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LASERQED

  LASERQED COMPTONtex2html_wrap_inline7312BREITWHEELER[,]tex2html_wrap_inline7850 NPH=tex2html_wrap_inline7854, [NY=tex2html_wrap_inline7404,] [NXI=tex2html_wrap_inline7862,] [NLAMBDA=tex2html_wrap_inline7866,] [NQ=tex2html_wrap_inline7870,] XIMAX=tex2html_wrap_inline7874, LAMBDAMAX=tex2html_wrap_inline7878, ETAMAX=tex2html_wrap_inline7882, [PMAX=tex2html_wrap_inline7886,] [ENHANCEFUNCTION=tex2html_wrap_inline7890,] ;
COMPTONtex2html_wrap_inline7312BREITWHEELER
   Specifies which parameters to define here.
tex2html_wrap_inline7854
Maximum number of laser photons to be absorbed in one process.
If <0, turn off Compton or Breit-Wheeler.
If =0, use linear Compton/Breit-Wheeler formula.
If tex2html_wrap_inline7900, use nonlinear formula.
Note that tex2html_wrap_inline7902 and tex2html_wrap_inline7904 are different. The former is the limit of tex2html_wrap_inline7906, which contains tex2html_wrap_inline7904 term only, where as the latter is a truncation of the exact series with respect to tex2html_wrap_inline7854. When tex2html_wrap_inline7902, none of the following variables are needed.
When tex2html_wrap_inline7914, only longitudinal polarization is considered and the lasers must be circularly polarized by 100% (i.e., tex2html_wrap_inline7916, tex2html_wrap_inline7918).
tex2html_wrap_inline7404
Number of abscissa for final energy. Default=20.
tex2html_wrap_inline7862
Number of abscissa for tex2html_wrap_inline7924 parameter. Default=20.
tex2html_wrap_inline7866
Number of abscissa for tex2html_wrap_inline7928 parameter. Applies to Compton case only. Default=20.
tex2html_wrap_inline7870
Number of abscissa for q parameter. Applies tp Breit-Wheeler case only. Default=50.
tex2html_wrap_inline7874
Maximum value of tex2html_wrap_inline7924 for the table.
tex2html_wrap_inline7878
Maximum value of tex2html_wrap_inline7928 for the table. Applies to Compton case only.
tex2html_wrap_inline7882
Maximum value of tex2html_wrap_inline7944 for the table. Applies to Breit-Wheeler case only.
tex2html_wrap_inline7886
Maximum probability of events per one time step. If the computed probability exceeds tex2html_wrap_inline7886, CAIN of present version stops with a message.
tex2html_wrap_inline7890
Defines a function in order to enhance a part of spectrum.   It is defined as an expression containing Y as the final energy parameter (tex2html_wrap_inline7952Ytex2html_wrap_inline7954). Its value must be tex2html_wrap_inline7900 for tex2html_wrap_inline7952Ytex2html_wrap_inline7954. Generally speaking, Y close to 1 generates low energy charged particles. For example,
E NH=1+Step(Y-0.8)*(Y-0.8)*10
will enhance the events with Y>0.8 by a factor upto 3 (at Y=1).
In the program, the real spectrum function is multiplied by tex2html_wrap_inline7890 and, when an event is generated, the created particles are asigned a weight tex2html_wrap_inline7966.
Note that tex2html_wrap_inline7890 slightly larger than 1 is useless (even harmful) because a small fraction tex2html_wrap_inline7970 of the parent particle will remain as a macro-particle, causing a waste of computing time. In the example above, tex2html_wrap_inline7972 exactly for Y<0.8.
This function is used only during the initialization by LASERQED command. Therefore, if the expression contains user-defined parameters, their values at the time of LASERQED command are used. Changing them afterwards will not affect the computation.

See Sec.5.7.3 and Appendix.A for more detail


next up previous contents index
Next: CFQED Up: Commands Previous: LASER

Toshiaki Tauchi
Thu Dec 3 17:27:26 JST 1998