pith. machine review for the scientific record. sign in

arxiv: 1303.3156 · v2 · submitted 2013-03-13 · ✦ hep-ph · nucl-th

Recognition: unknown

Renormalization Group Running of Dimension-Six Sources of Parity and Time-Reversal Violation

Authors on Pith no claims yet
classification ✦ hep-ph nucl-th
keywords operatorsscaledimension-sixbeyondcorrectionselectroweakhadronichigh-energy
0
0 comments X
read the original abstract

We perform a systematic study of flavor-diagonal parity- and time-reversal-violating operators of dimension six which could arise from physics beyond the SM. We begin at the unknown high-energy scale where these operators originate. At this scale the operators are constrained by gauge invariance which has important consequences for the form of effective operators at lower energies. In particular for the four-quark operators. We calculate one-loop QCD and, when necessary, electroweak corrections to the operators and evolve them down to the electroweak scale and subsequently to hadronic scales. We find that for most operators QCD corrections are not particularly significant. We derive a set of operators at low energy which is expected to dominate hadronic and nuclear EDMs due to physics beyond the SM and obtain quantitative relations between these operators and the original dimension-six operators at the high-energy scale. We use the limit on the neutron EDM to set bounds on the dimension-six operators.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Quantumness of top quark pairs produced at LHC within SMEFT framework

    hep-ph 2026-05 unverdicted novelty 6.0

    Quantum information observables in LHC top quark pair production are modified by SMEFT dimension-6 operators in ways that depend on their CP properties, offering a complementary probe beyond standard observables.