Abstract

The interpretation of nuclear electric dipole moment (EDM) experiments is clouded by large theoretical uncertainties associated with nonperturbative matrix elements. In various beyond-the-Standard Model scenarios nuclear and diamagnetic atomic EDMs are expected to be dominated by CP-violating pion-nucleon interactions that arise from quark chromo-electric dipole moments. The corresponding CP-violating pion-nucleon coupling strengths are, however, poorly known. In this work we propose a strategy to calculate these couplings by using spectroscopic lattice QCD techniques. Instead of directly calculating the pion-nucleon coupling constants, a challenging task, we use chiral symmetry relations that link the pion-nucleon couplings to nucleon sigma terms and mass splittings that are significantly easier to calculate. In this work, we show that these relations are reliable up to next-to-next-to-leading order in the chiral expansion in both SU(2) and SU(3) chiral perturbation theory. We conclude with a brief discussion about practical details regarding the required lattice QCD calculations and the phenomenological impact of an improved understanding of CP-violating matrix elements.

Highlights

  • The search for phenomena that can explain the apparent shortcomings of the Standard Model (SM) takes place over a large range of energy scales

  • The main result of this work is the derivation of reliable relations that can be used to simplify lattice calculations of the CPV pion-nucleon vertices that originate in the up, down, and strange qCEDMs

  • By using chiral symmetry arguments the required three-point functions can be linked to spectroscopic two-point functions which are more suitable for lattice calculations

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Summary

Introduction

The search for phenomena that can explain the apparent shortcomings of the Standard Model (SM) takes place over a large range of energy scales. An outstanding challenge is the calculation of the nucleon EDMs in terms of CP-violating (CPV) sources in the SM (the QCD θterm) and beyond The latter can be categorized in an effective field theory (EFT) picture, assuming the new physics is heavy, where the most relevant higher-dimensional operators are the quark electric dipole moments (qEDMs), chromo-electric dipole moments (qCEDMs), the Weinberg three-gluon operator, and several four-quark operators. In this case the CPV pion-nucleon couplings can be linked to hadron masses and mass splittings induced by CP-conserving quark chromo-magnetic dipole moments (qCMDMs) [31, 19, 32] While these matrix elements are not known, they are very suitable for lattice QCD (LQCD) calculations as they can be performed with simple spectroscopic methods.

CP violation at the quark-gluon level
Findings
Discussion
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