113 | | 1. '''set spinmode [none|madspin]'''[default:madspin] [[BR]] |
114 | | Allow to choose the spin-correlation mode of the decayed event. '''New in 2.3''' |
115 | | This mode do not include spin-correlation between production and decay, neither does he smear the invariant mass of the particle. But this mode allows to do three body decay and loop-induced decay which are not handle in other mode. |
116 | | 1. '''set use_dkevtfiles PATH''' [default:0]: [[BR]] |
117 | | Allow to use a previously generated file for the events decay. '''Not yet release''' |
| 113 | 1. '''set spinmode [none|onshell|madspin]'''[default:madspin] [[BR]] |
| 114 | a. '''madspin''' default mode with full-spin correlation and off-shell effect |
| 115 | b. '''none'''(new in 2.3) No spin-correlation between production and decay. No off-shell effects. However this mode allows to handle three-body decay and loop induced processes. Due to the lack of spin-correlation it is mainly intended for scalar particle (and in particular the Higgs). |
| 116 | c. '''onshell'' (new in 2.5.3) Keep the full spin-correlation but keep the particle exactly off-shell. |
| 117 | Supports three-body decay but not loop-induced processes (in either production or decay). Intended for particle with small width without any two body decay. |
| 118 | This mode requires f2py program to be available on your machine. |
| 119 | 1. '''set run_card PATH''': [[BR]] |
| 120 | Only for mode "none" or "onshell". This defines the cut to apply to the 1>N sample. Those cut will be applied in the frame where the particle is at rest. Transverse cut are meaningless in that card and should be kept to zero. |