()</TT> for wrong |
---|
758 | normalization of <TT>Y</TT> component.</LI> |
---|
759 | <LI>Bug fix in <TT>G4PolarizedAnnihilationModel::PostStepDoIt()</TT> for |
---|
760 | wrong treatment in error check.</LI> |
---|
761 | <LI>Bug fix in <TT>G4StokesVector::RotateAz()</TT> for wrong usage of vector |
---|
762 | product.</LI> |
---|
763 | <LI>Simplified initialisation in G4PolarizedAnnihilationModel.</LI> |
---|
764 | </UL></LI> |
---|
765 | <LI><B>Standard</B> |
---|
766 | <UL> |
---|
767 | <LI>Simplified initialisation of all models and code cleanup.</LI> |
---|
768 | <LI><TT>G4PEEffectModel</TT>: substituted <TT>ComputeMeanFreePath()</TT> |
---|
769 | with <TT>CrossSectionPerVolume()</TT> resulting in minor CPU speedup |
---|
770 | for compound materials.</LI> |
---|
771 | <LI>Added new class <TT>G4HeatedKleinNishinaCompton</TT>, prototype model |
---|
772 | for plasma.</LI> |
---|
773 | <LI>New class <TT>G4PairProductionRelModel</TT>, relativistic model for |
---|
774 | gamma conversion.</LI> |
---|
775 | <LI>Energy loss models: |
---|
776 | <UL> |
---|
777 | <LI><TT>G4UniversalFluctuation</TT>: modification in width correction, |
---|
778 | the dependence of the correction on energy deposition at previous |
---|
779 | steps is removed, width correction function is used instead. |
---|
780 | Addresses report from T2K setup.</LI> |
---|
781 | <LI><TT>G4IonFluctuations</TT>: removed extra phenomenological factor in |
---|
782 | fluctuation width.</LI> |
---|
783 | <LI><TT>G4BohrFluctuations</TT>: changed internal parameter to provide for |
---|
784 | smoother transition to Landau regime in the case of small cuts.</LI> |
---|
785 | <LI>Set <TT>linLossLimit</TT> to 0.02 in <TT>G4ionIonisation</TT> allowing |
---|
786 | to smooth computations of mean energy loss of ions.</LI> |
---|
787 | <LI><TT>G4BetheBlochModel</TT> and <TT>G4MollerBhabhaModel</TT>: compute |
---|
788 | density effect correction using method of <TT>G4IonisParamMat</TT> |
---|
789 | class, applying revised density effect parameterisation.</LI> |
---|
790 | <LI><TT>G4BetheBlochModel</TT>: fixed and simplified initialisation for |
---|
791 | ions needed for the new <TT>G4IonParametrisedLossModel</TT> of |
---|
792 | low-energy package. |
---|
793 | Minor speedup in <TT>CorrectionsAlongStep()</TT> method.</LI> |
---|
794 | <LI><TT>G4BetheBlochModel, G4BraggModel, G4BraggIonModel</TT>: removed |
---|
795 | computations of nuclear stopping power, which will is provided by |
---|
796 | the dedicated process, some CPU speedup.</LI> |
---|
797 | <LI><TT>G4WaterStopping</TT>: fix to Ar data; added Fe ion data.</LI> |
---|
798 | </UL></LI> |
---|
799 | <LI>Added new classes <TT>G4NuclearStopping</TT> and |
---|
800 | <TT>G4ICRU49NuclearStoppingModel</TT>, a new model providing computation |
---|
801 | of nuclear stopping.</LI> |
---|
802 | <LI><TT>G4PAIModel</TT>, <TT>G4PAIPhotonModel</TT>: removed usage of random |
---|
803 | numbers at initialisation, to avoid potential non-reproducibility issues.</LI> |
---|
804 | <LI>Added new <TT>G4alphaIonisation</TT> process to be used in experimental |
---|
805 | physics-lists.</LI> |
---|
806 | <LI>Single and multiple scattering: |
---|
807 | <UL> |
---|
808 | <LI>Added <TT>G4UrbanMscModel92</TT> and <TT>G4UrbanMscModel93</TT> |
---|
809 | classes, corresponding to 9.2 and 9.3 versions of the Urban multiple |
---|
810 | scattering model.</LI> |
---|
811 | <LI>Set default model <TT>G4UrbanMscModel92</TT> for |
---|
812 | <TT>G4eMultipleScattering</TT>.</LI> |
---|
813 | <LI><TT>G4UrbanMscModel93</TT>: new tuning for the central part and for |
---|
814 | the tail of the angular distribution using the old e- scattering data |
---|
815 | only (Phys. Rev. 84 (1951) 634; Phys. Rev. 61 (1942) 254). |
---|
816 | New version of <TT>theta0</TT> and correction in tail tuning using |
---|
817 | MuScat data.</LI> |
---|
818 | <LI><TT>G4WentzelVIModel</TT> and all <TT>G4UrbanMscModel*</TT>: use |
---|
819 | generic methods of <TT>G4VMscModel</TT> to access safety and other |
---|
820 | information with the geometry modeller.</LI> |
---|
821 | <LI>Added new alternative multiple-scattering model for <TT>e+-</TT>, |
---|
822 | <TT>G4GoudsmitSaundersonMscModel</TT>.</LI> |
---|
823 | <LI>Added warning in obsolete multiple-scattering classes |
---|
824 | <TT>G4MultipleScattering, G4UrbanMscModel, G4UrbanMscModel2, |
---|
825 | G4MscModel71</TT>.</LI> |
---|
826 | <LI><TT>G4hMultipleScattering</TT>: removed unused obsolete methods.</LI> |
---|
827 | <LI><TT>G4eCoulombScatteringModel</TT>: added relativistic factor to |
---|
828 | Rutherford cross section; added cut per recoil using proton production |
---|
829 | threshold (<TT>1 mm</TT> cut in range corresponding to <TT>100 KeV</TT>); |
---|
830 | Reduced low-limit from <TT>1 KeV</TT> to <TT>0.1 KeV</TT> to provide |
---|
831 | smoother transport cross-section table. Added protection for very low |
---|
832 | energies and changed screening parameters; fixed kinematic for ion/ion |
---|
833 | scattering.</LI> |
---|
834 | <LI><TT>G4CoulombScatteringModel</TT>: fixed energy in the center of mass |
---|
835 | reference system; added cut per recoil using proton production |
---|
836 | threshold.</LI> |
---|
837 | </UL></LI> |
---|
838 | </UL></LI> |
---|
839 | <LI><B>Utils</B> |
---|
840 | <UL> |
---|
841 | <LI><TT>G4VEmModel</TT>: |
---|
842 | <UL> |
---|
843 | <LI>Moved multiple-scattering methods to derived class <TT>G4VMscModel</TT>.</LI> |
---|
844 | <LI>Added new methods <TT>SampleDeexcitationAlongStep()</TT>, |
---|
845 | <TT>GetParticleChangeForLoss</TT>, <TT>GetParticleChangeForGamma</TT>.</LI> |
---|
846 | <LI>Insure definition of pointers to the current <TT>G4Element</TT> and |
---|
847 | <TT>G4MaterialCutsCouple</TT> objects both at initialisation and at |
---|
848 | run time.</LI> |
---|
849 | </UL></LI> |
---|
850 | <LI><TT>G4VMscModel</TT>: |
---|
851 | <UL> |
---|
852 | <LI>Added generic methods used by all multiple-scattering models |
---|
853 | <TT>InitialiseSafetyHelper()</TT>, <TT>ComputeSafety()</TT>, |
---|
854 | <TT>ComputeGeomLimit()</TT> and <TT>ComputeDisplacement()</TT>.</LI> |
---|
855 | <LI>Set default <TT>facsafety</TT> to 0.3 and <TT>range-factor</TT> |
---|
856 | to 0.04 to be the same as in <TT>G4UrbanMscModel92</TT>.</LI> |
---|
857 | </UL></LI> |
---|
858 | <LI><TT>G4VEnergyLossProcess, G4VEmProcess, G4VMultipleScattering</TT>: |
---|
859 | <UL> |
---|
860 | <LI>Set high energy limit to <TT>10 TeV</TT> and number of bins to 77. |
---|
861 | Adopt updated <TT>G4PhysicsVector</TT> with no longer hidden bin.</LI> |
---|
862 | <LI>Added initialisation of <TT>polarAngleLimit</TT> and |
---|
863 | <TT>highEnergyLimit</TT> parameters for all models.</LI> |
---|
864 | <LI>Fixed bug in method <TT>RetrieveTables()</TT>; check that each its |
---|
865 | physics-vector is retrieved before setting the <TT>SplineFlag</TT>.</LI> |
---|
866 | </UL></LI> |
---|
867 | <LI><TT>G4VEnergyLossProcess, G4VEmProcess</TT>: |
---|
868 | <UL> |
---|
869 | <LI>Added calls to de-excitation post-step; added de-excitation |
---|
870 | along-step per region.</LI> |
---|
871 | <LI>Added <TT>ActivateDeexcitation()</TT> method |
---|
872 | in <TT>G4EmProcessOptions</TT> and related UI command to messenger.</LI> |
---|
873 | </UL></LI> |
---|
874 | <LI><TT>G4VMultipleScattering</TT>: |
---|
875 | <UL> |
---|
876 | <LI>Added initialisation of generic multiple-scattering model parameters</LI> |
---|
877 | <LI>Added <TT>SetModel()</TT> method, allowing to overwrite default.</LI> |
---|
878 | <LI>Removed obsolete method <TT>GetMscContinuesStepLimit()</TT>.</LI> |
---|
879 | </UL></LI> |
---|
880 | <LI><TT>G4LossTableManager, G4EmProcessOptions, G4EnergyLossMessenger</TT>: |
---|
881 | <UL> |
---|
882 | <LI>Added parameter <TT>FactorForAngleLimit</TT> with accessors, modifiers |
---|
883 | and UI command, to be used in the computation of limit on -t |
---|
884 | (invariant momentum transfer) inside single scattering and |
---|
885 | <TT>G4WentzelVI</TT> models.</LI> |
---|
886 | </UL></LI> |
---|
887 | <LI><TT>G4EmCalculator</TT>: |
---|
888 | <UL> |
---|
889 | <LI>Added possibility to be used by DNA low-energy processes taking into |
---|
890 | account special DNA particles.</LI> |
---|
891 | <LI>Added method <TT>FindIon()</TT></LI> |
---|
892 | <LI>Improved computation for electronic stopping power of ions using |
---|
893 | <TT>CorrectionAlongStep</TT> method of <TT>G4vEnergyLossProcess</TT> |
---|
894 | allowing to be applied for any model including the model based on |
---|
895 | ICRU'73 data.</LI> |
---|
896 | <LI>Fixed bug in selection of models.</LI> |
---|
897 | </UL></LI> |
---|
898 | <LI><TT>G4EmConfigurator</TT>: fix for the case when only fluctuation model |
---|
899 | is set and main model is the default.</LI> |
---|
900 | <LI>Added <TT>G4EmConfigurator</TT> in <TT>G4LossTableManager</TT> providing |
---|
901 | for easier addition of models per region.</LI> |
---|
902 | <LI><TT>G4EmSaturation</TT>: use PDG encoding instead of pointer to |
---|
903 | <TT>G4ParticleDefinition</TT>.</LI> |
---|
904 | <LI><TT>G4EmCorrections</TT>: fixed bug reported in physics-list forum #532.</LI> |
---|
905 | <LI><TT>G4LossTableBuilder</TT>: added protection in <TT>BuildRangeTable()</TT> |
---|
906 | against zero <TT>dEdx</TT>. Use copy constructors to create physics |
---|
907 | vectors in order to reduce number of calls to <TT>exp()</TT> function.</LI> |
---|
908 | <LI><TT>G4EmModelManager</TT>: |
---|
909 | <UL> |
---|
910 | <LI>Fixed energy range selection algorithm for the case of a small |
---|
911 | intersection of model energy intervals.</LI> |
---|
912 | <LI>Fixed energy range selection algorithm for the case when there |
---|
913 | is an intersection of energy regions of standard and low-energy |
---|
914 | models.</LI> |
---|
915 | <LI>Reduced size and number of internal vectors if no model per region |
---|
916 | are initialized.</LI> |
---|
917 | <LI>Avoid to initilise unused models; simplified initialisation by |
---|
918 | smoothing procedure. The size of executable should be reduced.</LI> |
---|
919 | </UL></LI> |
---|
920 | <LI><TT>G4EmElementSelector</TT>: added protection for zero cross section |
---|
921 | at first and last bins of physics vector and disabled Spline |
---|
922 | interpolation.</LI> |
---|
923 | <LI>Added <TT>G4AtomicShell</TT> class from use by the low-energy module.</LI> |
---|
924 | <LI>Added new interface class <TT>G4VAtomDeexcitation</TT>.</LI> |
---|
925 | </UL></LI> |
---|
926 | <LI><B>Xrays</B> |
---|
927 | <UL> |
---|
928 | <LI>Exclude short-lived particle from <TT>IsApplicable()</TT> for |
---|
