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Lattice computation of the electromagnetic contributions to kaon and pion masses

Authors :
Steven Gottlieb
R. S. Van De Water
U. M. Heller
A. Torok
Jack Laiho
E. D. Freeland
C. DeTar
D. Toussaint
James C. Osborn
S. Basak
Ludmila Levkova
Alexei Bazavov
Robert L. Sugar
Claude Bernard
Ran Zhou
Source :
Physical Review
Publication Year :
2018
Publisher :
arXiv, 2018.

Abstract

We present a lattice calculation of the electromagnetic (EM) effects on the masses of light pseudoscalar mesons. The simulations employ 2+1 dynamical flavors of asqtad QCD quarks, and quenched photons. Lattice spacings vary from $\approx 0.12$ fm to $\approx 0.045$ fm. We compute the quantity $\epsilon$, which parameterizes the corrections to Dashen's theorem for the $K^+$-$K^0$ EM mass splitting, as well as $\epsilon_{K^0}$, which parameterizes the EM contribution to the mass of the $K^0$ itself. An extension of the nonperturbative EM renormalization scheme introduced by the BMW group is used in separating EM effects from isospin-violating quark mass effects. We correct for leading finite-volume effects in our realization of lattice electrodynamics in chiral perturbation theory, and remaining finite-volume errors are relatively small. While electroquenched effects are under control for $\epsilon$, they are estimated only qualitatively for $\epsilon_{K^0}$, and constitute one of the largest sources of uncertainty for that quantity. We find $\epsilon = 0.78(1)_{\rm stat}({}^{+\phantom{1}8}_{-11})_{\rm syst}$ and $\epsilon_{K^0}=0.035(3)_{\rm stat}(20)_{\rm syst}$. We then use these results on 2+1+1 flavor pure QCD HISQ ensembles and find $m_u/m_d = 0.4529(48)_{\rm stat}( {}_{-\phantom{1}67}^{+150})_{\rm syst}$.<br />Comment: Version published in Phys. Rev. D. Compared to v1, more discussion of nonperturbative EM renormalization scheme, of statistical errors (with 3 added figures), and of choice QED_{TL} in finite volume. 87 pages, 35 figures

Details

Database :
OpenAIRE
Journal :
Physical Review
Accession number :
edsair.doi.dedup.....e3b3ecf2ecd744d7be621d9be27d5fe0
Full Text :
https://doi.org/10.48550/arxiv.1807.05556