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RunI.dat
(run){
### basic settings ###
SCL:=0.5;
J1CUT:=80.0;
J2CUT:=60.0;
ETAMAX:=2.8;
RJET:=0.4;
DIPA:=0.1;
######################
EVENTS 10;
BATCH_MODE 2;
OUTPUT 2;
EVT_FILE_PATH=Event/I_HTSCL_mstw08_jJ1CUT_jJ2CUT_eETAMAX_adDIPA/
## for high multiplicity lower values of
## DIPOLE_ALPHA are preferred.
DIPOLE_ALPHA=DIPA
}(run);
(beam){
BEAM_1 = 2212; BEAM_ENERGY_1 = 3500;
BEAM_2 = 2212; BEAM_ENERGY_2 = 3500;
}(beam);
(isr){
PDF_LIBRARY MSTW08Sherpa;
PDF_SET mstw2008nlo;
};
(processes){
Process 93 93 -> 93 93;
## add extra jets e.g. Process 93 93 -> 93 93 93 for 3 jets
NLO_QCD_Mode Fixed_Order;
NLO_QCD_Part I;
Order_EW 0;
End process;
}(processes);
## top loops are not included the current version of NJet
## to ensure the top quark is not included in the running
## of alpha_s we set the mass to a large value
(model){
MASS[6] = 1e10
}(model)
(selector){
## asymmetric cuts : set the second parameter to the number
## of final state jets corresponding to the process above
FastjetFinder antikt 2 J2CUT 0.0 RJET 0.75 ETAMAX
FastjetFinder antikt 1 J1CUT 0.0 RJET 0.75 ETAMAX
}(selector)
(me){
ME_SIGNAL_GENERATOR Comix;
EVENT_GENERATION_MODE Weighted;
SCALES VAR{SCL*SCL*H_T2}
RESULT_DIRECTORY=Result/I_HTSCL_mstw08_jJ1CUT_jJ2CUT_eETAMAX_adDIPA/
}(me);
(integration){
INTEGRATOR 6;
ERROR 0.3;
PSI_ITMIN=10000;
Finish_Optimization=On;
}(integration);
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