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The events are produced assuming 100% polarization for the initial state electron and positron; different files for the same final state correspond to different polarization sign combinations. The variable IDRUPLH indexes the different final states and polarizations. Assume, for example, that a process has IDRUPLH=14995 . The stdhep file is ftp://ftp-lcd.slac.stanford.edu/ilcilc2/whizdata/ILC500/w14995_01.stdhep and the information about the generation of this file can be found in the directory ftp://ftp-lcd.slac.stanford.edu/ilcilc2/ILC500/StandardModeldoc/run_output/w14995/run_01/ .
The log file is ftp://ftp-lcd.slac.stanford.edu/ilcilc2/ILC500/StandardModeldoc/run_output/w14995/run_01/whizard.log ,
the whizard input file is ftp://ftp-lcd.slac.stanford.edu/ilcilc2/ILC500/StandardModeldoc/run_output/w14995/run_01/whizard.in
and cross section information is in ftp://ftp-lcd.slac.stanford.edu/ilcilc2/ILC500/StandardModeldoc/run_output/w14995/run_01/whizard.n3n3n3n3ss_o.out
The WHIZARD Monte Carlo version 1.40 is used for parton generation. The For processes without an on-shell Higgs boson in the final state the Higgs mass is assumed to be 2000 GeV. For process with an on-shell Higgs boson in the final state the Higgs mass is assumed to
be 120 GeV. The Makefile and build log files for this implementation of WHIZARD can be found in ftp://ftp-lcd.slac.stanford.edu/ilcilc2/ILC500/StandardModeldoc/whizard-v1r4p0
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Electron/Positron Beam Properties: Beamstrahlung and LINAC Energy Spread
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