Changes between Version 2 and Version 3 of TOPMassMeasurmentExample


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Timestamp:
Feb 4, 2014, 11:56:07 AM (10 years ago)
Author:
Pierre
Comment:

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  • TOPMassMeasurmentExample

    v2 v3  
    291291       ||        || log_level        || Indicates how much information as to be kept from the run. The two physical level are '''weights''' and '''permutations'''. '''full'' will return the log associated to each run' ||
    292292       ||        || nwa              || The integral on the invariant mass of particles with width below this threshold will be done in Narrow-width approximation (i.e. the mass of that particles will be kept fixed during the computation and the integral on the invariant mass assumed to correspond to the Breit-Wigner Shape. The default correspond to use this approximation ONLY for the Higgs. ||
    293        ||        || isr              || -> Pierre ||
     293       ||        || isr              ||  isr=0: no correction, except if all ME final-state particles are reconstructed
     294in the final state: in that case, the pT of the reconstructed particles
     295may not be balanced and one cannot ignore the effects from ISR. The
     296phase-space integration is done under the assumption that, point-by-point
     297in the phase-space, the parton-level final state has a pT balancing
     298pT(ISR), with pT(ISR) set to minus the transverse momentum of the
     299reconstructed objects in the LHCO file.
     300isr=1: point by point in the phase-space,  the parton-level final state has a pT
     301balancing pT(ISR), with pT(ISR) set to the experimental value read from
     302the lhco file [as -pT(visible)-pT(missing)]
     303isr=2: same as isr=1, except that the value of the weight is translated into
     304a frame where the hard system has no pT.
     305isr=3: only relevant if all final state ME particle are reconstructed.
     306   pT of ISR is assumed to be unconstrained (can be anything)
     307   -> the dimension of the phase-space integration is augmented by 2,
     308   since we also integrate over the pT of the parton-level final state.  ||
    294309       ||        || inputfile        || The path of the input_file in lhco (or lhco.gz) to use to get the events.||
    295310       ||        ||                  ||           ||