Abstract

We present an $\mathcal{O}(\alpha)$ Standard Model calculation of the inner radiative corrections to Gamow-Teller $\beta$ decays. We find that \textit{a priori} contributions arise from the photonic vertex correction and $\gamma W$ box diagram. Upon evaluation most elastic contributions vanish due to crossing symmetry or cancellation between isoscalar and isovector photonic contributions, leaving only the polarized parity-odd contribution, i.e., the Gamow-Teller equivalent of the well-known axial $\gamma W$ box contribution for Fermi decays. We show that weak magnetism contributes significantly to the Born amplitude, and consider additional hadronic contributions at low energy using a holomorphic continuation of the polarized Bjorken sum rule constrained by experimental data. We perform the same procedure for the Fermi inner radiative correction through a combination of the running of Bjorken and Gross-Llewellyn Smith sum rules. We discuss heavy flavor, higher-twist, and target mass corrections and find a significant increase at low momentum from the latter. We find $\Delta_R^A = 0.02532(22)$ and $\Delta_R^V = 0.02473(27)$ for axial and vector inner radiative corrections, respectively, resulting in $\Delta_R^A-\Delta_R^V=0.60(5) \times 10^{-3}$, which allows us to extract $g_A^0$ for the first time to our knowledge. We discuss consequences for comparing experimental data to lattice calculations in beyond Standard Model fits. Further, we show how some traditional $\beta$ decay calculations contain part of this effect but fail to account for cancellations in the full $\mathcal{O}(\alpha)$result. Finally, we correct for a double-counting instance in the isospin $T=1/2$ mirror decay extraction of $|V_{ud}|$, the up-down matrix element of the Cabibbo-Kobayashi-Maskawa matrix, resolving a long-standing tension and leading to increased precision.

Highlights

  • Precision studies of neutron and nuclear β decays were of paramount importance in the construction of the Standard Model and provide stringent constraints on TeV-scale beyond Standard Model (BSM) physics [1,2,3,4,5]

  • VII A we show that this cancellation is not taken into account in the traditional β decay calculations leading to important discrepancies

  • Because the Standard Model is a local theory, the commutator is proportional to δð3ÞðxÞ, and it is clear from Eq (70) that the asymptotic contribution of Dμ vanishes

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Summary

INTRODUCTION

Precision studies of neutron and nuclear β decays were of paramount importance in the construction of the Standard Model and provide stringent constraints on TeV-scale beyond Standard Model (BSM) physics [1,2,3,4,5]. ; ð1Þ where τn is the neutron lifetime, GF ≈ 10−5 GeV−2 is the Fermi coupling constant, me is the electron mass, λ ≡ gA=gV is the ratio of axial and vector coupling constants, fV=A are their respective phase space integrals, and RC represents electroweak radiative corrections [10]. The latter is traditionally written as 1 þ RC 1⁄4 1 þ δoutðEÞ þ ΔVR; ð2Þ where δoutðEÞ is an energy dependent, but nuclear structure independent correction, and ΔVR is the so-called inner. VI and VII, treating the comparison to LQCD and consistency errors in traditional β decay formalisms and mirror jVudj extraction, respectively

OVERVIEW OF STANDARD MODEL INPUT
Sketch of the ingredients
Common tools
Currents and commutation relations
G-parity and first-class currents
ELECTROWEAK VERTEX CORRECTION
Setting stage I
Three-point function evaluation
ELECTROWEAK BOX DIAGRAMS
Setting stage II The γW box matrix element is typically written as
Axial divergence
Parity-odd amplitude
Born contribution
Deep inelastic scattering
Nonperturbative contributions
Target mass corrections
Numerical results
Nucleons
THE LATTICE AND RIGHT-HANDED CURRENTS
CONSISTENCY ISSUES IN TRADITIONAL β DECAY THEORY INPUT
Missing cancellation
VIII. CONCLUSIONS
Axial vector transition
Findings
Vector transition

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