929 | <TT>G4Cerenkov</TT> and <TT>G4Scintillation</TT> processes.</LI> |
---|
930 | </UL></LI> |
---|
931 | </UL> |
---|
932 | |
---|
933 | <A NAME="errorprop-notes"> |
---|
934 | <H3><I>Error Propagation</I></H3></A> |
---|
935 | <UL> |
---|
936 | <LI>Inclusion of <TT>pi+, pi-</TT> and proton in physics list.</LI> |
---|
937 | <LI>Added possibility to account for error deflation (needed to make |
---|
938 | 'smoothing').</LI> |
---|
939 | <LI>Corrected usage of <TT>G4ThreeVector</TT> constructor in |
---|
940 | <TT>G4ErrorMagFieldLimitProces</TT>.</LI> |
---|
941 | </UL> |
---|
942 | |
---|
943 | <A NAME="event-notes"> |
---|
944 | <H3><I>Event</I></H3></A> |
---|
945 | <UL> |
---|
946 | <LI>Introducing <TT>G4SmartTrackStack</TT> class. By using this new stack |
---|
947 | as the urgent stack of <TT>G4StackManager</TT>, the next track popped |
---|
948 | up from the stack is not necessarily the last track stored in the |
---|
949 | stack, but the track of same particle type as the previous one, as |
---|
950 | long as such a track exists in the urgent stack. This mechanism is |
---|
951 | expected to improve the performance for ultra-large scale simulation |
---|
952 | such as LHC, by increasing the cache hit rate of the physics tables.<BR> |
---|
953 | The use of <TT>G4SmartTrackStack</TT> is temporarily optional. To use |
---|
954 | it, one should uncomment the <TT>#define</TT> line in |
---|
955 | <TT>include/evmandefs.hh</TT>.</LI> |
---|
956 | <LI>Added UI comand <TT>/event/stack/verbose</TT> providing a short report |
---|
957 | of peak number of tracks in the urgent stack.</LI> |
---|
958 | <LI>New classes implementing the "Reverse MonteCarlo" technique: |
---|
959 | <TT>G4AdjointPosOnPhysVolGenerator</TT>, <TT>G4AdjointPrimaryGenerator</TT> |
---|
960 | and <TT>G4AdjointStackingAction</TT>.</LI> |
---|
961 | </UL> |
---|
962 | |
---|
963 | <A NAME="gen-notes"> |
---|
964 | <H3><I>General Processes</I></H3></A> |
---|
965 | <UL> |
---|
966 | <LI><B>Cuts</B> |
---|
967 | <UL> |
---|
968 | <LI><TT>G4VRangeToEnergyConverter</TT>: modified implementation of |
---|
969 | <TT>ConvertCutToKineticEnergy()</TT> to improve performance. |
---|
970 | Measured a factor 2 to 3 improvement in initialisation speed when |
---|
971 | building physics tables. |
---|
972 | Modified <TT>BuildRangeVector()</TT> where integration is perfomed |
---|
973 | in this method; extended for <TT>e+/e-</TT>. |
---|
974 | Changed <TT>TotBin</TT> to be constant (i.e. same for all converters) |
---|
975 | and set to 100 (200 for previous versions). |
---|
976 | Added <TT>MaxEnergyCut</TT> (<TT>10 GeV</TT> set in default). |
---|
977 | Added <TT>fRangeVectorStore</TT> to ensure that range-vector is |
---|
978 | created only once for each material. Do not apply converter for neutron, |
---|
979 | anti-proton, and anti-neutron.</LI> |
---|
980 | <LI>A new method <TT>ResetConverters()</TT> has been added to |
---|
981 | <TT>G4ProductionCutTable</TT>. This method allows to reduce the memory |
---|
982 | footprint by clearing temporary loss tables and range vectors used at |
---|
983 | initialization, if invoked when starting the first run of a session.</LI> |
---|
984 | <LI>Added possibility to handle cuts for protons.</LI> |
---|
985 | <LI>Added new command <TT>/cuts/setMaxCutEnergy</TT> to messenger.</LI> |
---|
986 | </UL></LI> |
---|
987 | <LI><B>Optical</B> |
---|
988 | <UL> |
---|
989 | <LI>Added capability of simulating surface reflections with Look-Up-Tables |
---|
990 | (LUT), containing measured optical reflectance for a variety of surface |
---|
991 | treatments. Requires new data set <TT>RealSurface-1.0</TT> controlled |
---|
992 | by environment flag <TT>G4REALSURFACEDATA</TT>. |
---|
993 | Courtesy of M.Janecek and W.Moses (LBNL).</LI> |
---|
994 | <LI><TT>G4OpBoundaryProcess</TT>: added initialization of reflectivity |
---|
995 | and efficiency at the beginning of the <TT>PostStepDoIt()</TT>; added |
---|
996 | method <TT>BoundaryProcessVerbose()</TT> which will now print the |
---|
997 | process status for every call to <TT>PostStepDoIt()</TT>. |
---|
998 | Change in <TT>PostStepDoIt()</TT> so that all <TT>dielectric_dielectric</TT> |
---|
999 | surfaces may now have a reflectivity less than 1; |
---|
1000 | not only <TT>frontpainted</TT> as was the case in the past.</LI> |
---|
1001 | </UL></LI> |
---|
1002 | </UL> |
---|
1003 | |
---|
1004 | <A NAME="geo-notes"> |
---|
1005 | <H3><I>Geometry</I></H3></A> |
---|
1006 | <UL> |
---|
1007 | <LI><B>Divisions</B> |
---|
1008 | <UL> |
---|
1009 | <LI>Allow for generic divisions along <TT>Z</TT> for polyhedras and |
---|
1010 | polycones; now divisions can happen along <TT>Z</TT>-axis with width |
---|
1011 | and offset, which fulfils the condition that division does not span |
---|
1012 | over more than one segment.</LI> |
---|
1013 | <LI>Fixed initialization of division in <TT>Phi</TT> for polyhedras to not |
---|
1014 | take into account user defined width.</LI> |
---|
1015 | </UL></LI> |
---|
1016 | <LI><B>Magnetic field</B> |
---|
1017 | <UL> |
---|
1018 | <LI>New stepper <TT>G4NystromRK4</TT> for magnetic field with analytic |
---|
1019 | estimation of integration error. Greatly reduces number of field value |
---|
1020 | per step.</LI> |
---|
1021 | <LI>Added new virtual method <TT>CalculateRightHandSide()</TT> to |
---|
1022 | <TT>G4MagIntegratorStepper</TT> for use in caching momentum (and field |
---|
1023 | value) by <TT>G4NystromRK4</TT>; default implementation in |
---|
1024 | <TT>G4MagIntegratorStepper</TT> calls <TT>RightHandSide()</TT>.</LI> |
---|
1025 | <LI>New simple class <TT>G4CachedMagneticField</TT> to cache value of |
---|
1026 | magnetic field. Speeds up code when calculation of field value is |
---|
1027 | complex.</LI> |
---|
1028 | <LI>New <TT>G4EqEMFieldWithEDM</TT> class for RHS of EofM in a combined |
---|
1029 | electric and magnetic field, with spin tracking for both MDM and EDM |
---|
1030 | terms. Courtesy of Kevin Lynch, Phys. Dept. at Boston Univ.</LI> |
---|
1031 | <LI>Bug fix in <TT>G4EqEMFieldWithSpin</TT>, |
---|
1032 | following report on Hypernews EM-field forum #161.</LI> |
---|
1033 | </UL></LI> |
---|
1034 | <LI><B>Management</B> |
---|
1035 | <UL> |
---|
1036 | <LI>Fixed implementation of <TT>G4LogicalVolume::TotalVolumeEntities()</TT> |
---|
1037 | to become invariant to call sequence. Addressing problem report |
---|
1038 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1082">#1082</A>. |
---|
1039 | <LI>Clear possible excess capacity in node vectors in <TT>G4SmartVoxelHeader</TT> |
---|
1040 | <TT>BuildNodes()</TT> method. May reduce excess memory allocated in |
---|
1041 | optimisation in medium/large detector setups, at the price of a slight |
---|
1042 | time increase in initialisation for geometry voxelisation.</LI> |
---|
1043 | <LI><TT>G4VTouchable</TT>: moved inline vitual methods, constructor and |
---|
1044 | destructor to source, to avoid problem of memory alignment in allocation |
---|
1045 | of derived objects.</LI> |
---|
1046 | <LI><TT>G4Region</TT>: added pointer to field-manager and associated |
---|
1047 | accessor/modifier, to allow for association of a local field to a |
---|
1048 | geometrical region.</LI> |
---|
1049 | </UL></LI> |
---|
1050 | <LI><B>Navigation</B> |
---|
1051 | <UL> |
---|
1052 | <LI>Refinements in <TT>G4PropagatorInField</TT>: |
---|
1053 | <UL> |
---|
1054 | <LI>Activated field per region. A field manager can now be assigned to |
---|
1055 | a region, and it will be used for all logical volumes it contains, |
---|
1056 | except for those which override it by having a field manager of |
---|
1057 | their own.</LI> |
---|
1058 | <LI>Improved handling of repeated small steps at boundaries which are |
---|
1059 | due to geometry imprecision, navigation optimisation, or the |
---|
1060 | details of the algorithm used for tracking in field. |
---|
1061 | <UL> |
---|
1062 | <LI>Added new member <TT>fZeroStepThreshold</TT>, to enable tuning |
---|
1063 | of this existing threshold for identifying tiny or zero steps.</LI> |
---|
1064 | <LI>A new value for this threshold <TT>fZeroStepThreshold</TT> is |
---|
1065 | a large multiple (10^4) of <TT>kCarTolerance</TT>; the old |
---|
1066 | value was <TT>0.5*kCarTolerance</TT>. Addresses a problem of |
---|
1067 | tracks stuck at boundaries of volumes reported by ATLAS.</LI> |
---|
1068 | <LI>The condition for identifying a tiny step is changed in order |
---|
1069 | to avoid misidentifying small proposed physical steps as |
---|
1070 | problem tiny steps.</LI> |
---|
1071 | </UL></LI> |
---|
1072 | <LI>Changed parameters which determine the size of the next trial step. |
---|
1073 | This is used only when trying to recover from consecutive tiny/zero |
---|
1074 | steps. |
---|
1075 | <UL> |
---|
1076 | <LI>The default decrease factor is now 0.25 (from 0.1)</LI> |
---|
1077 | <LI>When the step size is comparable to the value of |
---|
1078 | <TT>fZeroStepThreshold</TT> a different decrease factor |
---|
1079 | is used. The value given to the decrease factor was changed |
---|
1080 | to 0.35 (from 0.25).</LI> |
---|
1081 | </UL></LI> |
---|
1082 | <LI>Added new method <TT>RefreshIntersectionLocator()</TT> to update |
---|
1083 | the state of helper class.</LI> |
---|
1084 | <LI>Improved printing of diagnostics.</LI> |
---|
1085 | <LI>Deleted obsolete internal methods: |
---|
1086 | <TT>SetAccuraciesWithDeltaOneStep(), SetDeltaIntersection(), |
---|
1087 | SetDeltaOneStep()</TT>.</LI> |
---|
1088 | </UL></LI> |
---|
1089 | <LI><TT>G4VIntersectionLocator</TT>: fixed problem in |
---|
1090 | <TT>ReEstimateEndPoint()</TT> for very small steps. Corrected |
---|
1091 | constructor to ensure that it initialises all data members. |
---|
1092 | Labelled methods in header to make noticable those that must change |
---|
1093 | attributes at every step.</LI> |
---|
1094 | </UL></LI> |
---|
1095 | <LI><B>Solids (CSG)</B> |
---|
1096 | <UL> |
---|
1097 | <LI><TT>G4Sphere</TT>: |
---|
1098 | <UL> |
---|
1099 | <LI>Implemented speed improvements and corrections from joint code |
---|
1100 | review. Cached computation for half-tolerances and use of Boolean |
---|
1101 | flag for identifying if full-sphere, shell or section.</LI> |
---|
1102 | <LI>Implemented caching of trigonometric values, now directly computed |
---|
1103 | inside modifiers for <TT>Phi</TT> and <TT>Theta</TT> angles as |
---|
1104 | required for parameterised cases.</LI> |
---|
1105 | <LI>Rationalised usage of relative radial tolerances.</LI> |
---|
1106 | <LI>Correction in <TT>DistanceToOut(p,v)</TT> for <TT>phi</TT> |
---|
1107 | sections for rays passing through zero.</LI> |
---|
