33 | | Unlike prescribed by the LHC TOP WG, the top quark chromomagnetic-dipole operator coefficient {{{ctG}}} is normalised with a factor of the strong coupling, g,,S,,. |
34 | | This normalisation factor temporarily ensures compatibility with the 2.X.X series of MadGraph5_aMC@NLO but may be dropped in the future. |
| 33 | Unlike prescribed by the LHC TOP WG, the top quark chromomagnetic-dipole operator (with coefficient {{{ctG}}}) is normalised with a factor of the strong coupling, so that {{{ctG_LHCTOPWG = gS ctG_SMEFTatNLO}}}. |
| 34 | This may however change in the future. |
| 35 | In both 2.X.X and 3.X.X series of MadGraph5_aMC@NLO, already at LO, such a normalization is notably required for jet merging, systematics computation, and the default dynamical scale. |
| 36 | It is also required for NLO computations in the 2.X.X series. |