{"title":"A Procedure g5anchor to Anchor $γ_5$ in Feynman Diagrams for the Standard Model","authors":"Long Chen","doi":"arxiv-2409.08099","DOIUrl":null,"url":null,"abstract":"We present a procedure g5anchor to anchor $\\gamma_5$ in the definition of a\nDirac trace with $\\gamma_5$ in Dimensional Regularization (DR) in Feynman\ndiagrams for the Standard Model, based on a recent revision of the works by\nKreimer, Gottlieb and Donohue. For each closed fermion chain with an odd number\nof primitive (i.e.~not-yet-clearly-defined) $\\gamma_5$ in a given Feynman\ndiagram, g5anchor returns a definite set of anchor points for $\\gamma_5$, in\nterms of pairs of ordered fermion propagators; at each of these $\\gamma_5$\nanchor points a fixed expression in terms of the Levi-Civita tensor and\nelementary Dirac matrices will be inserted together with a sign determined by\nanticommutatively shifting all $\\gamma_5$ from their original places (dictated\nby the Feynman rules) to this anchor point. The defining expressions for the\ncyclic $\\gamma_5$-odd Dirac traces in DR associated with closed fermion chains\nin amplitudes, or more generally squared amplitudes, thus follow from this\nprocedure, where the Levi-Civita tensors are not necessarily treated strictly\nin 4-dimensions. We propose utilizing this definition in practical perturbative\ncalculations in the Standard Model at least to three-loop orders with the\ncurrent implementation, and maybe to higher loop orders in absence of Yukawa\ncouplings to Higgs fields. Certain limitations and modifications of the KKS\nand/or the Kreimer scheme are addressed.","PeriodicalId":501339,"journal":{"name":"arXiv - PHYS - High Energy Physics - Theory","volume":"384 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.08099","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
We present a procedure g5anchor to anchor $\gamma_5$ in the definition of a
Dirac trace with $\gamma_5$ in Dimensional Regularization (DR) in Feynman
diagrams for the Standard Model, based on a recent revision of the works by
Kreimer, Gottlieb and Donohue. For each closed fermion chain with an odd number
of primitive (i.e.~not-yet-clearly-defined) $\gamma_5$ in a given Feynman
diagram, g5anchor returns a definite set of anchor points for $\gamma_5$, in
terms of pairs of ordered fermion propagators; at each of these $\gamma_5$
anchor points a fixed expression in terms of the Levi-Civita tensor and
elementary Dirac matrices will be inserted together with a sign determined by
anticommutatively shifting all $\gamma_5$ from their original places (dictated
by the Feynman rules) to this anchor point. The defining expressions for the
cyclic $\gamma_5$-odd Dirac traces in DR associated with closed fermion chains
in amplitudes, or more generally squared amplitudes, thus follow from this
procedure, where the Levi-Civita tensors are not necessarily treated strictly
in 4-dimensions. We propose utilizing this definition in practical perturbative
calculations in the Standard Model at least to three-loop orders with the
current implementation, and maybe to higher loop orders in absence of Yukawa
couplings to Higgs fields. Certain limitations and modifications of the KKS
and/or the Kreimer scheme are addressed.