Pion decay constant for the Kogut-Susskind quark action in quenched lattice QCD -: art. no. 094501

被引:15
作者
Aoki, S [1 ]
Fukugita, M
Hashimoto, S
Ishikawa, KI
Ishizuka, N
Iwasaki, Y
Kanaya, K
Kaneda, T
Kaya, S
Kuramashi, Y
Okawa, M
Onogi, T
Tominaga, S
Tsutsui, N
Ukawa, A
Yamada, N
Yoshié, T
机构
[1] Univ Tsukuba, Inst Phys, Tsukuba, Ibaraki 3058571, Japan
[2] Univ Tokyo, Inst Cosm Ray Res, Tokyo 1888502, Japan
[3] High Energy Accelerator Res Org KEK, Tsukuba, Ibaraki 3050801, Japan
[4] Univ Tsukuba, Ctr Computat Phys, Tsukuba, Ibaraki 3058577, Japan
[5] Washington Univ, Dept Phys, St Louis, MO 63130 USA
[6] Hiroshima Univ, Dept Phys, Hiroshima 7398526, Japan
关键词
D O I
10.1103/PhysRevD.62.094501
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a study for the pion decay constant f(pi) in the quenched approximation to lattice QCD with the Kogut-Susskind (KS) quark action, with the emphasis given to the renormalization problems. Numerical simulations are carried out at the couplings beta = 6.0 and 6.2 on 32(3) x 64 and 48(3) x 64 lattices, respectively. The pion decay constant is evaluated for all KS flavors via gauge invariant and noninvariant axial vector currents with the renormalization constants calculated by both the nonperturbative method and perturbation theory. We obtain f(pi) = 89(6) MeV in the continuum limit as the best value using the partially conserved axial vector current, which requires no renormalization. From a study for the other KS flavors we find that the results obtained with the nonperturbative renormalization constants are well convergent among the KS flavors in the continuum limit, confirming restoration of SU(4)(A), flavor symmetry, while perturbative renormalization still leaves an apparent flavor breaking effect even in the continuum limit.
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页码:1 / 15
页数:15
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