Kπ scattering and the K* decay width from lattice QCD

被引:54
作者
Prelovsek, Sasa [1 ,2 ]
Leskovec, Luka [2 ]
Lang, C. B. [3 ]
Mohler, Daniel [4 ]
机构
[1] Univ Ljubljana, Fac Math & Phys, Ljubljana 1000, Slovenia
[2] Jozef Stefan Inst, Ljubljana 1000, Slovenia
[3] Graz Univ, Inst Phys, A-8010 Graz, Austria
[4] Fermilab Natl Accelerator Lab, Batavia, IL 60510 USA
来源
PHYSICAL REVIEW D | 2013年 / 88卷 / 05期
基金
美国能源部;
关键词
QUANTUM-FIELD THEORIES; FINITE-VOLUME; STATES; RESONANCE; MATRIX; MESON;
D O I
10.1103/PhysRevD.88.054508
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
K* mesons and in particular the K*(892) were frequently addressed in lattice simulations, but always while ignoring that the K*(892) decays strongly. We present an exploratory extraction of the masses and widths for the K* resonances by simulating K pi scattering in p waves with I 1/2 on the lattice. The K pi system with total momenta P = 2 pi/Le(z), 2 pi/L(e(x) + e(y)), and 0, that allows the extraction of phase shifts at several values of K pi relative momenta, is studied. A Breit-Wigner fit of the phase renders a K*(892) resonance mass m(lat) = 891 +/- 14 MeV and the K*(892) -> K pi coupling g(lat) = 5.7 +/- 1.6 compared to the experimental values m(exp) approximate to 892 MeV and g(exp) = 5.72 +/- 0: 06, where g parametrizes the K* -> K pi width. When extracting the phase shift around the K*(1410) and K-2*(1430) resonances, we take into account the mixing of p waves with d waves and assume that the scattering is elastic in our simulation. This gives us an estimate of the K*(1410) resonance mass m(lat) = 1.33 +/- 0.02 GeV compared to m(exp) = 1.414 -> 0.0015 GeV, assuming the experimental K*(1410)-> K pi coupling. We contrast the resonant I = 1/2 channel with the repulsive nonresonant I = 3/2 channel, where the phase is found to be negative and small, in agreement with experiment.
引用
收藏
页数:12
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