Changes between Version 3 and Version 4 of SMWeinberg


Ignore:
Timestamp:
Dec 15, 2020, 9:04:15 PM (4 years ago)
Author:
Richard Ruiz
Comment:

Synopsis edits

Legend:

Unmodified
Added
Removed
Modified

  • SMWeinberg

    v3 v4  
    2121
    2222=== Synopsis ===
    23 This set of UFO libraries enables one to simulate the Weinberg operator in high-energy scattering and resonant decay processes up to next-to-leading order in QCD.
     23The  {{{SMWeinberg}}} UFO libraries allows one to simulate the Weinberg operator in high-energy scattering and resonant decay processes up to next-to-leading order in QCD when used in conjunction with event generators, like {{{MadGraph5_aMC@NLO}}}.
    2424
    2525
    2626=== Full Description ===
    27 This model file is constructed in the context of the Standard Model (SM) Effective Field Theory (SM EFT), and extend the SM Lagrangian by gauge-invariant operators up to dimension {{{$d=5$}}}. In the canonical representation the Lagrangian is given by
     27This model file works in the context of the Standard Model (SM) Effective Field Theory (SM EFT), where the SM Lagrangian is extended by gauge-invariant operators up to dimension {{{$d=5$}}}. In the canonical representation the Lagrangian is given by
    2828{{{
    2929#!latex
    … …  
    4141}}}
    4242where
    43 {{{$\Lambda$}}} is the EFT cutoff scale,
    44 {{{$C^{\ell\ell'}_5$}}} is the flavor-dependent Wilson coefficient in the flavor basis,
     43{{{Lambda}}} is the EFT cutoff scale [GeV],
     44{{{#!latex
     45$C^{\ell\ell'}_5$
     46}}}
     47{{{#!latex $C^{\ell\ell'}_5$}}}
     48 is the flavor-dependent Wilson coefficient in the flavor basis,
    4549and the the SU(2)-invariant product {{{$\Phi\cdot \overline{L^c} = \Phi^i\varepsilon_{ij} \overline{L^{cj}}$}}} is fixed by {{{$\varepsilon_{12}=1$}}}.
    4650