text: DipoleMIOperator implements the I() insertion operator for the massive case. DipoleMIOperator does only apply for expanded con- vention and also not for dimensional reduction. More...
  #include <DipoleMIOperator.h>
  DipoleMIOperator implements the I() insertion operator for the massive case. DipoleMIOperator does only apply for expanded con- vention and also not for dimensional reduction.
  Definition at line 33 of file DipoleMI Matchbox convention is =.
  Often however, is defined in the literature as =2*. Be aware of consistent usage! In the massive case (see hep-ph/0011222v3): = 11/3*C_A - 4/3*T_R*(N_f+N_F) with T_R=1/2, N_f the number of light flavours ,and N_F the number of heavy flavours, which originate in the splittings g->qqbar or g->QQbar. In our conventions, however: = 11/6*C_A - 2/3*T_R*(N_f+N_F) The "massive" applies as soon as we define massive flavours in the jet particle group. Be aware that some OLP might generically(!) use something like N_f=5 and N_F=1 in their definition of !
  Definition at line 208 of file DipoleMIOperator.h.