Abstract

We present a package for FeynRules which derives the Feynman rules for the Standard Model Effective Field Theory up to dimension-six using the background field method for gauge fixing. The package includes operators which shift the kinetic and mass terms of the Lagrangian up to dimension-eight and including dimension-six squared effects consistently. To the best of the author’s knowledge this is the first publicly available package to include dimension-six squared effects consistently. The package is validated in a partner publication by analyzing the Ward Identities at dimension-six and one-loop order. We also extend the partner work in this article by including the dimension-six squared effects further demonstrating the consistency of their implementation. In doing so we find that failure to consistently include field shifts to dimension-six squared causes a breakdown in the Ward identities implying concerns about many calculations in the literature which do not properly incorporate these effects.The FeynRules files, as well as Mathematica notebooks performing the relevant calculations, can be downloaded from the FeynRules website and are included as supplementary material to this publication.

Highlights

  • The FeynRules files, as well as Mathematica notebooks performing the relevant calculations, can be downloaded from the FeynRules website and are included as supplementary material to this publication

  • We present a package for FeynRules which derives the Feynman rules for the Standard Model Effective Field Theory up to dimension-six using the background field method for gauge fixing

  • The SMEFT is formed of the SM plus a tower of operators of dimension n ≥ 5, each suppressed by the new physics scale to the power n − 4:

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Summary

Definitions and implementation of the Lagrangian

We follow the geometric formulation of the SMEFT presented in [61,62,63,64]. At this time the only dimension-eight operators implemented are of classes two, three, and four. To outline the implementation of the SMEFT with background gauge fixing we first define necessary conventions, define the fields and metrics, and the full SMEFT Lagrangian. This is the order in which the FeynRules files are organized. The following is written in standard particle physics notation, but is meant to demonstrate the way in which the Lagrangian is defined from the ground up in the language of Mathematica and Feynrules

Conventions
Fields and metrics
The bosonic Lagrangian
Implementation of the fermionic operators
Ward identities
Verification of Ward Identities for dimension-six squared contributions
Longitudinal photons and Zγ mixing
Charged Ward identities
Neutral Ward identities involving Zand χ
Conclusions
A Barred quantities
B SMEFT operators used in this work
C Dimension-six squared contributions to the amplitudes
D Speeding up the tools
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