Fodor Z, Hoelbling C, Krieg S, Lellouch L, Lippert Th, Portelli A, Sastre A, Szabo K K, Varnhorst L
Department of Physics, Wuppertal University, Gaussstr. 20, D-42119 Wuppertal, Germany.
Institute for Theoretical Physics, Eötvös University, Pázmány P. sét. 1/A, H-1117 Budapest, Hungary.
Phys Rev Lett. 2016 Aug 19;117(8):082001. doi: 10.1103/PhysRevLett.117.082001. Epub 2016 Aug 15.
In a previous Letter [Borsanyi et al., Phys. Rev. Lett. 111, 252001 (2013)] we determined the isospin mass splittings of the baryon octet from a lattice calculation based on N_{f}=2+1 QCD simulations to which QED effects have been added in a partially quenched setup. Using the same data we determine here the corrections to Dashen's theorem and the individual up and down quark masses. Our ensembles include 5 lattice spacings down to 0.054 fm, lattice sizes up to 6 fm, and average up-down quark masses all the way down to their physical value. For the parameter which quantifies violations to Dashen's theorem, we obtain ϵ=0.73(2)(5)(17), where the first error is statistical, the second is systematic, and the third is an estimate of the QED quenching error. For the light quark masses we obtain, m_{u}=2.27(6)(5)(4) and m_{d}=4.67(6)(5)(4) MeV in the modified minimal subtraction scheme at 2 GeV and the isospin breaking ratios m_{u}/m_{d}=0.485(11)(8)(14), R=38.2(1.1)(0.8)(1.4), and Q=23.4(0.4)(0.3)(0.4). Our results exclude the m_{u}=0 solution to the strong CP problem by more than 24 standard deviations.
在之前的一篇快报[博尔萨尼等人,《物理评论快报》111, 252001 (2013)]中,我们基于(N_f = 2 + 1) QCD模拟的格点计算确定了重子八重态的同位旋质量劈裂,在部分淬火设置中加入了QED效应。在此,我们使用相同的数据确定对达申定理的修正以及上夸克和下夸克的个体质量。我们的系综包括5个格点间距,小至0.054飞米,格点尺寸大至6飞米,并且平均上夸克 - 下夸克质量一直到其物理值。对于量化对达申定理违反情况的参数,我们得到(\epsilon = 0.73(2)(5)(17)),其中第一个误差是统计误差,第二个是系统误差,第三个是QED淬火误差的估计值。对于轻夸克质量,在2吉电子伏特的修正最小减除方案中,我们得到(m_u = 2.27(6)(5)(4))和(m_d = 4.67(6)(5)(4))兆电子伏特,同位旋破缺比(m_u / m_d = 0.485(11)(8)(14)),(R = 38.2(1.1)(0.8)(1.4)),以及(Q = 23.4(0.4)(0.3)(0.4))。我们的结果排除了强CP问题中(m_u = 0)的解超过24个标准差。