1108 | <LI>Fix for the calculation of the normal in <TT>DistanceToOut()</TT> |
---|
1109 | to avoid cases of division by zero in specific configurations. |
---|
1110 | Addresses problem report |
---|
1111 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=977">#977</A>.</LI> |
---|
1112 | </UL></LI> |
---|
1113 | <LI><TT>G4Tubs, G4Cons</TT>: rationalised usage of modifiers for <TT>Phi</TT> |
---|
1114 | angles and simplified constructors.</LI> |
---|
1115 | <LI><TT>G4Cons</TT>: fix to <TT>DistanceToIn(p,v)</TT>, added a check on |
---|
1116 | the direction in case of point on surface. Fixes a problem of stuck |
---|
1117 | tracks observed in CMS, due to wrong reply from the solid for points |
---|
1118 | on the inner radius surface base, with direction along the imaginary |
---|
1119 | extension of the cone.</LI> |
---|
1120 | <LI><TT>G4Torus</TT>: fix in <TT>SolveNumericJT()</TT> in order to take |
---|
1121 | into account the difference in the value of <TT>theta</TT> for different |
---|
1122 | intervals, <TT>[0:pi]</TT> or <TT>[-pi:0]</TT>, and for <TT>SPhi</TT> |
---|
1123 | in <TT>[0:twopi]</TT> or <TT>[-twopi:0]</TT>. Addresses problem report |
---|
1124 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1086">#1086</A>.</LI> |
---|
1125 | <LI><TT>G4Orb</TT>: moved debug warning in <TT>DistanceToIn(p,v)</TT> |
---|
1126 | within <TT>G4CSGDEBUG</TT> flag.</LI> |
---|
1127 | </UL></LI> |
---|
1128 | <LI><B>Solids (Specific)</B> |
---|
1129 | <UL> |
---|
1130 | <LI><TT>G4Ellipsoid</TT>: refined fix in <TT>DistanceToIn(p,v)</TT> for |
---|
1131 | points located on the curved surface, and correct treatment of |
---|
1132 | geometrical tolerance. Addresses problem report |
---|
1133 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1076">#1076</A>.</LI> |
---|
1134 | <LI>Avoid redundant assignment of value to 3-vector in <TT>G4PolyconeSide</TT> |
---|
1135 | and in <TT>G4TwistTubsSide</TT>.</LI> |
---|
1136 | </UL></LI> |
---|
1137 | <LI><B>Volumes</B> |
---|
1138 | <UL> |
---|
1139 | <LI>Fix in <TT>G4PVParameterised::CheckOverlaps()</TT> to not modify |
---|
1140 | daughter volume transformation matrix for application to points in |
---|
1141 | the daughter's frame. Adopt <TT>Inverse()</TT> instead of <TT>Invert()</TT> |
---|
1142 | in call to <TT>G4AffineTransform</TT>. Addresses problem report |
---|
1143 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1078">#1078</A>. |
---|
1144 | <LI>Added missing implementation for composing <TT>G4AssemblyVolume</TT> |
---|
1145 | constructor.</LI> |
---|
1146 | <LI>Use <TT>G4Allocator</TT> for dynamic allocation of |
---|
1147 | <TT>G4TouchableHistory</TT> objects. Should reduce the number of direct |
---|
1148 | calls to <TT>malloc</TT> and memory fragmentation. |
---|
1149 | Measured an average improvement of ~5% in CPU speed with same memory |
---|
1150 | footprint. Moved inline constructors to source to avoid problems of |
---|
1151 | memory alignment in allocation.</LI> |
---|
1152 | </UL></LI> |
---|
1153 | </UL> |
---|
1154 | |
---|
1155 | <A NAME="glob-notes"> |
---|
1156 | <H3><I>Global</I></H3></A> |
---|
1157 | <UL> |
---|
1158 | <LI><TT>G4PhysicsVector</TT>: |
---|
1159 | <UL> |
---|
1160 | <LI>Added <TT>ComputeSecDerivative()</TT> and <TT>SplinePossible()</TT> |
---|
1161 | methods as a computation of Spline coefficients for small number of |
---|
1162 | bins. Removed old obsolete hidden bin approach.</LI> |
---|
1163 | <LI>Added method <TT>ComputeSecondDerivatives()</TT> for the case when |
---|
1164 | user provides first derivative at end-points; use "Not-a-Knot" |
---|
1165 | algorithm for the computation of second derivatives in default method |
---|
1166 | <TT>FillSecondDerivatives()</TT>.</LI> |
---|
1167 | <LI>Cleaned up initialisation of cached values; simplified <TT>Value()</TT> |
---|
1168 | method, now not looking into previous bin; added method |
---|
1169 | <TT>ScaleVector()</TT> needed for ICRU'73 data.</LI> |
---|
1170 | </UL></LI> |
---|
1171 | <LI>New class <TT>G4Pow</TT> for fast computation of <TT>log()</TT> and |
---|
1172 | <TT>pow()</TT> for integer and double arguments in the interval |
---|
1173 | <TT>[1-256]</TT>.</LI> |
---|
1174 | <LI>Added <TT>G4ErrorStage</TT> enum to <TT>G4ErrorPropagatorData</TT> class.</LI> |
---|
1175 | <LI>Cleared warning for unused argument in <TT>G4Allocator</TT> internal method.</LI> |
---|
1176 | <LI>Changed date for release 9.3.</LI> |
---|
1177 | </UL> |
---|
1178 | |
---|
1179 | <A NAME="greps-notes"> |
---|
1180 | <H3><I>Graphical Representations</I></H3></A> |
---|
1181 | <UL> |
---|
1182 | <LI>Improved ability of visualization system to render Boolean solids. |
---|
1183 | Certain cases involving very near co-planar faces had resulted in incorrect |
---|
1184 | visualization (though not incorrect tracking). A previously included |
---|
1185 | mechanism to deal with this by shifting the position of one solid in a |
---|
1186 | chosen direction has been expanded by attempting shifts in different |
---|
1187 | directions by varying small amounts until one is found that does not give |
---|
1188 | an error. The system still can not handle every situation, but results in |
---|
1189 | far fewer visualization inaccuracies than were previously seen in such |
---|
1190 | difficult cases.</LI> |
---|
1191 | <LI>Improved infrastructure for scoring (supporting new UI command |
---|
1192 | <TT>/vis/scene/add/psHits</TT>).</LI> |
---|
1193 | <LI><TT>G4VVisManager</TT>: added notify scene handlers (<TT>G4VGraphicsScene</TT> |
---|
1194 | objects) taking care to notify that the scene has changed so that they may |
---|
1195 | rebuild their graphics database, if any, and redraw all views.</LI> |
---|
1196 | <LI><TT>G4VMarker</TT>: added enum <TT>SizeType</TT> {<TT>none, world, screen</TT>}; |
---|
1197 | added <TT>GetSizeType()</TT> and <TT>SetSize/Diameter/Radius()</TT> methods.</LI> |
---|
1198 | <LI><TT>G4VGraphicsScene</TT>: added method <TT>AddCompound(HitsMap)</TT>.</LI> |
---|
1199 | </UL> |
---|
1200 | |
---|
1201 | <A NAME="had-notes"> |
---|
1202 | <H3><I>Hadronic Processes</I></H3></A> |
---|
1203 | <UL> |
---|
1204 | <LI><B>Cross sections</B> |
---|
1205 | <UL> |
---|
1206 | <LI>Added new Glauber-Gribov cross section for ions, |
---|
1207 | <TT>G4GGNuclNuclCrossSection</TT>.</LI> |
---|
1208 | <LI><TT>G4IonsKoxCrossSection, G4IonsShenCrossSection, |
---|
1209 | G4TripathiCrossSection, G4TripathiLightCrossSection</TT>: added |
---|
1210 | protections against numerical FPE exceptions.</LI> |
---|
1211 | <LI>Use as a default hadron-nucleon cross section parameterisation |
---|
1212 | in <TT>G4GlauberGribovCrossSection, G4GGNuclNuclCrossSection, |
---|
1213 | G4NeutronElasticXS, G4NeutronInelasticXS, G4BGGNucleonElasticXS, |
---|
1214 | G4BGGNucleonInelasticXS, G4BGGPionElasticXS, G4BGGPionInelasticXS</TT>.</LI> |
---|
1215 | <LI>Bug fixes for <TT>G4BGG*</TT> classes and added new classes |
---|
1216 | <TT>G4NeutronElasticXS, G4NeutronInelasticXS, G4NeutronCaptureXS</TT>.</LI> |
---|
1217 | <LI>Modified upper limit of validity to <TT>100 TeV</TT> in |
---|
1218 | <TT>G4PiNuclearCrossSection</TT>, G4NeutronInelasticCrossSection</TT> |
---|
1219 | and <TT>G4ProtonInelasticCrossSection</TT>. |
---|
1220 | Use constant cross-section above original range.</LI> |
---|
1221 | </UL></LI> |
---|
1222 | <LI><B>Management</B> |
---|
1223 | <UL> |
---|
1224 | <LI><TT>G4HadronicInteraction</TT>: renamed <TT>SampleT</TT> as |
---|
1225 | <TT>SampleInvariantT</TT>; added <TT>recoilEnergyThreshold</TT> |
---|
1226 | parameter and accessor methods; use <TT>const</TT> pointers to |
---|
1227 | <TT>G4Element</TT> and </TT>G4Material</TT>; moved |
---|
1228 | <TT>G4ReactionDynamics</TT> instance to parameterised model class |
---|
1229 | <TT>G4InelasticInteraction</TT>.</LI> |
---|
1230 | <LI><TT>G4HadronicInteraction</TT>: added <TT>SetModelName()</TT> method.</LI> |
---|
1231 | <LI><TT>G4V3DNucleus</TT>: added two functions to sort nucleons along |
---|
1232 | +/- <TT>Z</TT>.</LI> |
---|
1233 | </UL></LI> |
---|
1234 | <LI><B>Abrasion</B> |
---|
1235 | <UL> |
---|
1236 | <LI>Fixed problems of negative <TT>sqrt()</TT> and made code more robust |
---|
1237 | to potential loop problems.</LI> |
---|
1238 | </UL></LI> |
---|
1239 | <LI><B>Binary Cascade</B> |
---|
1240 | <UL> |
---|
1241 | <LI>Added interface to set de-excitation handler in |
---|
1242 | <TT>G4BinaryLightIonReaction</TT> used to de-excite lighter initial |
---|
1243 | nucleus; precompound handling low energy interactions can be set too.</LI> |
---|
1244 | <LI>Removed dependency on unused class <TT>G4NucleiPropertiesTable</TT>.</LI> |
---|
1245 | <LI>Made capture-threshold a tunable parameter in |
---|
1246 | <TT>G4GeneratorPrecompoundInterface</TT>.</LI> |
---|
1247 | <LI>Changes to <TT>G4BinaryCascade</TT> to protects against energy |
---|
1248 | non-conservation: shift of particle's formation times; inclusion of |
---|
1249 | captured particles; correction in <TT>GetExcitationEnergy()</TT> for |
---|
1250 | the case when all nucleons are ejected; correction for the nuclear |
---|
1251 | field for baryons.</LI> |
---|
1252 | <LI>Bug fix in <TT>G4BinaryCascade::ApplyCollision()</TT>: decay products |
---|
1253 | outside nucleus were nevertheless counted as if these were within |
---|
1254 | nucleus.</LI> |
---|
1255 | <LI>Corrected assignment to 3-vector, avoid use of 3vector=0.</LI> |
---|
1256 | <LI>Added protection against void nucleus after cascade.</LI> |
---|
1257 | </UL></LI> |
---|
1258 | <LI><B>Bertini Cascade</B> |
---|
1259 | <UL> |
---|
1260 | <LI>New class <TT>G4PionSampler</TT>: samples partial cross sections, |
---|
1261 | multiplicities and final state particle types required for <TT>pi+, |
---|
1262 | pi-</TT> and <TT>pi0</TT> scattering within a nucleus. This class |
---|
1263 | uses re-evaluated pion partial cross-sections and includes production |
---|
1264 | of strange particle pairs.</LI> |
---|
1265 | <LI>Added class <TT>G4NucleonSampler</TT> which replaces old <TT>pp, pn</TT> |
---|
1266 | and <TT>nn</TT> partial and total cross-sections; also modified other |
---|
1267 | classes which use them.</LI> |
---|
1268 | <LI>Added class <TT>G4FinalStateSampler</TT>.</LI> |
---|
1269 | <LI><TT>G4CascadeSigmaPlusNChannel</TT>: corrected sigma plus |
---|
1270 | cross-sections.</LI> |
---|
1271 | <LI><TT>G4CascadSpecialFunctions</TT>: moved pion, kaon, hyperon |
---|
1272 | total cross-sections to this class. Put copy of total cross-section |
---|
1273 | method in <TT>G4NucleiModel</TT>, also removed unneeded energy scale |
---|
1274 | arrays, now replaced with a new one.</LI> |
---|
1275 | <LI><TT>G4ElementaryParticleCollider</TT>: re-written to use |
