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/MultiplicityAnalysis [ Modules ]

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NAME

module MultiplicityAnalysis

PURPOSE

This module contains collision independent analysis routines concerning multiplicity of particles

INPUTS

(none)


MultiplicityAnalysis/Multiplicity_Reset [ Subroutines ]

[ Top ] [ MultiplicityAnalysis ] [ Subroutines ]

NAME

subroutine Multiplicity_Reset

PURPOSE


MultiplicityAnalysis/Multiplicity_AddEvent [ Subroutines ]

[ Top ] [ MultiplicityAnalysis ] [ Subroutines ]

NAME

subroutine Multiplicity_AddEvent(E)

PURPOSE


MultiplicityAnalysis/Multiplicity_Write [ Subroutines ]

[ Top ] [ MultiplicityAnalysis ] [ Subroutines ]

NAME

subroutine Multiplicity_Write(Prefix,iFile)

PURPOSE


MultiplicityAnalysis/Multiplicity_Ave.dat [ Output files ]

[ Top ] [ MultiplicityAnalysis ] [ Output files ]

NAME

file Multiplicity_Ave.dat

PURPOSE

The file shows the average multiplicity and its standard deviation for the various outging hadrons

Columns:

  • #1: running variable (see Multiplicity_Distr.dat for explanation)
  • #2: average multiplicity of "ALL" particles
  • #3: standard deviation (of average multiplicity) of "ALL" particles
  • #4: average multiplicity of "ALL CHARGED" particles
  • #5: standard deviation (of average multiplicity) of "ALL CHARGED" particles
  • #6: average multiplicity of "charge -1" particles
  • #7: standard deviation (of average multiplicity) of "charge -1" particles
  • #8: average multiplicity of "charge 0" particles
  • #9: standard deviation (of average multiplicity) of "charge 0" particles
  • #10: average multiplicity of "charge +1" particles
  • #11: standard deviation (of average multiplicity) of "charge +1" particles
  • #12: average multiplicity of "ALL pions"
  • #13: standard deviation (of average multiplicity) of "ALL pions"
  • #14: average multiplicity of "pion -1"
  • #15: standard deviation (of average multiplicity) of "pion -1"
  • #16: average multiplicity of "pion 0"
  • #17: standard deviation (of average multiplicity) of "pion 0"
  • #18: average multiplicity of "pion +1"
  • #19: standard deviation (of average multiplicity) of "pion +1"
  • #20: average multiplicity of "ALL nucleons"
  • #21: standard deviation (of average multiplicity) of "ALL nucleons"
  • #22: average multiplicity of "neutrons"
  • #23: standard deviation (of average multiplicity) of "neutrons"
  • #24: average multiplicity of "protons"
  • #25: standard deviation (of average multiplicity) of "protons"
  • #26: average multiplicity of "ALL kaons"
  • #27: standard deviation (of average multiplicity) of "ALL kaons"
  • #28: average multiplicity of "Kbar -1"
  • #29: standard deviation (of average multiplicity) of "Kbar -1"
  • #30: average multiplicity of "Kbar 0"
  • #31: standard deviation (of average multiplicity) of "Kbar 0"
  • #32: average multiplicity of "K 0"
  • #33: standard deviation (of average multiplicity) of "K 0"
  • #34: average multiplicity of "K +1"
  • #35: standard deviation (of average multiplicity) of "K +1"
  • #36: average multiplicity of "Lambda"
  • #37: standard deviation (of average multiplicity) of "Lambda"


MultiplicityAnalysis/Multiplicity_Distr.dat [ Output files ]

[ Top ] [ MultiplicityAnalysis ] [ Output files ]

NAME

file Multiplicity_Distr.dat

PURPOSE

The file shows the multiplicity distributions of various hadrons in the final state

The commented line with one number only (looks like # 1.000) is the "running variable" from your jobcard, For example, for neutrino mode runs versus neutrino energy (mode 0 or mode 6) this is neutrino energy for neutrino mode runs versus Q2 (mode 3) this is Q2 For neutrino model calculations with a given flux this 'running variable' is a dummy, its the last energy in the flux sampling For each value of "running variable" you have several (="num_runs_sameEnergy") blocks of output separated by two empty lines For flux-averaged results these blocks should be (within statistics) the same. This can be used to check if statistics are sufficient

Columns:

  • #1: number of outgoing particles (integer)
  • #2: percentage of events with #1 particles of type "ALL"
  • #3: percentage of events with #1 particles of type "ALL CHARGED"
  • #4: percentage of events with #1 particles of type "charge -1"
  • #5: percentage of events with #1 particles of type "charge 0"
  • #6: percentage of events with #1 particles of type "charge +1"
  • #7: percentage of events with #1 particles of type "ALL pions"
  • #8: percentage of events with #1 particles of type "pion -1"
  • #9: percentage of events with #1 particles of type "pion 0"
  • #10: percentage of events with #1 particles of type "pion +1"
  • #11: percentage of events with #1 particles of type "ALL baryons"
  • #12: percentage of events with #1 particles of type "neutrons"
  • #13: percentage of events with #1 particles of type "protons"
  • #14: percentage of events with #1 particles of type "ALL kaons" (incl antikaons)
  • #15: percentage of events with #1 particles of type "Kbar -1"
  • #16: percentage of events with #1 particles of type "Kbar 0"
  • #17: percentage of events with #1 particles of type "K0"
  • #18: percentage of events with #1 particles of type "K+"
  • #19: percentage of events with #1 particles of type "Lambda"
  • In the following columns all values in one column are idential, since col. 1 is irrelevant for multiplicities
  • #20: average multiplicity of "ALL"
  • #21: average multiplicity of "ALL CHARGED"
  • #22: average multiplicity of "charge -1"
  • #23: average multiplicity of "charge 0"
  • #24: average multiplicity of "charge +1"
  • #25: average multiplicity of "ALL pions"
  • #26: average multiplicity of "pion -1"
  • #27: average multiplicity of "pion 0"
  • #28: average multiplicity of "pion +1"
  • #29: average multiplicity of "ALL baryons"
  • #30: average multiplicity of "neutrons"
  • #31: average multiplicity of "protons"
  • #32: average multiplicity of "ALL kaons"
  • #33: average multiplicity of "Kbar -1"
  • #34: average multiplicity of "Kbar 0"
  • #35: average multiplicity of "K0"
  • #36: average multiplicity of "K+"
  • #37: average multiplicity of "Lambda"

NOTES

The numbers in one row should NOT add-up in any way

Example: consider an event with 1 neutron, 1 pi+ and 1pi0 in the final state; it will contribute to "3 ALL", "1 ALL CHARGED", "0 charge -1", "2 charge 0", "1 charge +1",

                        "2 ALL pions", "0 pion -1", "1 pion 0", "1 pion+", "1 ALL baryons", "1 neutrons", "0 protons"

In each column (in each block) the probabilities should sum up to 1