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| 1 | +Beams:eCM 13000. # GeV |
| 2 | +### processes |
| 3 | +Next:numberShowLHA = 1 |
| 4 | +Next:numberShowInfo = 1 |
| 5 | +Next:numberShowProcess = 1 |
| 6 | +Next:numberShowEvent = 1 |
| 7 | +Main:timesAllowErrors = 10 |
| 8 | +! Read LHE file from POWHEG |
| 9 | +Beams:frameType = 4 |
| 10 | +Beams:LHEF = powheg.lhe |
| 11 | + |
| 12 | +! Number of outgoing particles of POWHEG Born level process |
| 13 | +! (i.e. not counting additional POWHEG radiation) |
| 14 | +POWHEG:nFinal = 2 |
| 15 | + |
| 16 | +! How vetoing is performed: |
| 17 | +! 0 - No vetoing is performed (userhooks are not loaded) |
| 18 | +! 1 - Showers are started at the kinematical limit. |
| 19 | +! Emissions are vetoed if pTemt > pThard. |
| 20 | +! See also POWHEG:vetoCount below |
| 21 | +POWHEG:veto = 1 |
| 22 | + |
| 23 | +! After 'vetoCount' accepted emissions in a row, no more emissions |
| 24 | +! are checked. 'vetoCount = 0' means that no emissions are checked. |
| 25 | +! Use a very large value, e.g. 10000, to have all emissions checked. |
| 26 | +POWHEG:vetoCount = 3 |
| 27 | + |
| 28 | +! Selection of pThard (note, for events where there is no |
| 29 | +! radiation, pThard is always set to be SCALUP): |
| 30 | +! 0 - pThard = SCALUP (of the LHA/LHEF standard) |
| 31 | +! 1 - the pT of the POWHEG emission is tested against all other |
| 32 | +! incoming and outgoing partons, with the minimal value chosen |
| 33 | +! 2 - the pT of all final-state partons is tested against all other |
| 34 | +! incoming and outgoing partons, with the minimal value chosen |
| 35 | +POWHEG:pThard = 2 |
| 36 | + |
| 37 | +! Selection of pTemt: |
| 38 | +! 0 - pTemt is pT of the emitted parton w.r.t. radiating parton |
| 39 | +! 1 - pT of the emission is checked against all incoming and outgoing |
| 40 | +! partons. pTemt is set to the minimum of these values |
| 41 | +! 2 - the pT of all final-state partons is tested against all other |
| 42 | +! incoming and outgoing partons, with the minimal value chosen |
| 43 | +! WARNING: the choice here can give significant variations in the final |
| 44 | +! distributions, notably in the tail to large pT values. |
| 45 | +POWHEG:pTemt = 0 |
| 46 | + |
| 47 | +! Selection of emitted parton for FSR |
| 48 | +! 0 - Pythia definition of emitted |
| 49 | +! 1 - Pythia definition of radiator |
| 50 | +! 2 - Random selection of emitted or radiator |
| 51 | +! 3 - Both are emitted and radiator are tried |
| 52 | +POWHEG:emitted = 0 |
| 53 | + |
| 54 | +! pT definitions |
| 55 | +! 0 - POWHEG ISR pT definition is used for both ISR and FSR |
| 56 | +! 1 - POWHEG ISR pT and FSR d_ij definitions |
| 57 | +! 2 - Pythia definitions |
| 58 | +POWHEG:pTdef = 1 |
| 59 | + |
| 60 | +! MPI vetoing |
| 61 | +! 0 - No MPI vetoing is done |
| 62 | +! 1 - When there is no radiation, MPIs with a scale above pT_1 are vetoed, |
| 63 | +! else MPIs with a scale above (pT_1 + pT_2 + pT_3) / 2 are vetoed |
| 64 | +POWHEG:MPIveto = 0 |
| 65 | +! Note that POWHEG:MPIveto = 1 should be combined with |
| 66 | +! MultipartonInteractions:pTmaxMatch = 2 |
| 67 | +! which here is taken care of in main31.cc. |
| 68 | + |
| 69 | +! QED vetoing |
| 70 | +! 0 - No QED vetoing is done for pTemt > 0. |
| 71 | +! 1 - QED vetoing is done for pTemt > 0. |
| 72 | +! 2 - QED vetoing is done for pTemt > 0. If a photon is found |
| 73 | +! with pT>pThard from the Born level process, the event is accepted |
| 74 | +! and no further veto of this event is allowed (for any pTemt). |
| 75 | +POWHEG:QEDveto = 2 |
| 76 | + |
| 77 | +### decays |
| 78 | +ParticleDecays:limitTau0 on |
| 79 | +ParticleDecays:tau0Max 10. |
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