---|
1276 | <TT>G4PionSampler</TT> class for cross-sections and multiplicities; |
---|
1277 | removed method <TT>reChargering()</TT>, now redundant.</LI> |
---|
1278 | <LI>Moved large arrays which are instantiated at every call of frequently |
---|
1279 | used methods. They are now initialized once in constructors.</LI> |
---|
1280 | <LI><TT>G4CascadeInterface</TT>: moved instantiation of various collider |
---|
1281 | classes outside of loop, and put on stack instead of heap.</LI> |
---|
1282 | <LI><TT>G4ElementaryParticleCollider</TT>: redesigned to use |
---|
1283 | <TT>G4NucleonSampler</TT> and remove instantiation of large arrays |
---|
1284 | from within loops in code.</LI> |
---|
1285 | <LI><TT>G4CascadParticle, G4InuclElementaryParticle</TT>: added integer |
---|
1286 | argument to constructor to indicate which generation cascade particle |
---|
1287 | belongs to. Changed <TT>G4NucleiModel</TT> and |
---|
1288 | <TT>G4BertiniNucleiModel</TT> to use this.</LI> |
---|
1289 | <LI><TT>G4NucleiModel</TT>: removed instantiation of large arrays from |
---|
1290 | with loops; added new total cross section sampling, removed use of all |
---|
1291 | but one energy scale. Updated <TT>pi-</TT> and <TT>pi0</TT> total |
---|
1292 | cross-sections. Clean up of dead code.</LI> |
---|
1293 | <LI>Added assignment operator to class <TT>G4CollisionOutput</TT>.</LI> |
---|
1294 | </UL></LI> |
---|
1295 | <LI><B>Chiral Invariant Phase Space (CHIPS)</B> |
---|
1296 | <UL> |
---|
1297 | <LI>First implementation of CHIPS ion-ion elastic.</LI> |
---|
1298 | <LI>Extended model for all energies for all particles. |
---|
1299 | Removed obsolete classes.</LI> |
---|
1300 | <LI>Added photon and lepton-nuclear CHIPS inelastic; improved model to |
---|
1301 | work for all targets, including Hydrogen. |
---|
1302 | Added diffraction to CHIPS inelastic.</LI> |
---|
1303 | <LI>Added 8 new cross-section classes and bug fixes in pA |
---|
1304 | cross-sections. Tuning of the <TT>G4QCollision</TT> for better |
---|
1305 | description of the pA interactions (<TT>E<290 MeV</TT>).</LI> |
---|
1306 | <LI>Reorganised CHIPS classes in sub-modules: body, cross_sections, |
---|
1307 | fragmentation, interface and processes. |
---|
1308 | Better readability of the CHIPS code and code improvements.</LI> |
---|
1309 | <LI>Improvements in hadron+proton, heavy fragments in low-energy, |
---|
1310 | various bug fixes in <TT>G4QNucleus</TT>, <TT>G4QEnvironment</TT>, |
---|
1311 | <TT>G4QCollision</TT>.</LI> |
---|
1312 | <LI>Improvement of <TT>G4QuasiFreeRatios</TT> for application in |
---|
1313 | <TT>QGSC</TT> from <TT>E=0</TT>.</LI> |
---|
1314 | <LI><TT>MuCaptureEMCascade</TT> excluded from capture at rest for |
---|
1315 | <TT>mu-</TT>; all the atomic de-excitation energy of capture is |
---|
1316 | concentrated in the energy deposition.</LI> |
---|
1317 | <LI>Bug fix against division by zero in <TT>G4QEnvironment</TT>; |
---|
1318 | improvement for the case when the Hypernucleus cannot decay in the |
---|
1319 | residual nucleus and pion; now it is decayed in the residual nucleus |
---|
1320 | and gamma.</LI> |
---|
1321 | <LI>Fixed non-initialised variables in <TT>G4QContent</TT> and fix in |
---|
1322 | quasi-elastic for photons and leptons.</LI> |
---|
1323 | <LI>Change of <TT>GetNuclearMass(A-1.,Z-1.)</TT> (and similar) to |
---|
1324 | <TT>GetNuclearMass(A-1,Z-1)</TT> to be consistent with changes in |
---|
1325 | particles.</LI> |
---|
1326 | <LI>Replaced internal <TT>RndmDir()</TT> with general |
---|
1327 | <TT>G4RandomDirection()</TT> in the code.</LI> |
---|
1328 | <LI>Bug fix in <TT>G4QNeutronCaptureRatio</TT> (Cu65): accelerate CuSc |
---|
1329 | by 1.5.</LI> |
---|
1330 | <LI>Cleared dependency of now removed <TT>G4NucleiPropertiesTable</TT> |
---|
1331 | class.</LI> |
---|
1332 | </UL></LI> |
---|
1333 | <LI><B>De-excitation</B> |
---|
1334 | <UL> |
---|
1335 | <LI>GEM code: |
---|
1336 | <UL> |
---|
1337 | <LI>Fixes in <TT>G4GEMProbability</TT> and <TT>G4GEMChannel</TT> |
---|
1338 | to provide same probability as proposed in original papers. |
---|
1339 | Fixed old problem in <TT>G4GEMChannel</TT>, computation of |
---|
1340 | Coulomb barrier was not consistent with probability. Added |
---|
1341 | protection on unphysical initial state in <TT>G4GEMChannel</TT>. |
---|
1342 | Fixed units (<TT>hbar_Plank -> hbarc</TT>) in |
---|
1343 | <TT>G4GEMProbability</TT>.</LI> |
---|
1344 | <LI><TT>G4EvaporationDefaultGEMFactory</TT>: new class where light |
---|
1345 | meson probabilities are computed from default classes and other |
---|
1346 | fragments from GEM.</LI> |
---|
1347 | <LI>Introduction of new classes <TT>G4GEMCoulombBarrier, |
---|
1348 | G4AlphaGEMCoulombBarrier, G4DeuteronGEMCoulombBarrier, |
---|
1349 | G4He3GEMCoulombBarrier, G4ProtonGEMCoulombBarrier, |
---|
1350 | G4TritonGEMCoulombBarrier</TT> and corresponding |
---|
1351 | changes in other classes of the sub-package.</LI> |
---|
1352 | </UL></LI> |
---|
1353 | <LI>Added a <TT>G4NeutronRadCapture</TT> model, a simple 1-gamma emission |
---|
1354 | with 4-momentum balance.</LI> |
---|
1355 | <LI>Fixed 4-momentum balance by using direct Lorentz computations in |
---|
1356 | <TT>G4CompetitiveFission</TT>. Make use of internal units.</LI> |
---|
1357 | <LI><TT>G4Evaporation</TT>: added method <TT>SetCombinedCannels()</TT> to |
---|
1358 | define new evaporation factory <TT>G4EvaporationDefaultGEMFactory</TT>.</LI> |
---|
1359 | <LI><TT>G4FissionLevelDensityParameter, G4FissionParameters</TT>: tuned |
---|
1360 | against IAEA benchmark spallation data.</LI> |
---|
1361 | <LI><TT>G4FermiFragmentsPool</TT>: fixed units (<TT>keV -> MeV</TT>), |
---|
1362 | removed wrong levels, added new levels according to Broohaven data |
---|
1363 | (see <A href="http://www.nndc.bnl.gov/chart">chart of nuclides</A>).</LI> |
---|
1364 | <LI>Fixed <TT>G4ExitationHandler</TT> for the case when Fermi-BreakUp |
---|
1365 | and multi-fragmentation model are activated.</LI> |
---|
1366 | <LI>Improved implementation of Gamma function computation in configuration |
---|
1367 | weight inside <TT>G4FermiConfiguration</TT>.</LI> |
---|
1368 | <LI>Updated ablation largely to comply with updates in <TT>G4Evaporation</TT> |
---|
1369 | and handling of <TT>G4Fragment</TT>; fixed a bug in fragment |
---|
1370 | identification when evaporation isn't used.</LI> |
---|
1371 | </UL></LI> |
---|
1372 | <LI><B>Elastic scattering</B> |
---|
1373 | <UL> |
---|
1374 | <LI>Model precise sampling and 'on the fly' table preparation in |
---|
1375 | <TT>G4DiffuseElastic</TT>.</LI> |
---|
1376 | <LI>Migrated to the hadronic model design of elastic scattering. |
---|
1377 | Modified <TT>G4ElasticHadrNucleusHE</TT> to be now capable to work |
---|
1378 | with old and new interface.</LI> |
---|
1379 | <LI>Added new elastic process <TT>G4WHadronElasticProcess</TT>.</LI> |
---|
1380 | <LI>Added new class <TT>G4VHadronElastic</TT>, base class for elastic |
---|
1381 | models with default GHEISHA model</LI> |
---|
1382 | <LI>New class <TT>G4CHIPSElastic</TT>, model interface to <TT>CHIPS</TT> |
---|
1383 | parameterization.</LI> |
---|
1384 | <LI>Removed had-hoc NaN finder and printout in destructor of |
---|
1385 | <TT>G4HadronElastic</TT>.</LI> |
---|
1386 | </UL></LI> |
---|
1387 | <LI><B>High Energy Theoretical</B> |
---|
1388 | <UL> |
---|
1389 | <LI>Quasi Elastic part is made more used in <TT>QGSC</TT> at low energies |
---|
1390 | to improve the performance of <TT>QGSC</TT> at low energies.</LI> |
---|
1391 | </UL></LI> |
---|
1392 | <LI><B>Im_r_matrix</B> |
---|
1393 | <UL> |
---|
1394 | <LI>Fix in <TT>G4CollisionComposite</TT> reproducibility. Removed dependence |
---|
1395 | of the energy grid of the cross-section set on the order of the |
---|
1396 | particles by forcing heavier particle to be at rest when caching the |
---|
1397 | cross section.</LI> |
---|
1398 | <LI>Reduced usage of strings; maps of cross-sections use |
---|
1399 | <TT>G4Particledefinition</TT> in place of particle name.</LI> |
---|
1400 | </UL></LI> |
---|
1401 | <LI><B>INCL/ABLA</B> |
---|
1402 | <UL> |
---|
1403 | <LI>Bug fixes to INCL nuclear potential handling; the interpolation |
---|
1404 | function used to produce discontinuous results due to an array index |
---|
1405 | off-by-one. This bug fix corrects the impact parameter distribution.</LI> |
---|
1406 | <LI>Fixed several variable initialization and F77 to C++ translation issues |
---|
1407 | in INCL.</LI> |
---|
1408 | <LI>Added several safeguards for division by zero or negative sqrt().</LI> |
---|
1409 | <LI>Use centralised random number generator instead of built-in one.</LI> |
---|
1410 | <LI>Minor fix in the INCL particle reflection time calculation.</LI> |
---|
1411 | </UL></LI> |
---|
1412 | <LI><B>Parton-String</B> |
---|
1413 | <UL> |
---|
1414 | <LI>Improved <TT>FTF</TT> model for pion obsorption on nuclei: introduced |
---|
1415 | status of nuclear nucleon involved in an interaction (Status 0 - |
---|
1416 | spectator, 1 - involved nucleon, 2 - absorbed nucleon); introduced |
---|
1417 | connection between a participant nucleon and a nuclear nucleon in |
---|
1418 | <TT>G4InteractionContent</TT>.</LI> |
---|
1419 | <LI>Completed <TT>FTF</TT> model with Reggeon cascade and added excitation |
---|
1420 | energy calculation.</LI> |
---|
1421 | <LI>Tuned <TT>FTFP</TT> with parameters of nuclear de-excitation.</LI> |
---|
1422 | <LI>Implemented charge-exchange for <TT>pn->np</TT> in elastic and |
---|
1423 | inelastic interactions simulated by <TT>FTF</TT>. Implemented also |
---|
1424 | pion absorption by a nucleon.</LI> |
---|
1425 | <LI>New Boolean parameter added in <TT>G4VSplitableHadron</TT> class for |
---|
1426 | activation and corresponding methods to operate with it; needed for |
---|
1427 | absorption of meson in nuclear collision generated by <TT>FTF</TT>.</LI> |
---|
1428 | <LI>Fixed bug in <TT>G4VLongitudinalStringDecay</TT> for the calculation |
---|
1429 | of formation/creation time, <TT>c_light</TT> was inserted. Due to this |
---|
1430 | string tension parameter was set to the usual value (<TT>1 GeV/fm</TT>) |
---|
1431 | in <TT>G4LundStringFragmentation</TT>.</LI> |
---|
1432 | <LI><TT>G4VParticipants</TT>: use modified name of method to sort nucleons |
---|
1433 | in <TT>G4V3DNucleus</TT>.</LI> |
---|
1434 | </UL></LI> |
---|
1435 | <LI><B>Photolepton-hadron</B> |
---|
1436 | <UL> |
---|
1437 | <LI>Code cleanup.</LI> |
---|
1438 | </UL></LI> |
---|
1439 | <LI><B>Pre-equilibrium</B> |
---|
1440 | <UL> |
---|
1441 | <LI><TT>G4PreCompoundModel</TT>: CEM transition probabilities are set by |
---|
