293 | | || || isr || -> Pierre || |
| 293 | || || isr || isr=0: no correction, except if all ME final-state particles are reconstructed |
| 294 | in the final state: in that case, the pT of the reconstructed particles |
| 295 | may not be balanced and one cannot ignore the effects from ISR. The |
| 296 | phase-space integration is done under the assumption that, point-by-point |
| 297 | in the phase-space, the parton-level final state has a pT balancing |
| 298 | pT(ISR), with pT(ISR) set to minus the transverse momentum of the |
| 299 | reconstructed objects in the LHCO file. |
| 300 | isr=1: point by point in the phase-space, the parton-level final state has a pT |
| 301 | balancing pT(ISR), with pT(ISR) set to the experimental value read from |
| 302 | the lhco file [as -pT(visible)-pT(missing)] |
| 303 | isr=2: same as isr=1, except that the value of the weight is translated into |
| 304 | a frame where the hard system has no pT. |
| 305 | isr=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. || |