B meson leptonic decay constant with quenched lattice NRQCD -: art. no. 074501

被引:36
作者
Ishikawa, KI [1 ]
Yamada, N
Aoki, S
Fukugita, M
Hashimoto, S
Iskizuka, N
Iwasaki, Y
Kanaya, K
Kaneda, T
Kaya, S
Kuramashi, Y
Matsufuru, H
Okawa, M
Onogi, T
Tominaga, S
Tsutsui, N
Ukawa, A
Yoshié, T
机构
[1] Hiroshima Univ, Dept Phys, Hiroshima 7398526, Japan
[2] KEK, High Energy Accelerator Res Org, Tsukuba, Ibaraki 3050801, Japan
[3] Univ Tsukuba, Inst Phys, Tsukuba, Ibaraki 3058571, Japan
[4] Univ Tokyo, Inst Cosm Ray Res, Tokyo 1888502, Japan
[5] Univ Tsukuba, Ctr Computat Phys, Tsukuba, Ibaraki 3058577, Japan
[6] Washington Univ, Dept Phys, St Louis, MO 63130 USA
关键词
D O I
10.1103/PhysRevD.61.074501
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a lattice NRQCD study of the B meson decay constant in the quenched approximation with emphasis given to the scaling behavior. The NRQCD action and the heavy-light axial vector current we use include all terms of order 1/M and the perturbative O(alpha(s)a) and O(alpha(s)/M) corrections. Using simulations at three values of couplings beta = 5.7, 5.9, and 6.1 on lattices of sizes 12(3) x 32, 16(3) x 48, and 24(3) x 64, we find a significant a dependence disappears in f(B) if the O(alpha(s)a) correction is included in the axial vector current. We observe that beta = 5.9- 6.1 is the window where systematic errors are expected to be minimum within one-loop improved theory. Our final results are f(B) = 170(5)(15) MeV, f(Bs) = 191(4)(17)(-0 +4) MeV, and f(Bs) / f(B) = 1.12(2)(1)(-0 +3), where the first error is statistical, the second is systematic, and the third is due to the uncertainty of the strange quark mass, while quenching errors are not included.
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页数:14
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