1442 | default. In <TT>G4PreCompoundTransitions</TT>, CEM transition |
---|
1443 | probabilities have been renormalized (transitions with Delta N=+2 |
---|
1444 | are increased by factor 5).</LI> |
---|
1445 | <LI><TT>G4PrecompoundEmission</TT>: modified <TT>AngularDistribution()</TT> |
---|
1446 | to avoid floating point exceptions. Removed calls to <TT>log()</TT> |
---|
1447 | in <TT>rho()</TT> and replaced by use of new <TT>logfactorial()</TT>.</LI> |
---|
1448 | </UL></LI> |
---|
1449 | <LI><B>QMD Reaction</B> |
---|
1450 | <UL> |
---|
1451 | <LI>Fixed bug for incidence of neutral particles in <TT>G4QMDReaction</TT> |
---|
1452 | and <TT>G4QMDGroundStateNucleus</TT>; verified for nucleon-nucleus |
---|
1453 | interactions.</LI> |
---|
1454 | <LI>Beta version of code for enabling meson incidence.</LI> |
---|
1455 | </UL></LI> |
---|
1456 | <LI><B>Radioactive Decay</B> |
---|
1457 | <UL> |
---|
1458 | <LI>Added dependence on EM 'util' module for usage of the |
---|
1459 | <TT>G4AtomicShell</TT> class.</LI> |
---|
1460 | </UL></LI> |
---|
1461 | <LI><B>Re-Parameterized Gheisha</B> |
---|
1462 | <UL> |
---|
1463 | <LI><TT>G4RPGInelastic</TT>: added temporary message stating the <TT>RPG</TT> |
---|
1464 | model is under development and should not be used for production.</LI> |
---|
1465 | </UL></LI> |
---|
1466 | <LI><B>Stopping</B> |
---|
1467 | <UL> |
---|
1468 | <LI>Removed dependency on unused class <TT>G4NucleiPropertiesTable</TT>.</LI> |
---|
1469 | <LI><TT>G4PiMinusAbsorptionAtRest, G4KaonMinusAbsorptionAtRest</TT>: fixed |
---|
1470 | usage of 3vector constructor.</LI> |
---|
1471 | </UL></LI> |
---|
1472 | <LI><B>Utils</B> |
---|
1473 | <UL> |
---|
1474 | <LI>Restored methods for storing/retrieving <TT>G4SplitableHadron</TT>, |
---|
1475 | now in use in <TT>FTF</TT> model.</LI> |
---|
1476 | <LI>Corrected assignment to 3-vector, avoid use of 3vector=0.</LI> |
---|
1477 | <LI><TT>G4WilsonRadius</TT>: fixed data vector type qualification.</LI> |
---|
1478 | <LI><TT>G4NuclearFermiDensity</TT>: added protection to <TT>GetDeriv()</TT> |
---|
1479 | for positions far outside the nucleus causing an FP overflow in |
---|
1480 | <TT>exp()</TT>.</LI> |
---|
1481 | </UL></LI> |
---|
1482 | </UL> |
---|
1483 | |
---|
1484 | <A NAME="interc-notes"> |
---|
1485 | <H3><I>Intercoms</I></H3></A> |
---|
1486 | <UL> |
---|
1487 | <LI><TT>G4UIcommandTree</TT>: added a new function to complete a command path |
---|
1488 | with maximum characters guess; <TT>FindCommandTree()</TT> will now return |
---|
1489 | current tree when command path is "/".<BR> |
---|
1490 | Fixed incorrect directory deletion of <TT>G4UIcommandTree::RemoveCommand()</TT>. |
---|
1491 | Addresses problem report |
---|
1492 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1087">#1087</A>. |
---|
1493 | <LI>Added method <TT>GetPreviousSession()</TT> in <TT>G4UIbatch</TT>.</LI> |
---|
1494 | </UL> |
---|
1495 | |
---|
1496 | <A NAME="interf-notes"> |
---|
1497 | <H3><I>Interfaces</I></H3></A> |
---|
1498 | <UL> |
---|
1499 | <LI><TT>G4UIExecutive</TT>: new class for automatic instantiation of user |
---|
1500 | interactive sessions.</LI> |
---|
1501 | <LI><TT>G4VBasicShell</TT>: better command completion in command line. |
---|
1502 | Fix for commands strings that match shorter commands.</LI> |
---|
1503 | <LI><TT>G4VUIshell</TT>: added <TT>SetLsColor()</TT> method.</LI> |
---|
1504 | <LI><TT>G4UIQt</TT>: added interactor to be able to add button on file and |
---|
1505 | help menu; added public method to get the main window. |
---|
1506 | Added <TT>CTRL+A</TT> and <TT>CTRL+E</TT> to move to begin/end of |
---|
1507 | command line. Fixed a problem on macOSX 10.6 with Qt 4.6-Beta. |
---|
1508 | Added debug flags for Qt. Fixed compilation warnings.</LI> |
---|
1509 | </UL> |
---|
1510 | |
---|
1511 | <A NAME="materials-notes"> |
---|
1512 | <H3><I>Materials</I></H3></A> |
---|
1513 | <UL> |
---|
1514 | <LI>ICRU'73 stopping power classes: |
---|
1515 | <UL> |
---|
1516 | <LI>Migrated to the <TT>G4VIonDEDXTable</TT> interface: access methods |
---|
1517 | of physics vectors have changed (vectors can also be identified via |
---|
1518 | atomic number of material if material is pure). Classes now deliver |
---|
1519 | mass stopping powers instead of stopping powers per unit length. |
---|
1520 | Any dependency on ICRU'73 material densities was removed (no densities |
---|
1521 | are included in the classes any longer). Stopping power vectors are |
---|
1522 | now only built on request and not anymore in the constructor. |
---|
1523 | Affected classes: <TT>G4IronStoppingICRU73, G4MaterialStoppingICRU73</TT> |
---|
1524 | and <TT>G4SimpleMaterialStoppingICRU73</TT>.</LI> |
---|
1525 | <LI><TT>G4IronStoppingICRU73</TT>: extended upper limit of the data vector |
---|
1526 | from <TT>10 MeV</TT> to <TT>1 GeV</TT>; 53 bins are now used. |
---|
1527 | Added <TT>G4WATER</TT> data. Also fixed <TT>GetDEDX()</TT> methods in |
---|
1528 | these classes for <TT>E=10 MeV</TT> (upper limit).</LI> |
---|
1529 | <LI><TT>G4MaterialStoppingICRU73</TT>: extended energy range of revised |
---|
1530 | ICRU'73 tables for water from <TT>0.025-10 MeV/u</TT> to |
---|
1531 | <TT>0.025-1 GeV/u</TT>. |
---|
1532 | Added new function <TT>AddPhysicsVectorFullRange()</TT> for creating |
---|
1533 | corresponding physics vectors. Changed material name from |
---|
1534 | <TT>G4_NYLON-6/6</TT> to <TT>G4_NYLON-6-6</TT>.</LI> |
---|
1535 | </UL></LI> |
---|
1536 | <LI>New class <TT>G4IonStoppingData</TT>, which can read ion stopping power |
---|
1537 | vectors contained in <TT>G4LEDATA</TT> data set; allows for inclusion of |
---|
1538 | larger physics vectors than those in the ICRU'73 classes, where vectors |
---|
1539 | are restricted to the maximum energy <TT>10 MeV/nuc</TT>.</LI> |
---|
1540 | <LI><TT>G4NistMaterialBuilder</TT>: mean ionisation potential for <TT>G4_WATER</TT> |
---|
1541 | is set to <TT>78 eV</TT> according to GSI Annual Report (2008) p.373, in |
---|
1542 | order to be consistent with ICRU'73 tables. Fixed ICRU'73 data provided by |
---|
1543 | Prof. P.Sigmund (Univ. Southern Denmark): <TT>G4WATER, G4WATER_VAPOR, |
---|
1544 | G4_NYLON-6-6</TT> (in <TT>G4MaterialStoppingICRU73</TT>); <TT>G4_Cu</TT> |
---|
1545 | (in <TT>G4SimpleMaterialStoppingICRU73</TT>). |
---|
1546 | Changed material names, <TT>G4_NYLON-6/6</TT> to <TT>G4_NYLON-6-6</TT>, |
---|
1547 | and <TT>G4_NYLON-6/10</TT> to <TT>G4_NYLON-6-10</TT>, to allow matching |
---|
1548 | with ion stopping power data files. Old names can still be used for |
---|
1549 | backward compatibility. Changed density of <TT>G4_GRAPHITE</TT> according |
---|
1550 | to PDG-2008, added new material <TT>G4_GRAPHITE_POROUS</TT>.</LI> |
---|
1551 | <LI><TT>G4NistMessenger</TT>: added UI command to print parameters of density |
---|
1552 | effect data. Improved implementation of UI commands in |
---|
1553 | <TT>G4NistManager</TT>, G4NistMessenger</TT> and |
---|
1554 | <TT>G4NistElementBuilder</TT>.</LI> |
---|
1555 | <LI><TT>G4VIonDEDXTable</TT>: added interface class for electronic stopping |
---|
1556 | power tables for ions. Added new method <TT>BuildPhysicsVector()</TT> |
---|
1557 | which invokes the build of physics vectors on demand in the initialisation |
---|
1558 | phase. Added method <TT>BuildPhysicsVector()</TT> according to base class |
---|
1559 | for <TT>G4ExtDEDXTable, G4SimpleMaterialStoppingICRU73, |
---|
1560 | G4MaterialStoppingICRU73</TT> and <TT>G4IronStoppingICRU73</TT>.</LI> |
---|
1561 | <LI><TT>G4ExtDEDXTable</TT>: new utility class to handle external |
---|
1562 | electronic stopping power tables for ions.</LI> |
---|
1563 | <LI>Use 'const' references for strings as arguments/return-values in material |
---|
1564 | properties tables and related classes. Inlined some methods and some minor |
---|
1565 | cleanup.</LI> |
---|
1566 | <LI>Added <TT>Entries()</TT> method to <TT>G4MaterialPropertyVector</TT> and |
---|
1567 | accessors for maps in <TT>G4MaterialPropertiesTable</TT>, required for |
---|
1568 | internal use in persistency of material properties. Make visible |
---|
1569 | <TT>GetEntry()</TT> accessor in <TT>G4MaterialPropertyVector</TT> for |
---|
1570 | use restricted to persistency.</LI> |
---|
1571 | <LI>Increased flexibily of G4SurfaceProperty and G4OpticalSurface classes |
---|
1572 | to allow for lookup-table boundary process simulations.</LI> |
---|
1573 | <LI><TT>G4Element</TT>: added method <TT>GetNbOfShellElectrons()</TT> |
---|
1574 | returning the number of electrons on a shell.</LI> |
---|
1575 | <LI><TT>G4DensityEffectData</TT>: added data from |
---|
1576 | Atom. Data Nucl. Data Tabl.30 (1984) 261, accessible via material name. |
---|
1577 | added method <TT>GetIndex()</TT></LI> |
---|
1578 | <LI><TT>G4IonisParamMat</TT>: added new members: <TT>Eplasma, AdjustmentFactor, |
---|
1579 | Delta0</TT> parameter of density effect parameterisation, and hook to |
---|
1580 | <TT>G4DensityEffectData</TT>. Fixed copy constructor. |
---|
1581 | Added new access method and method <TT>DensityCorrection()</TT>. |
---|
1582 | Fixed density effect computation; added plasma energy |
---|
1583 | computation and access to <TT>G4DensityEffectData</TT> by the atomic number.</LI> |
---|
1584 | </UL> |
---|
1585 | |
---|
1586 | <A NAME="part-notes"> |
---|
1587 | <H3><I>Particles</I></H3></A> |
---|
1588 | <UL> |
---|
1589 | <LI>Added new classes for "Reverse MonteCarlo" technique: |
---|
1590 | <TT>G4AdjointProton</TT> and light ions.</LI> |
---|
1591 | <LI>Make use of new experimental class <TT>G4NucleiPropertiesTableAME03</TT> |
---|
1592 | including data updated to the Ame-2003 atomic mass evaluation (II) by |
---|
1593 | G.Audi, A.H.Wapstra and C.Thibault, Nuclear Physics A729, 2003.</LI> |
---|
1594 | <LI>Removed obsolete class <TT>G4NucleiPropertiesTable</TT>.</LI> |
---|
1595 | <LI>Added method <TT>CreateAllIon()</TT> in <TT>G4IonTable</TT> |
---|
1596 | and added <TT>/particle/createAllIon</TT> UI command. By this method and |
---|
1597 | command, all stable ions are created.</LI> |
---|
1598 | <LI><TT>G4ParticleDefinition</TT> should be created in <TT>pre-init</TT> state; |
---|
1599 | a warning is thrown if constructors of <TT>G4ParticleDefinition</TT> are |
---|
1600 | called in a different application state.</LI> |
---|
1601 | <LI>Added <TT>CalculateAnomaly()</TT> method to <TT>G4ParticleDefinition</TT>.</LI> |
---|
1602 | <LI>Fixed small difference of mass of taus, mesons, and anti-baryons between |
---|
1603 | PDG-2009.</LI> |
---|
1604 | <LI>Changed <TT>G4ElectronOccupancies::MaxSizeOfOrbit</TT> to 10 to allow for |
---|
1605 | higher excited atom.</LI> |
---|
1606 | </UL> |
