BK with two flavors of dynamical overlap fermions

被引:17
|
作者
Aoki, S. [1 ,2 ]
Fukaya, H. [3 ]
Hashimoto, S. [4 ,5 ]
Noaki, J. [4 ]
Kaneko, T. [4 ,5 ]
Matsufuru, H. [4 ]
Onogi, T. [6 ]
Yamada, N. [4 ,5 ]
机构
[1] Univ Tsukuba, Grad Sch Pure & Appl Sci, Tsukuba, Ibaraki 3058571, Japan
[2] Assoc Univ Inc, Brookhaven Natl Lab, Riken BNL Res Ctr, Upton, NY 11973 USA
[3] Niels Bohr Int Acad, Niels Bohr Inst, DK-2100 Copenhagen O, Denmark
[4] High Energy Accelerator Res Org KEK, Tsukuba, Ibaraki 3050801, Japan
[5] Grad Univ Adv Studies Sokendai, Sch High Energy Accelerator Sci, Tsukuba, Ibaraki 3050801, Japan
[6] Kyoto Univ, Yukawa Inst Theoret Phys, Kyoto 6068502, Japan
来源
PHYSICAL REVIEW D | 2008年 / 77卷 / 09期
关键词
D O I
10.1103/PhysRevD.77.094503
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a two-flavor QCD calculation of B-K on a 16(3)x32 lattice at a similar to 0.12 fm (or equivalently a(-1)=1.67 GeV). Both valence and sea quarks are described by the overlap fermion formulation. The matching factor is calculated nonperturbatively with the so-called RI/MOM scheme. We find that the lattice data are well described by the next-to-leading order (NLO) partially quenched chiral perturbation theory (PQChPT) up to around a half of the strange quark mass (m(s)(phys)/2). The data at quark masses heavier than m(s)(phys)/2 are fitted including a part of next-to-next-to-leading order terms. We obtain B-K((MS) over bar) (2 GeV)=0.537(4)(40), where the first error is statistical and the second is an estimate of systematic uncertainties from finite volume, fixing topology, the matching factor, and the scale setting.
引用
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页数:16
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