Abstract

We demonstrate that the leading and next-to-leading finite-volume effects in the evaluation of leptonic decay widths of pseudoscalar mesons at $O(\ensuremath{\alpha})$ are universal; i.e. they are independent of the structure of the meson. This is analogous to a similar result for the spectrum but with some fundamental differences, most notably the presence of infrared divergences in decay amplitudes. The leading nonuniversal, structure-dependent terms are of $O(1/{L}^{2})$ [compared to the $O(1/{L}^{3})$ leading nonuniversal corrections in the spectrum]. We calculate the universal finite-volume effects, which requires an extension of previously developed techniques to include a dependence on an external three-momentum (in our case, the momentum of the final-state lepton). The result can be included in the strategy proposed in Ref. [N. Carrasco et al.,Phys. Rev. D 91, 074506 (2015).] for using lattice simulations to compute the decay widths at $O(\ensuremath{\alpha})$, with the remaining finite-volume effects starting at order $O(1/{L}^{2})$. The methods developed in this paper can be generalized to other decay processes, most notably to semileptonic decays, and hence open the possibility of a new era in precision flavor physics.

Highlights

  • We demonstrate that the leading and next-to-leading finite-volume effects in the evaluation of leptonic decay widths of pseudoscalar mesons at OðαÞ are universal; i.e. they are independent of the structure of the meson

  • D 91, 074506 (2015).] for using lattice simulations to compute the decay widths at OðαÞ, with the remaining finite-volume effects starting at order Oð1=L2Þ

  • For many physical quantities relevant for studies of flavor physics, recent improvements in lattice computations have led to such a precision that electromagnetic effects and isospin-breaking contributions cannot be neglected anymore

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Summary

INTRODUCTION

For many physical quantities relevant for studies of flavor physics, recent improvements in lattice computations have led to such a precision that electromagnetic effects and isospin-breaking contributions cannot be neglected anymore (see e.g. Ref. [1] and references therein). In this paper we show that the 1=L finite-volume (FV) corrections are universal; that is, they are independent of the structure of the pseudoscalar meson and cancel in the difference Γ0ðLÞ − Γp0tðLÞ. We do this in the Appendix using the QED skeleton expansion, in which the meson propagator and the vertices to which the photon couples are defined in terms of QCD correlation functions and inserted into one-loop diagrams. Able to demonstrate explicitly that the leading and next-toleading FV effects are universal This allows us to calculate Γp0tðLÞ in perturbation theory with a pointlike pseudoscalar meson up to and including the 1=L corrections and present the result expanded in inverse powers of L. There is a single appendix in which the universality of the leading and next-to-leading FV effects is proved using the skeleton expansion

THE DECAY RATE WITHOUT ELECTROMAGNETIC CORRECTIONS
ULTRAVIOLET DIVERGENCES AND THE W-RENORMALIZATION SCHEME
INFRARED DIVERGENCES AND FINITE-VOLUME CORRECTIONS
UNIVERSALITY OF THE FINITE-VOLUME CORRECTIONS TO MASSES AND DECAY AMPLITUDES
FV corrections for the self-energy diagram
Universality of the FV corrections to the remaining diagrams
The rainbow diagrams
Wave-function renormalization of the pseudoscalar meson and charged lepton
MASTER INTEGRALS IN A FINITE VOLUME
Calculation of S3
L3λ3 þ imP 48π2El ð75Þ
Calculation of S1
Calculation of S2
Calculation of S4 and S5
The auxiliary constants Kij
Elements of the skeleton expansion
The Ward identities at small photon momenta
Universality of leading and next-to-leading FV effects
Findings
Summary

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