---|
1607 | |
---|
1608 | <A NAME="pers-notes"> |
---|
1609 | <H3><I>Persistency</I></H3></A> |
---|
1610 | <UL> |
---|
1611 | <LI>ASCII |
---|
1612 | <UL> |
---|
1613 | <LI>Inclusion of extruded and tessellated solids.</LI> |
---|
1614 | <LI>Additions of accessors and constructors of <TT>G4tgbVolume</TT> |
---|
1615 | and <TT>G4tgrVolume</TT>.</LI> |
---|
1616 | </UL></LI> |
---|
1617 | <LI>GDML |
---|
1618 | <UL> |
---|
1619 | <LI>Implemented virtual layer for allowing customisation of the writer |
---|
1620 | for user-extended schemas.</LI> |
---|
1621 | <LI>Implemented ability to write surface properties associated with |
---|
1622 | surfaces and material properties.</LI> |
---|
1623 | <LI>Allow for reading/writing of constant material properties.</LI> |
---|
1624 | <LI>Added support for the GDML <TT>assembly</TT> tag, implementing assemblies of |
---|
1625 | simple placements through <TT>G4AssemblyVolume</TT>.</LI> |
---|
1626 | <LI>Added support for GDML <TT>expression</TT> tag, implementing generic |
---|
1627 | expressions stored as literal constants.</LI> |
---|
1628 | <LI>Corrected handling of <TT>quantity</TT> tag; added missing caching |
---|
1629 | of evaluation.</LI> |
---|
1630 | <LI>Some code cleanup: rationalised inclusion of headers, replacing them |
---|
1631 | with forward declarations where possible.</LI> |
---|
1632 | </UL></LI> |
---|
1633 | </UL> |
---|
1634 | |
---|
1635 | <A NAME="lst-notes"> |
---|
1636 | <H3><I>Physics lists</I></H3></A> |
---|
1637 | <UL> |
---|
1638 | <LI>New physics lists and builders: |
---|
1639 | <UL> |
---|
1640 | <LI><TT>QGSP_FTFP_BERT</TT> based on <TT>QGSP_BERT</TT> replacing |
---|
1641 | the bridging <TT>LEP</TT> with <TT>FTFP</TT>, and transitioning from |
---|
1642 | <TT>BERT</TT> to <TT>FTFP</TT> between 7 and 9 <TT>GeV</TT>.</LI> |
---|
1643 | <LI><TT>FTFP_BERT_TRV</TT> list as variant of <TT>FTFP_BERT</TT> with |
---|
1644 | transition between 6 and 8 <TT>GeV</TT>.</LI> |
---|
1645 | <LI><TT>QGSP_BERT_TRV</TT>: with transition energies to use |
---|
1646 | <TT>BERT ]0,9.9]</TT>, <TT>LEP [9.5, 15]</TT> and |
---|
1647 | <TT>QGSP [10, inf[</TT>.</LI> |
---|
1648 | <LI>New physics-lists with special EM options: <TT>FTFP_BERT_EMV</TT>, |
---|
1649 | <TT>FTFP_BERT_EMX</TT>, <TT>QGSP_BERT_EMX</TT>, <TT>QGSP_BIC_EMY</TT> |
---|
1650 | (opt3 EM physics).</LI> |
---|
1651 | <LI><TT>CHIPS</TT> physics list, using <TT>CHIPS</TT> model for all |
---|
1652 | energies. Added two builders <TT>G4QNeutrinoPhysics, |
---|
1653 | G4QPhotoNuclearPhysics</TT> with messenger.</LI> |
---|
1654 | <LI><TT>QGSC_QGSC</TT>: using <TT>QGS</TT> model with interface to |
---|
1655 | <TT>CHIPS</TT> at all energies, starting from <TT>E=0</TT>; |
---|
1656 | for neutrons it still uses <TT>LHEP</TT> models for the radioactive |
---|
1657 | capture and fission.</LI> |
---|
1658 | <LI><TT>QGSC_CHIPS</TT>: using <TT>QGS</TT> model with interface to |
---|
1659 | <TT>CHIPS</TT> at all energies; for <TT>pA</TT> interactions |
---|
1660 | the native <TT>CHIPS</TT> process <TT>G4QCollision</TT> is used below |
---|
1661 | <TT>290 MeV</TT>.</LI> |
---|
1662 | <LI>Added builders for DNA, Livermore and Penelope physics processes. |
---|
1663 | Upper limit of Livermore models is set to <TT>1 GeV</TT>. |
---|
1664 | Adapted <TT>G4EmLivermorePolarizedPhysics</TT> builder as for the non |
---|
1665 | polarized case. Added high energy limit to <TT>e-</TT> models |
---|
1666 | in <TT>G4EmLivermorePhysics</TT> and <TT>G4EmLivermorePolarizedPhysics</TT></LI> |
---|
1667 | <LI>Added <TT>G4OpticalPhysics</TT> and <TT>G4OpticalPhysicsMessenger</TT> |
---|
1668 | classes.</LI> |
---|
1669 | </UL></LI> |
---|
1670 | <LI>Physics lists qualification changes (obsolete/partially |
---|
1671 | disabled/experimental/supported): |
---|
1672 | <UL> |
---|
1673 | <LI>Obsolete and disabled (removed): <TT>FTF_EMV</TT>, replaced by |
---|
1674 | <TT>FTFP_BERT_EMV</TT>; <TT>QGSC_EFLOW</TT>, replaced by |
---|
1675 | <TT>QGSC_CHIPS</TT>; <TT>QGSP_EMX</TT>, replaced by |
---|
1676 | <TT>QGSP_BERT_EMX</TT>.</LI> |
---|
1677 | <LI>Obsolete: <TT>FTFC, LHEP_BERT, LHEP_BERT_HP, LHEP_PRECO_HP |
---|
1678 | QGSP_BERT_DIF, QGSP_BERT_NQE, QGSP_DIF, QGSP_EMV, QGSP_EMV_NQE, |
---|
1679 | QGSP_NQE, QGSP_QEL, FTFP, QGSP, QGSC, QGSC_CHIPS, QGSC_EMV, |
---|
1680 | QGSC_QGSC.</TT>. |
---|
1681 | <LI>Explicitely marked experimental: <TT>QGSP_BERT_EMX, |
---|
1682 | QGSP_BERT_TRV, QGSP_FTFP_BERT, QGSP_INCL_ABLA</TT>.</LI> |
---|
1683 | <LI>Marked as supported: <TT>FTFP_BERT, FTFP_BERT_EMV</TT>.<BR> |
---|
1684 | <TT>G4PhysicsListFactory</TT>: updated choice of supported |
---|
1685 | physics-lists.</LI> |
---|
1686 | </UL></LI> |
---|
1687 | <LI>EM physics builders and options: |
---|
1688 | <UL> |
---|
1689 | <LI><TT>G4EmStandardPhysics, G4EmStandardPhysics_option1</TT>: use 9.2 |
---|
1690 | physics configuration; use <TT>ApplyCuts=true</TT>.</LI> |
---|
1691 | <LI><TT>G4EmStandardPhysics_option2</TT>: use <TT>G4eMultipleScattering</TT> |
---|
1692 | for <TT>e+-</TT>. Use default StepFunction for ions.</LI> |
---|
1693 | <LI><TT>G4EmStandardPhysics_option3</TT>: use updated <TT>G4UrbanMscModel2</TT> |
---|
1694 | and use <TT>G4RayleighScattering</TT> process.</LI> |
---|
1695 | <LI>Separated definition of processes for He3 and He4 ions; |
---|
1696 | <TT>G4eMultipleScattering</TT> for <TT>e+, e-, G4MuMultipleScattering</TT> |
---|
1697 | for muons.</LI> |
---|
1698 | <LI><TT>G4UrbanMscModel93</TT> for <TT>e+-</TT> and <TT>G4WentzelVIModel</TT> |
---|
1699 | for muons for all builders except <TT>Opt0</TT> and <TT>Opt1</TT>.</LI> |
---|
1700 | <LI><TT>G4ParameterizedIonModel</TT> for <TT>Opt3</TT> and all combined |
---|
1701 | builders.</LI> |
---|
1702 | <LI>StepFunction <TT>(0.1, 0.02*mm)</TT> for ions inside <TT>Opt2</TT>.</LI> |
---|
1703 | <LI><TT>G4EmStandardPhysics_option3, G4EmLivermorePhysics, |
---|
1704 | G4EmPenelopePhysics, G4EmLivermorePolarizedPhysics</TT>: |
---|
1705 | added <TT>G4NuclearStopping</TT> process for |
---|
1706 | GenericIon, He3, alpha particles. Set <TT>finalRange=10um</TT> |
---|
1707 | for ions.</LI> |
---|
1708 | </UL></LI> |
---|
1709 | <LI>Updates to lists: |
---|
1710 | <UL> |
---|
1711 | <LI>Added <TT>MaxEnergy()</TT> method in <TT>FTF</TT> builders.</LI> |
---|
1712 | <LI><TT>QBBC</TT> list: removed templated interface and moved inline code |
---|
1713 | to source; use new interface through <TT>G4VHadronPhysics</TT> class.</LI> |
---|
1714 | <LI>Change to <TT>G4HadroHElasticPhysics</TT> to make use of |
---|
1715 | <TT>G4WHadronElasticProcess</TT> as part of the design review for |
---|
1716 | elastic.</LI> |
---|
1717 | <LI>Change to <TT>QGSP_BERT_EMV</TT> to make use of |
---|
1718 | <TT>G4HadroHElasticPhysics</TT>.</LI> |
---|
1719 | <LI>Updated <TT>QBBC</TT> physics-list and fixed cross-section for |
---|
1720 | hadron elastic.</LI> |
---|
1721 | <LI><TT>QGSP_BERT_NOLEP</TT>: use <TT>G4HadronQElasticPhysics</TT>.</LI> |
---|
1722 | <LI>Added initial version of <TT>G4IonQMDPhysics</TT>.</LI> |
---|
1723 | </UL></LI> |
---|
1724 | </UL> |
---|
1725 | |
---|
1726 | <A NAME="run-notes"> |
---|
1727 | <H3><I>Run</I></H3></A> |
---|
1728 | <UL> |
---|
1729 | <LI><TT>G4VUserPhysicsList</TT>: |
---|
1730 | <LI>Added method <TT>CheckParticleList()</TT> to probe consistency of |
---|
1731 | list of particles before constructing processes; check being executed |
---|
1732 | within call to <TT>BuildPhysicsTable()</TT>. Added |
---|
1733 | <TT>DisableCheckParticleList()</TT> method as well and modified |
---|
1734 | <TT>BuildPhysicsTable()</TT> to avoid problem when ions are created |
---|
1735 | in the <TT>Pre-Init</TT> state.</LI> |
---|
1736 | <LI>Adapted implementation for handling proton cuts.</LI> |
---|
1737 | <LI><TT>G4RunManagerKernel</TT>: now invokes <TT>CheckParticleList()</TT> |
---|
1738 | from <TT>G4VUserPhysicsList</TT> just before invoking <TT>SetCuts()</TT>. |
---|
1739 | Also checking <TT>G4VUserPhysicsList</TT> to confirm no particle |
---|
1740 | is registered when <TT>G4RunManagerKernel</TT> is instantiated. |
---|
1741 | Fixed two minor bugs for the dump printout of regions.</LI> |
---|
1742 | <LI>Added UI command <TT>/run/setCutForAGivenParticle</TT> in |
---|
1743 | <TT>G4UserPhysicsListMessenger</TT>.</LI> |
---|
1744 | <LI>New classes implementing the "Reverse MonteCarlo" technique: |
---|
1745 | <TT>G4AdjointSimManager, G4AdjointSimMessenger, |
---|
1746 | G4AdjointPrimaryGeneratorAction</TT>.</LI> |
---|
1747 | </UL> |
---|
1748 | |
---|
1749 | <A NAME="track-notes"> |
---|
1750 | <H3><I>Track & Tracking</I></H3></A> |
---|
1751 | <UL> |
---|
1752 | <LI>Modified implementation of <TT>GetVelocity()</TT> for particle-change for |
---|
1753 | performance improvement.</LI> |
---|
1754 | <LI>Set <TT>lowEnergyLimit</TT> to <TT>1 eV</TT> in |
---|
1755 | <TT>G4ParticleChangeForLoss</TT>. Added method <TT>SetLowEnergyLimit()</TT>, |
---|
1756 | also to <TT>G4VUserTrackInformation</TT>; added a string property to |
---|
1757 | indicate type of UserTrackInformation.</LI> |
---|
1758 | <LI>Correction to <TT>G4SteppingManager::InvokeAtRestDoItProcs()</TT> in the |
---|
1759 | handling of <TT>G4Scintillation</TT> process.</LI> |
---|
1760 | <LI>New classes implementing the "Reverse MonteCarlo" technique: |
---|
1761 | <TT>G4AdjointCrossSurfChecker, G4AdjointSteppingAction</TT>.</LI> |
---|
1762 | <LI><TT>G4Trajectory, G4SmoothTrajectory, G4RichTrajectory</TT>: added initial |
---|
1763 | kinetic energy. <TT>G4RichTrajectory</TT>: added final kinetic energy. |
---|
1764 | <TT>G4RichTrajectoryPoint</TT>: added "remaining energy" at each step |
---|
1765 | and attributes.</LI> |
---|
1766 | </UL> |
---|
1767 | |
---|
1768 | <A NAME="vis-notes"> |
---|
1769 | <H3><I>Visualization</I></H3></A> |
---|
1770 | <UL> |
---|
1771 | <LI><B>Overall</B> |
---|
1772 | <UL> |
---|
1773 | <LI>Rich Trajectories and Rich Trajectory Points now include additional |
---|
1774 | information such as the complete volume path of the starting and ending |
---|
1775 | volume including all replica and copy numbers, etc.</LI> |
---|
1776 | <LI>Fixed bug in screen location and screen ratio handling for |
---|
1777 | <TT>X/Xm/Qt/Win32</TT> viewers.</LI> |
---|
1778 | <LI>Vector and bitmapped printing through <TT>/vis/ogl/printEPS</TT> is now |
---|
1779 | fully functional for all OpenGL viewers (previously only for OGLIX and |
---|
1780 | OGLSX). Related new commands are <TT>/vis/ogl/set/printSize</TT> and |
---|
1781 | <TT>/vis/ogl/set/printFilename</TT>.</LI> |
---|
1782 | </UL></LI> |
---|
1783 | <LI><B>Management</B> |
---|
1784 | <UL> |
---|
1785 | <LI><TT>G4VisManager</TT>: implemented handlers notification. A user may |
