Physical point simulation in 2+1 flavor lattice QCD

被引:114
|
作者
Aoki, S. [1 ,2 ]
Ishikawa, K. -I. [3 ,4 ]
Ishizuka, N. [1 ,2 ]
Izubuchi, T. [5 ]
Kadoh, D. [3 ]
Kanaya, K. [1 ]
Kuramashi, Y. [1 ,3 ]
Namekawa, Y. [3 ]
Okawa, M. [4 ]
Taniguchi, Y. [1 ,3 ]
Ukawa, A. [1 ,3 ]
Ukita, N. [3 ]
Yamazaki, T. [3 ]
Yoshie, T. [1 ,3 ]
机构
[1] Univ Tsukuba, Grad Sch Pure & Appl Sci, Tsukuba, Ibaraki 3058571, Japan
[2] Brookhaven Natl Lab, Riken BNL Res Ctr, Upton, NY 11973 USA
[3] Univ Tsukuba, Ctr Computat Sci, Tsukuba, Ibaraki 3058577, Japan
[4] Hiroshima Univ, Grad Sch Sci, Hiroshima 7398526, Japan
[5] Kanazawa Univ, Inst Theoret Phys, Kanazawa, Ishikawa 9201192, Japan
来源
PHYSICAL REVIEW D | 2010年 / 81卷 / 07期
关键词
DYNAMICAL FERMIONS; PHMC ALGORITHM;
D O I
10.1103/PhysRevD.81.074503
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present the results of the physical point simulation in 2 + 1 flavor lattice QCD with the non-perturbatively O(a)-improved Wilson quark action and the Iwasaki gauge action at beta = 9 on a 32(3) x 64 lattice. The physical quark masses together with the lattice spacing is determined with m(pi), m(K) and m(Omega) as physical inputs. There are two key algorithmic ingredients to make possible the direct simulation at the physical point: One is the mass-preconditioned domain-decomposed HMC algorithm to reduce the computational cost. The other is the reweighting technique to adjust the hopping parameters exactly to the physical point. The physics results include the hadron spectrum, the quark masses and the pseudo-scalar meson decay constants. The renormalization factors are nonperturbatively evaluated with the Schrodinger functional method. The results are compared with the previous ones obtained by the chiral extrapolation method.
引用
收藏
页数:12
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