Changes between Version 7 and Version 8 of jobCards/omegaTaps

Timestamp:

May 6, 2009, 1:41:51 PM (16 years ago)

Author:

jweil

Comment:

--

jobCards/omegaTaps

@@ -5 +5 @@
 
 == Target definition ==
+
 The namelist ''target'' controls the target. Do not modify the ''fermimotion'' and ''densitySwitch_Static'' switches besides for testing.
 {{{
@@ -37 +38 @@
 $lowPhotonAnalysis
 ! Analysis flags
-outputEvents   =.true.     ! Print events to file
-photonAnalyse  =.true.     ! Generate analysis for final state photons
+outputEvents          = .true.     ! Print events to file
+outputEvents_onlyFree = .true.     ! Prints only "free" nucleons to file (.false.=print all nucleons)
+photonAnalyse         = .true.     ! Generate analysis for final state photons
 ! Switch off unnessary analysis
-KruscheOutput  =.false.
-fissumOutput   =.false.
-twoPiOutput    =.false.
-$end
-}}}
+KruscheOutput = .false.
+fissumOutput  = .false.
+twoPiOutput   = .false.
+$end
+}}}
+
+
 == General Input ==
+
 These namelists control the general input for each run:
  * The variable ''numEnsembles'' defines how many ensembles of test-particles are used to model a  physical one, so it defines the granularity of our numerical realization. Use ''numEnsembles=1000...10000'' for a real calculation.
@@ -86 +91 @@
 $end
 }}}
+
+
 == Numerical details ==
+
 Don't touch!
 {{{
@@ -105 +113 @@
 predictorCorrector=.true.  ! Whether to use a predictor/corrector algorithm to do the propagation
 $end
-
-
-}}}
+}}}
+
+
 == Input for potentials ==
+
 Influences the hadronic potentials. In the scenario below we use no potential for the mesons and our standard Skyrme-type potential for the baryons.
 {{{
-
 $Coulomb
 CoulombFlag=.false.
@@ -137 +145 @@
              ! 2= 100 MeV *rho/rhoNull
 $end
-
-}}}
+}}}
+
+
 == The collision term ==
+
 Here one can modify the collision term, e.g. by switching off three-body interactions. The scenario below is standard, so don't modify besides for testing. Note that the parameter ''minimumEnergy      =0.005'' in the namelist ''insertion'' removes all final state nucleons which have kinetic energies less than 5 MeV. 
 {{{
-
 $hadronFormation
 tauForma=0.8             ! formation proper time in restframe of hadron
@@ -172 +181 @@
 $end
 
-
-
 $initStability
 stabilityFlag(101) = 4 ! Let Pi^0 Decay
@@ -181 +188 @@
 MDCY(102,1)=1 ! KC code of pi0, not KF!  !Pi^0 unstable in Pythia
 $end 
-
-
-}}}
+}}}
+
+
 == The widths of the particles ==
+
 The scenario below corresponds to a broadening of the Delta, but to no broadening of any other particle. Such a broadening can be included by setting
 ''mediumSwitch_coll=.true.'' in the namelist width_Baryon and/or ''mediumSwitch=.true.'' in the namelist width_Meson.
@@ -198 +206 @@
 $end
 }}}
+
+
 == Temperature and thermodynamics ==
+
 Don't touch this! Otherwise computation time blows up
 {{{