---|
1786 | notify scene handlers that the scene has changed, so that they may |
---|
1787 | rebuild their graphics database, if any, and redraw all views.</LI> |
---|
1788 | <LI>Introduced <TT>/vis/initialize</TT> UI command; instantiating |
---|
1789 | <TT>/vis/verbose</TT> and <TT>/vis/initialize</TT> in constructor |
---|
1790 | of <TT>G4VisManager</TT> so that a user may set verbosity before |
---|
1791 | initialisation.</LI> |
---|
1792 | <LI>New UI command, <TT>/vis/viewer/set/targetPoint</TT>, sets a specific |
---|
1793 | point to be the center of the view. Helps with doing extreme zoom in to |
---|
1794 | a specific point.</LI> |
---|
1795 | <LI>New UI command, <TT>/vis/scene/add/psHits</TT> for visualization of |
---|
1796 | scoring quantities to <TT>gMocrenFile</TT>.</LI> |
---|
1797 | <LI>Improved end of run event keeping information.</LI> |
---|
1798 | <LI>Allow for arbitrary viewer deletion (fixes some situations that had |
---|
1799 | caused crashes).</LI> |
---|
1800 | <LI>Allow refresh in <TT>GeomClosed</TT> as well as <TT>Idle</TT> state.</LI> |
---|
1801 | <LI><TT>G4VisExecutive</TT>: made methods inline.</LI> |
---|
1802 | </UL></LI> |
---|
1803 | <LI><B>Modeling</B> |
---|
1804 | <UL> |
---|
1805 | <LI>Added warning if logical volume is not defined.</LI> |
---|
1806 | <LI><TT>G4PhysicalVolumeModelTouchable</TT>: new class to allow |
---|
1807 | visualization attributes to be individually set for each volume within |
---|
1808 | a nested parameterization.</LI> |
---|
1809 | <LI>Added unit to <TT>setAux/StepPtsSizeType</TT> UI commands so that size |
---|
1810 | can be specified either in pixels or relative to screen size.</LI> |
---|
1811 | <LI>Added <TT>G4PSHitsModel</TT> for gMocren driver.</LI> |
---|
1812 | <LI><TT>G4ModelApplyCommands</TT>: added call to <TT>NotifyHandlers()</TT> |
---|
1813 | to force update of all viewers after a change of model, e.g., |
---|
1814 | trajectory colour, point size, etc.</LI> |
---|
1815 | </UL></LI> |
---|
1816 | <LI><B>Externals</B> |
---|
1817 | <UL> |
---|
1818 | <LI>gl2ps: Added dependency on zlib (even if <TT>G4LIB_BUILD_ZLIB</TT> is |
---|
1819 | not set).</LI> |
---|
1820 | <LI>Corrected setup for building DLLs on Windows.</LI> |
---|
1821 | </UL></LI> |
---|
1822 | <LI><B>gMocren</B> |
---|
1823 | <UL> |
---|
1824 | <LI>First Beta release of this new visualization driver to output data in |
---|
1825 | the <TT>gdd</TT> format used by the gMocren volume visualization tool. |
---|
1826 | <TT>gMocrenFile</TT> can include volume data from sensitive detector |
---|
1827 | volumes, or from command-based scoring meshes, in addition to detector |
---|
1828 | geometry and trajectories. Use the new UI command |
---|
1829 | <TT>/vis/scene/add/psHits</TT> to add scorer hits to gMocren output. |
---|
1830 | For details, see the Application Developers Guide and: |
---|
1831 | <A href="http://geant4.kek.jp/gMocren/">http://geant4.kek.jp/gMocren/</A>.</LI> |
---|
1832 | </UL></LI> |
---|
1833 | <LI><B>HepRep</B> |
---|
1834 | <UL> |
---|
1835 | <LI>New UI commands of the form <TT>/vis/heprep</TT> allow easy control of |
---|
1836 | output file name and output directory, whether a file name should be |
---|
1837 | reused (rather than having a sequential suffix appended at each new |
---|
1838 | file) and whether culled geometry volumes should be included.</LI> |
---|
1839 | <LI>Changed messenger to a singleton to facilitate sharing by |
---|
1840 | <TT>HepRepFile</TT> and <TT>HepRepXML</TT>.</LI> |
---|
1841 | <LI>Fixed a bug in representation of <TT>G4Tubs</TT> which had caused wrong |
---|
1842 | visualization for cases in which the tube was at an unusual angle.</LI> |
---|
1843 | </UL></LI> |
---|
1844 | <LI><B>OpenGL</B> |
---|
1845 | <UL> |
---|
1846 | <LI><TT>G4OpenGLQtViewer</TT>: ensure the GL frame size will be correct |
---|
1847 | by setting a zero size margin around.</LI> |
---|
1848 | <LI><TT>G4OpenGLStoredQtViewer</TT>: removed picking to true at |
---|
1849 | initialisation.</LI> |
---|
1850 | </UL></LI> |
---|
1851 | <LI><B>OpenInventor</B> |
---|
1852 | <UL> |
---|
1853 | <LI>Created new "externals" module for gl2ps library, moving out code from |
---|
1854 | OpenInventor module. Added ability to draw markers.</LI> |
---|
1855 | </UL></LI> |
---|
1856 | <LI><B>Qt</B> |
---|
1857 | <UL> |
---|
1858 | <LI>Continued improvements to this new driver. The <TT>Qt</TT> visualization |
---|
1859 | driver and the associated <TT>Qt</TT> User Interface now work well on |
---|
1860 | almost all platforms and with both Qt3 and Qt4 (but still considered a |
---|
1861 | Beta release due to a few rare combinations of commands on certain |
---|
1862 | platforms that can cause crashes).</LI> |
---|
1863 | </UL></LI> |
---|
1864 | <LI><B>RayTracer</B> |
---|
1865 | <UL> |
---|
1866 | <LI>Fixed a crash of <TT>RayTracerX</TT> on some platforms. |
---|
1867 | Addressing problem report |
---|
1868 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1072">#1072</A>.</LI> |
---|
1869 | </UL></LI> |
---|
1870 | </UL> |
---|
1871 | |
---|
1872 | <A NAME="env-notes"> |
---|
1873 | <H3><I>Environments</I></H3></A> |
---|
1874 | <UL> |
---|
1875 | <LI>G4Py: updated configuration script and wrappers to physics-lists.</LI> |
---|
1876 | <LI>Momo: updated documentation.</LI> |
---|
1877 | </UL> |
---|
1878 | |
---|
1879 | <A NAME="data-notes"> |
---|
1880 | <H3><I>Data sets</I></H3></A> |
---|
1881 | <UL> |
---|
1882 | <LI>New data for measured optical surface reflectance, RealSurface.1.0: |
---|
1883 | <UL> |
---|
1884 | <LI>Path to data controlled by variable <TT>G4REALSURFACEDATA</TT></LI> |
---|
1885 | </UL></LI> |
---|
1886 | <LI>New low-energy data set, G4EMLOW.6.9: |
---|
1887 | <UL> |
---|
1888 | <LI>Corrected corrupted data files: ioni/ion-sp-38.dat, ioni/ion-sp-56.dat |
---|
1889 | and ioni/ion-sp-57.dat. Addresses problem report |
---|
1890 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1042">#1042</A>.</LI> |
---|
1891 | <LI>Extended energy range of Champion e- elastic scattering model from |
---|
1892 | <TT>10 KeV</TT> up to <TT>10 MeV</TT>.</LI> |
---|
1893 | <LI>Extended high energy coverage of proton excitation and ionization.</LI> |
---|
1894 | <LI>Improved precision of e- ionisation Born model.</LI> |
---|
1895 | <LI>Included ICRU 73 stopping powers and revised tables provided by |
---|
1896 | P.Sigmund/Univ. of Southern Denmark.</LI> |
---|
1897 | <LI>Updated Geant4-DNA e- elastic Champion files and e- ionisation |
---|
1898 | Born files.</LI> |
---|
1899 | </UL></LI> |
---|
1900 | </UL> |
---|
1901 | |
---|
1902 | <A NAME="ex-notes"> |
---|
1903 | <H3><I>Examples</I></H3></A> |
---|
1904 | <UL> |
---|
1905 | <LI>Various fixes, improvements, adoption of new features.</LI> |
---|
1906 | <LI>Updated reference outputs.</LI> |
---|
1907 | <LI><B>advanced</B> |
---|
1908 | <UL> |
---|
1909 | <LI>Retired advanced examples: cosmicray_charging, radiation_monitor, |
---|
1910 | Tiara.</LI> |
---|
1911 | <LI>air_shower |
---|
1912 | <UL> |
---|
1913 | <LI>Changed UltraPhysicsList to use new processes |
---|
1914 | <TT>G4eMultipleScattering</TT>, <TT>G4MuMultipleScattering</TT> and |
---|
1915 | <TT>G4hMultipleScattering</TT>.</LI> |
---|
1916 | </UL></LI> |
---|
1917 | <LI>amsEcal |
---|
1918 | <UL> |
---|
1919 | <LI>New example implementing the AMS Ecal calorimeter.</LI> |
---|
1920 | </UL></LI> |
---|
1921 | <LI>brachytherapy |
---|
1922 | <UL> |
---|
1923 | <LI>Updated physics-list and analysis setup.</LI> |
---|
1924 | </UL></LI> |
---|
1925 | <LI>composite_calorimeter |
---|
1926 | <UL> |
---|
1927 | <LI>Use <TT>QGSP_BIC_EMY</TT> as default physics-list to test the |
---|
1928 | low-energy EM.</LI> |
---|
1929 | </UL></LI> |
---|
1930 | <LI>gammaray_telescope |
---|
1931 | <UL> |
---|
1932 | <LI>Updated physics-list setup.</LI> |
---|
1933 | </UL></LI> |
---|
1934 | <LI>hadrontherapy |
---|
1935 | <UL> |
---|
1936 | <LI>Reviewed physics implementation. Now Hadrontherapy can be launched |
---|
1937 | with physics-lists, packages and built-in physic models. |
---|
1938 | All models can be activated via macro command.</LI> |
---|
1939 | <LI>Implemented new low-energy models Livermore and Penelope.</LI> |
---|
1940 | <LI>Modified and revised the README (now in PDF format) and macro |
---|
1941 | files.</LI> |
---|
1942 | <LI>Added messengers to control the event number and to draw only |
---|
1943 | particular tracks.</LI> |
---|
1944 | <LI>Added a method to retrieve stopping power values for protons, |
---|
1945 | alphas and electrons.</LI> |
---|
1946 | <LI>Added local INCL/ABLA physics list for deuterons, tritons and |
---|
1947 | alphas.</LI> |
---|
1948 | <LI>Added first version of the IAEA benchmark geometry based on |
---|
1949 | E.Haettner's thesis. Added ability to remove the phantom by |
---|
1950 | setting its thickness to zero. Added ability to select the |
---|
1951 | geometry using macro commands.</LI> |
---|
1952 | <LI>Collect simulation metadata: number of events, distance of the |
---|
1953 | detector (IAEA geometry), depth of the phantom (IAEA geometry), |
---|
1954 | beam energy, energy error. Added ability to produce angular |
---|
1955 | distribution plots.</LI> |
---|
1956 | <LI>Added ability to change the name of the output file between runs.</LI> |
---|
1957 | <LI>Added ability to use command based scoring; IAEA geometry: now can |
---|
1958 | produce Bragg peak using command based scoring.</LI> |
---|
1959 | <LI>Added possibility to make a graphical user interface (GUI) using |
---|
1960 | the Qt libraries.</LI> |
---|
1961 | <LI>Added some functionalities in order to change, via messengers, |
---|
1962 | geometry, voxelization of the detector and disposition in the |
---|
1963 | space of the detector/phantom.</LI> |
---|
1964 | </UL></LI> |
---|
1965 | <LI>lAr_calorimeter |
---|
1966 | <UL> |
---|
1967 | <LI>Use <TT>QGSP_BIC_EMY</TT> as default physics-list to tests |
---|
1968 | the low-energy EM.</LI> |
---|
1969 | </UL></LI> |
---|
1970 | <LI>medical_linac |
---|
1971 | <UL> |
---|
1972 | <LI>New release of the example: updated physics models and deleted |
---|
1973 | old and no longer supported processes; added possibility to |
---|
1974 | activate the physics lists and reference physics-lists directly |
---|
1975 | via UI command; added possibility to set cuts and max allowed |
---|
1976 | step lenghts via UI commands.</LI> |
---|
1977 | </UL></LI> |
---|
1978 | <LI>microbeam |
---|
1979 | <UL> |
---|
1980 | <LI>Updated physics-list to migrated Livermore processes.</LI> |
---|
1981 | <LI>Corrected plotting fuctions and switching field value.</LI> |
---|
