Abstract

In this work, we consider expressions for the masses and decay constants of the pseudoscalar mesons in $SU(3)$ chiral perturbation theory. These involve sunset diagrams and their derivatives evaluated at $p^2=m_P^2$ ($P=\pi, K, \eta$). Recalling that there are three mass scales in this theory, $m_\pi$, $m_K$ and $m_\eta$, there are instances when the finite part of the sunset diagrams do not admit an expression in terms of elementary functions, and have therefore been evaluated numerically in the past. In a recent publication, an expansion in the external momentum was performed to obtain approximate analytic expressions for $m_\pi$ and $F_\pi$, the pion mass and decay constant. We provide fully analytic exact expressions for $m_K$ and $m_\eta$, the kaon and eta masses, and $F_K$ and $F_\eta$, the kaon and eta decay constants. These expressions, calculated using Mellin-Barnes methods, are in the form of double series in terms of two mass ratios. A numerical analysis of the results to evaluate the relative size of contributions coming from loops, chiral logarithms as well as phenomenological low-energy constants is presented. We also present a set of approximate analytic expressions for $m_K$, $F_K$, $m_\eta$ and $F_\eta$ that facilitate comparisons with lattice results. Finally, we show how exact analytic expressions for $m_\pi$ and $F_\pi$ may be obtained, the latter having been used in conjunction with the results for $F_K$ to produce a recently published analytic representation of $F_K/F_\pi$.

Highlights

  • The important ratio FK=Fπ was evaluated in a scheme that allows for the derivation of compact analytic approximations in two loop chiral perturbation theory (ChPT) [1], based on the Mellin-Barnes (MB) approach detailed in [2]

  • To get the simplified expressions, we use a simple criterion: for a given set of numerical values of the pseudoscalar masses, in each of the different contributions of Eqs. (B3)–(B9) we keep terms that are bigger than 10−p, p ≥ 1 being incremented until we achieve the precision goal given by the numerical difference between the corresponding partial sum and the sum of the first hundreds4 of terms, the latter being defined as the “exact” value

  • SUð3Þ ChPT is the effective theory of the strong interactions at low energies and describes the pseudoscalar octet degrees of freedom and their interactions

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Summary

Introduction

The important ratio FK=Fπ was evaluated in a scheme that allows for the derivation of compact analytic approximations in two loop chiral perturbation theory (ChPT) [1], based on the Mellin-Barnes (MB) approach detailed in [2]. A different scheme was employed to obtain analytic approximations of mπ and Fπ in SUð3Þ ChPT at two loops [3]. Recall that ChPT is an effective field theory for the pseudoscalar octet degrees of freedom, namely the pions, kaons and eta. The SUð2Þ theory with just the pion degrees of freedom was worked out in [6], while the significantly more complicated SUð3Þ theory has been described in [7].

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