Abstract

Left-Right (LR) models are extensions of the Standard Model where left-right symmetry is restored at high energies, and which are strongly constrained by kaon mixing described in the framework of the $|\Delta S|=2$ effective Hamiltonian. We consider the short-distance QCD corrections to this Hamiltonian both in the Standard Model (SM) and in LR models. The leading logarithms occurring in these short-distance corrections can be resummed within a rigourous Effective Field Theory (EFT) approach integrating out heavy degrees of freedom progressively, or using an approximate simpler method of regions identifying the ranges of loop momentum generating large logarithms in the relevant two-loop diagrams. We compare the two approaches in the SM at next-to-leading order, finding a very good agreement when one scale dominates the problem, but only a fair agreement in the presence of a large logarithm at leading order. We compute the short-distance QCD corrections for LR models at next-to-leading order using the method of regions, and we compare the results with the EFT approach for the $WW'$ box with two charm quarks (together with additional diagrams forming a gauge-invariant combination), where a large logarithm occurs already at leading order. We conclude by providing next-to-leading-order estimates for $cc$, $ct$ and $tt$ boxes in LR models.

Highlights

  • A natural extension of the Standard Model (SM) is provided by Left-Right (LR) symmetric models, which explain the left-handed structure of the SM through the existence of a larger gauge group SUC(3) × SUL(2) × SUR(2) × UY (1), broken first at a scale μR of the order of the TeV followed by an electroweak symmetry breaking occurring at a scale μW [1,2,3,4,5]

  • The leading logarithms occurring in these short-distance corrections can be resummed within a rigourous Effective Field Theory (EFT) approach integrating out heavy degrees of freedom progressively, or using an approximate simpler method of regions identifying the ranges of loop momentum generating large logarithms in the relevant twoloop diagrams

  • We compute the short-distance QCD corrections for LR models at next-to-leading order using the method of regions, and we compare the results with the EFT approach for the W W ′ box with two charm quarks, where a large logarithm occurs already at leading order

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Summary

Introduction

A natural extension of the Standard Model (SM) is provided by Left-Right (LR) symmetric models, which explain the left-handed structure of the SM through the existence of a larger gauge group SUC(3) × SUL(2) × SUR(2) × UY (1), broken first at a scale μR of the order of the TeV (inducing a difference between left and right sectors) followed by an electroweak symmetry breaking occurring at a scale μW [1,2,3,4,5]. Studies in the framework of flavour physics suggest that the structure for the right-handed CKM-like matrix should be quite different from the left-handed one, far from the manifest or pseudo-manifest scenarios [21,22,23,24,25] In this setting, a important indirect constraint comes from kaon-meson mixing, favouring a mass scale for the new scalar particles of a few TeV or beyond [26,27,28,29,30]. This method of regions was applied to resum the leading logarithms both in the SM [42] and LR models [43, 44], with a much more limited amount of computation, since most of the method relies on anomalous dimensions already known

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