Lattice QCD at the physical point: Light quark masses

被引:100
|
作者
Durr, S. [1 ,3 ]
Fodor, Z. [1 ,3 ,4 ]
Hoelbling, C. [1 ,2 ,5 ,6 ,7 ,8 ]
Katz, S. D. [1 ,4 ]
Krieg, S. [1 ,3 ]
Kurth, T. [1 ]
Lellouch, L. [2 ,5 ,6 ,7 ,8 ]
Lippert, T. [1 ,3 ]
Szabo, K. K. [1 ]
Vulvert, G. [2 ,5 ,6 ,7 ,8 ]
机构
[1] Berg Univ Wuppertal, D-42119 Wuppertal, Germany
[2] CNRS, UMR 6207, Ctr Phys Theor, CPT,Res Unit, F-13288 Marseille, France
[3] Forschungszentrum Julich, Julich Supercomp Ctr, D-52425 Julich, Germany
[4] Eotvos Lorand Univ, Inst Theoret Phys, H-1117 Budapest, Hungary
[5] Univ Aix Marseille 1, Ctr Phys Theor, F-13288 Marseille, France
[6] Univ Aix Marseille 2, Ctr Phys Theor, F-13288 Marseille, France
[7] Univ Sud Toulon Var, Ctr Phys Theor, F-13288 Marseille, France
[8] FRUMAM, Ctr Phys Theor, F-13288 Marseille, France
关键词
Quark masses; Lattice QCD; MONTE-CARLO; RENORMALIZATION; ALGORITHM; FIELD;
D O I
10.1016/j.physletb.2011.05.053
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Ordinary matter is described by six fundamental parameters: three couplings (gravitational, electromagnetic and strong) and three masses: the electron's (m(e)) and those of the up (m(u)) and down (m(d)) quarks. An additional mass enters through quantum fluctuations: the strange quark mass (m(s)). The three couplings and m(e) are known with an accuracy of better than a few per mil. Despite their importance, m(u), m(d) (their average m(ud)) and m(s) are far less accurately known. Here we determine them with a precision below 2% by performing ab initio lattice quantum chromodynamics (QCD) calculations, in which all systematics are controlled. We use pion and quark masses down to (and even below) their physical values, lattice sizes of up to 6 fm, and five lattice spacings to extrapolate to continuum spacetime. All necessary renormalizations are performed nonperturbatively. (C) 2011 Elsevier B.V. All rights reserved.
引用
收藏
页码:265 / 268
页数:4
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