Topological susceptibility in two-flavor lattice QCD with exact chiral symmetry

被引:45
|
作者
Aoki, S. [3 ,4 ]
Chiu, T. W. [1 ,2 ]
Fukaya, H. [5 ]
Hashimoto, S. [6 ,7 ]
Hsieh, T. H. [8 ]
Kaneko, T. [6 ,7 ]
Matsufuru, H. [6 ]
Noaki, J. [6 ]
Ogawa, K. [1 ,2 ]
Onogi, T. [9 ]
Yamada, N. [6 ,7 ]
机构
[1] Natl Taiwan Univ, Ctr Theoret Sci, Dept Phys, Taipei 10617, Taiwan
[2] Natl Taiwan Univ, Natl Ctr Theoret Sci, Taipei 10617, Taiwan
[3] Univ Tsukuba, Grad Sch Pure & Appl Sci, Tsukuba, Ibaraki 3058571, Japan
[4] Brookhaven Natl Lab, Riken BNL Res Ctr, Upton, NY 11973 USA
[5] RIKEN, Theoret Phys Lab, Wako, Saitama 3510198, Japan
[6] High Energy Accelerator Res Org, Tsukuba, Ibaraki 3050801, Japan
[7] Grad Univ Adv Studies Sokendai, Sch High Energy Accelerator Sci, Tsukuba, Ibaraki 3050801, Japan
[8] Acad Sinica, Res Ctr Appl Sci, Taipei 115, Taiwan
[9] Kyoto Univ, Yukawa Inst Theoret Phys, Kyoto 6068502, Japan
关键词
D O I
10.1016/j.physletb.2008.06.039
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We determine the topological susceptibility X-t in two-flavor QCD using the lattice simulations at a fixed topological sector. The topological charge density is unambiguously defined on the lattice using the overlap-Dirac operator which possesses exact chiral symmetry. Simulations are performed on a 163 x 32 lattice at lattice spacing similar to 0.12 fm at six sea quark masses m(q) ranging in m(s)/6 - m(s) with m(s) the physical strange quark mass. The Xt is extracted from the constant behavior of the time-correlation of flavor-singlet pseudo-scalar meson two-point function at large distances, which arises from the finite size effect due to the fixed topology. In the Small m(q) regime, our result of Xt is proportional to m(q) as expected from chiral effective theory. Using the formula X-t = m(q) Sigma/N-f by Leutwyler-Smilga, we obtain the chiral condensate in N-f = 2 QCD as Sigma(MS) over bar (2 GeV) = [252(5)(10) MeV](3), in good agreement with our previous result obtained in the c-regime. (C) 2008 Elsevier B.V. All rights reserved.
引用
收藏
页码:294 / 297
页数:4
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