Changeset 1222 for trunk/documents/UserDoc/DocBookUsersGuides/PhysicsReferenceManual/latex/electromagnetic/standard
- Timestamp:
- Dec 16, 2009, 12:14:47 PM (16 years ago)
- Location:
- trunk/documents/UserDoc/DocBookUsersGuides/PhysicsReferenceManual/latex/electromagnetic/standard
- Files:
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- 14 added
- 2 edited
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Fig1.eps (added)
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Fig2.eps (added)
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Fig3.eps (added)
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MuPgen.tex (added)
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PsiGen.eps (added)
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SigApRat.eps (added)
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SigTot.eps (added)
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dsigdx.eps (added)
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f1t_10.eps (added)
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f1t_1000.eps (added)
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f1tgen.eps (added)
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hion.tex (modified) (1 diff)
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msc.tex (modified) (3 diffs)
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rho.eps (added)
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thetaPlus.eps (added)
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xPlusGen.eps (added)
Legend:
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trunk/documents/UserDoc/DocBookUsersGuides/PhysicsReferenceManual/latex/electromagnetic/standard/hion.tex
r1211 r1222 244 244 \subsubsection{Nuclear Stopping} 245 245 246 For scaled energies below $T_{lim} = 2 MeV$ the contribution of non-ionizing energy loss 247 needs to be taken into account. The additional energy loss due to {\it nuclear stopping power} 248 $\Delta T_N \Delta s$ is added the the energy loss. The process {\it G4ionIonisation} 249 has a flag, which allows to switch on or off this correction. For that the method\\ 250 \\ 251 {\it G4ionIonisation::ActivateNuclearStopping(G4bool)} 252 \\ 253 \\ 254 can be used. By default 255 this correction is active and the ICRU'49 parameterisation \cite{hion.ICRU49} is used. 246 Nuclear stopping due to elastic ion-ion scattering since Geant4 v9.3 247 can be simulated with the continuous process 248 {\it G4NuclearStopping}. By default 249 this correction is active and the ICRU'49 parameterisation \cite{hion.ICRU49} is used, 250 which is implemented in the model class {\it G4ICRU49NuclearStoppingModel}. 256 251 257 252 -
trunk/documents/UserDoc/DocBookUsersGuides/PhysicsReferenceManual/latex/electromagnetic/standard/msc.tex
r1211 r1222 15 15 \item 16 16 G4MuMultipleScattering. 17 \item18 G4MultipleScattering;19 17 \end{itemize} 20 18 For concrete simulation the {\it G4VMscModel} interface is used, which is an extension … … 22 20 \begin{itemize} 23 21 \item 24 G4UrbanMscModel ;22 G4UrbanMscModel90 - Geant4 v9.0 applied to muons, hadrons and ions; 25 23 \item 26 G4UrbanMscModel 2;24 G4UrbanMscModel92 - Geant4 v9.2 (current default) applied for electron and positron; 27 25 \item 28 G4UrbanMscModel9 0;26 G4UrbanMscModel93 - Geant4 v9.3 applied for electron and positron for Option2, Option3 and other EM Physics Lists; 29 27 \item 30 G4WentzelVIModel. 28 G4GoudsmitSaundersonModel - for electrons and positrons (beta-version); 29 \item 30 G4WentzelVIModel - for muons and hadrons, should be included in Physics Lists together with G4CoulombScattering process; 31 31 \end{itemize} 32 The last model is not yet in the production mode, so below we will concentrate 33 on models developed by L.~Urban \cite{msc.urban}. Today default model for 34 electrons and positrons is {\it G4UrbanMscModel2}, for hadrons - {\it G4UrbanMscModel90}. 32 The last models are not yet in the production mode, so below we will concentrate 33 on models developed by L.~Urban \cite{msc.urban}. 35 34 36 35 \subsection{Introduction} … … 811 810 08.12.08 revised by L. Urb\'an, for Geant4 V9.2 \\ 812 811 11.12.08 minor revision by V. Ivanchenko \\ 812 11.12.09 minor revision by V. Ivanchenko, for Geant4 v9.3 \\ 813 813 814 814 \begin{latexonly}
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