1982 | </UL></LI> |
---|
1983 | <LI>microdosimetry |
---|
1984 | <UL> |
---|
1985 | <LI>Updated physics-list to migrated Geant4-DNA processes. |
---|
1986 | Modified SteppingAction accordingly. Updated README.</LI> |
---|
1987 | <LI>Replaced H2O material by NIST <TT>G4_WATER</TT>.</LI> |
---|
1988 | <LI>Added GenericIon definition to PhysicsList.</LI> |
---|
1989 | </UL></LI> |
---|
1990 | <LI>radioprotection |
---|
1991 | <UL> |
---|
1992 | <LI>Updated physics-lists setup.</LI> |
---|
1993 | <LI>Changed analysis output format to XML.</LI> |
---|
1994 | </UL></LI> |
---|
1995 | <LI>Rich |
---|
1996 | <UL> |
---|
1997 | <LI>Added possibility to use <TT>QGSP_BIC_EMY</TT> as physics-list; |
---|
1998 | by default, the example's physics-list is used still.</LI> |
---|
1999 | </UL></LI> |
---|
2000 | <LI>xray_fluorescence |
---|
2001 | <UL> |
---|
2002 | <LI>Migrated physics-list to new low-energy processes design |
---|
2003 | <LI>Migrated <TT>XrayFluoDataSet</TT> to meet new specifications |
---|
2004 | in <TT>G4VEMDataSet</TT>.</LI> |
---|
2005 | </UL></LI> |
---|
2006 | <LI>xray_telescope |
---|
2007 | <UL> |
---|
2008 | <LI>Updated and simplified physics-list.</LI> |
---|
2009 | </UL></LI> |
---|
2010 | </UL></LI> |
---|
2011 | <LI><B>extended</B> |
---|
2012 | <UL> |
---|
2013 | <LI>analysis/A01 |
---|
2014 | <UL> |
---|
2015 | <LI><TT>A01DetectorConstruction, A01MagneticField</TT>: improved |
---|
2016 | handling of field. Addresses problem report |
---|
2017 | <A HREF="http://bugzilla-geant4.kek.jp/show_bug.cgi?id=1012">#1012</A>.</LI> |
---|
2018 | <LI>Removed A01Trajectory, to now use default G4Trajectory. |
---|
2019 | <LI>Update physics-list to use new multiple scattering classes. |
---|
2020 | <LI>Introduced use of G4UIExecutive. |
---|
2021 | <LI>General update to README.</LI> |
---|
2022 | </UL></LI> |
---|
2023 | <LI>biasing/ReverseMC01 |
---|
2024 | <UL> |
---|
2025 | <LI>New example demonstrating the use of Reverse MonteCarlo |
---|
2026 | technique in Geant4.</LI> |
---|
2027 | </UL></LI> |
---|
2028 | <LI>electromagnetic |
---|
2029 | <UL> |
---|
2030 | <LI>Physics list: renamed "standard" to "local"; "emstandard" to |
---|
2031 | "emstandard_opt0". Substituted obsolete low-energy physics |
---|
2032 | builders with builders from the reference physics_list library.</LI> |
---|
2033 | <LI>Replaced obsolete G4MultipleScattering in PhysListEmStandard.</LI> |
---|
2034 | <LI>Updated README and macro files.</LI> |
---|
2035 | </UL></LI> |
---|
2036 | <LI>electromagnetic/TestEm2 |
---|
2037 | <UL> |
---|
2038 | <LI>Substituted obsolete low-energy physics builders with builders |
---|
2039 | from the 'physics_list' module.</LI> |
---|
2040 | <LI>Reduced number of hard-coded materials, added a possiblity to |
---|
2041 | use NIST materials.</LI> |
---|
2042 | <LI>Some cleanup to macro files.</LI> |
---|
2043 | </UL></LI> |
---|
2044 | <LI>electromagnetic/TestEm3 |
---|
2045 | <UL> |
---|
2046 | <LI>Fix to <TT>HistoManager::PrintHisto()</TT>: avoid empty ascii |
---|
2047 | file.</LI> |
---|
2048 | <LI>Removed <TT>G4EMConfigurator</TT> in physics-list.</LI> |
---|
2049 | </UL></LI> |
---|
2050 | <LI>electromagnetic/TestEm5 |
---|
2051 | <UL> |
---|
2052 | <LI>Added UI command <TT>/testem/phys/cutLimit</TT> allowing to change |
---|
2053 | low limit for production threshold.</LI> |
---|
2054 | <LI>Added missing notification to <TT>G4RunManager</TT> when geometry |
---|
2055 | or material are modified between runs.</LI> |
---|
2056 | <LI>Added PAI models configuration to Physics List.</LI> |
---|
2057 | <LI>Modified cuts in PhysicsList. Added <TT>blaha.mac</TT> input macro.</LI> |
---|
2058 | <LI>Removed UI command <TT>/testem/phys/cutLimit</TT>.</LI> |
---|
2059 | <LI>PhysicsList: removed obsolete low-energy EM builders, substituted |
---|
2060 | by builders from the 'physics_list' module; added "standardGS" |
---|
2061 | option: use GoudsmitSaunderson multiple-scattering model.</LI> |
---|
2062 | <LI>New local physics-list <TT>PhysListEmStandardGS</TT>.</LI> |
---|
2063 | <LI>Removed G4EMConfigurator in physics-list.</LI> |
---|
2064 | </UL></LI> |
---|
2065 | <LI>electromagnetic/TestEm6 |
---|
2066 | <UL> |
---|
2067 | <LI>Increased upper limit of energy in the tables to <TT>1000 TeV</TT>.</LI> |
---|
2068 | <LI>Added StackingAction to allow for removal of secondary particles.</LI> |
---|
2069 | </UL></LI> |
---|
2070 | <LI>electromagnetic/TestEm9 |
---|
2071 | <UL> |
---|
2072 | <LI>Changed options to physics-list.</LI> |
---|
2073 | </UL></LI> |
---|
2074 | <LI>electromagnetic/TestEm18 |
---|
2075 | <UL> |
---|
2076 | <LI>Added UI command <TT>/testem/phys/cutLimit</TT> allowing to change |
---|
2077 | low limit for production threshold.</LI> |
---|
2078 | <LI>Changed options to physics-list.</LI> |
---|
2079 | <LI>Removed UI command <TT>/testem/phys/cutLimit</TT>.</LI> |
---|
2080 | </UL></LI> |
---|
2081 | <LI>electromagnetic/TestEm13 |
---|
2082 | <UL> |
---|
2083 | <LI>Replacement with new Livermore and Penelope physics-lists.</LI> |
---|
2084 | </UL></LI> |
---|
2085 | <LI>electromagnetic/TestEm14 |
---|
2086 | <UL> |
---|
2087 | <LI>Replacement with new Livermore and Penelope physics-lists.</LI> |
---|
2088 | </UL></LI> |
---|
2089 | <LI>exoticphysics/monopole |
---|
2090 | <UL> |
---|
2091 | <LI>Added messenger to define mass and charge of the monopole.</LI> |
---|
2092 | </UL></LI> |
---|
2093 | <LI>field |
---|
2094 | <UL> |
---|
2095 | <LI>Fixed density of STP Carbon Dioxide in DetectorConstruction.</LI> |
---|
2096 | </UL></LI> |
---|
2097 | <LI>field/field04 |
---|
2098 | <UL> |
---|
2099 | <LI>Introduced <TT>/rndm/autoSeed</TT> UI command and changed default |
---|
2100 | seeding of random generator.</LI> |
---|
2101 | <LI>Changed <TT>F04PhysicsList</TT> and <TT>F04PhysicsListMessenger</TT> |
---|
2102 | to use <TT>G4PhysListFactory</TT>.</LI> |
---|
2103 | <LI>Introduced use of <TT>G4UIExecutive</TT>.</LI> |
---|
2104 | </UL></LI> |
---|
2105 | <LI>field/field05 |
---|
2106 | <UL> |
---|
2107 | <LI>New example to test the spin-frozen condition whereby the g-2 |
---|
2108 | muon spin precession is canceled by an applied electric field. |
---|
2109 | Courtesy of Hiromi Iinuma from KEK.</LI> |
---|
2110 | </UL></LI> |
---|
2111 | <LI>hadronic/Hadr00 |
---|
2112 | <UL> |
---|
2113 | <LI>Added possibility to define physics-list as a job parameter.</LI> |
---|
2114 | <LI>Added script for the test run of all physics-lists.</LI> |
---|
2115 | </UL></LI> |
---|
2116 | <LI>hadronic/Hadr01 |
---|
2117 | <UL> |
---|
2118 | <LI>Updated physics-list. Using <TT>FTFP_BERT_TRV</TT>.</LI> |
---|
2119 | <LI>Added histograms on energy depositions: total/electromagnetic, |
---|
2120 | pion/proton.</LI> |
---|
2121 | </UL></LI> |
---|
2122 | <LI>medical/DICOM |
---|
2123 | <UL> |
---|
2124 | <LI>Changed DICOM Handler to read CT files coming from CONQUEST |
---|
2125 | DICOM server.</LI> |
---|
2126 | </UL></LI> |
---|
2127 | <LI>medical/electronScattering, electronScattering2 |
---|
2128 | <UL> |
---|
2129 | <LI>Two alternate approaches to simulating the published electron |
---|
2130 | scattering benchmark experiment of C. K. Ross et al.</LI> |
---|
2131 | </UL></LI> |
---|
2132 | <LI>medical/fanoCavity[1,2] |
---|
2133 | <UL> |
---|
2134 | <LI>Corrected computation of 'error' in EndOfRun.</LI> |
---|
2135 | <LI>Using GoudsmitSaunderson multiple-scattering model. |
---|
2136 | Added cut for proton recoil in case of Single Scattering.</LI> |
---|
2137 | </UL></LI> |
---|
2138 | <LI>medical/GammaTherapy |
---|
2139 | <UL> |
---|
2140 | <LI>Updated physics-list for EM.</LI> |
---|
2141 | </UL></LI> |
---|
2142 | <LI>optical/LXe |
---|
2143 | <UL> |
---|
2144 | <LI>Exhibit the usage of a complex index of refraction for the photo |
---|
2145 | cathode.</LI> |
---|
2146 | <LI>Use of <TT>G4OpticalPhysics</TT> builder/messenger, instead of |
---|
2147 | <TT>LXeOpticalPhysics</TT>.</LI> |
---|
2148 | <LI>Introduced use of <TT>G4UIExecutive</TT>.</LI> |
---|
2149 | </UL></LI> |
---|
2150 | <LI>optical/wls |
---|
2151 | <UL> |
---|
2152 | <LI>New example tracking optical photons in a realistic plastic |
---|
2153 | scintillator bar geometry with a wave length shifting (WLS) fiber |
---|
2154 | and propagating the WLS photons inside the fiber. |
---|
2155 | Courtesy of Siu Pak Mok from TRIUMF.</LI> |
---|
2156 | </UL></LI> |
---|
2157 | <LI>persistency/gdml |
---|
2158 | <UL> |
---|
2159 | <LI><TT>G01</TT>: added new GDML samples for matrices+loops and |
---|
2160 | optical-surfaces. Modified matricesandloops.gdml, following |
---|
2161 | new specifications for loops. |
---|
2162 | Added possibility to run application in batch mode giving a macro |
---|
2163 | as input (e.g.: <TT>load_gdml solids.gdml g01.gdml g01.in</TT>); |
---|
2164 | option to be used by system testing for batch test. |
---|
2165 | Added assembly.gdml to demonstrate support for 'assembly' tags. |
---|
2166 | Added usage of 'expression' and 'quantity' in solids.gdml.</LI> |
---|
2167 | <LI><TT>G02</TT>: |
---|
2168 | Added missing inclusion of headers after cleanup.</LI> |
---|
2169 | <LI><TT>G03</TT>: |
---|
2170 | Extended example to show also capability to write extended schema; |
---|
2171 | added custom writer class. |
---|
2172 | Renamed translation unit for main to "gdml_ext.cc".</LI> |
---|
2173 | </UL></LI> |
---|
2174 | <LI>persistency/P03 |
---|
2175 | <UL> |
---|
2176 | <LI>Use G4XMultipleScattering in physics-list.</LI> |
---|
2177 | </UL></LI> |
---|
2178 | <LI>polarisation/Pol01 |
---|
2179 | <UL> |
---|
2180 | <LI>Updated multiple-scattering physics.</LI> |
---|
2181 | </UL></LI> |
---|
2182 | <LI>radioactivedecay/exrdm |
---|
2183 | <UL> |
---|
2184 | <LI>Fixed trivial compilation warning when compiled without |
---|
2185 | <TT>G4ANALYSIS_USE</TT>.</LI> |
---|
2186 | </UL></LI> |
---|
2187 | </UL></LI> |
---|
2188 | <LI><B>novice</B> |
---|
2189 | <UL> |
---|
2190 | <LI>Introduced use of <TT>G4UIExecutive</TT>.</LI> |
---|
2191 | <LI>N02 |
---|
2192 | <UL> |
---|
2193 | <LI>Use G4MuMultipleScattering for muons; separated alpha |
---|
2194 | from GenericIon.</LI> |
---|
2195 | </UL></LI> |
---|
2196 | <LI>N03 |
---|
2197 | <UL> |
---|
2198 | <LI>Use G4MuMultipleScattering for muons; separated alpha |
---|
2199 | from GenericIon.</LI> |
---|
2200 | </UL></LI> |
---|
2201 | <LI>N06 |
---|
2202 | <UL> |
---|
2203 | <LI>Use G4eMultipleScattering, G4MuMultipleScattering and |
---|
2204 | G4hMultipleScattering instead of standard G4MultipleScattering.</LI> |
---|
2205 | </UL></LI> |
---|
2206 | </UL></LI> |
---|
2207 | </UL> |
---|
2208 | |
---|
2209 | <HR> |
---|
2210 | |
---|
2211 | </BODY> |
---|
2212 | </HTML> |
---|