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三味格点量子色动力学中的B介子和D介子衰变常数

Bs and Ds decay constants in three-flavor lattice QCD.

作者信息

Wingate Matthew, Davies Christine T H, Gray Alan, Lepage G Peter, Shigemitsu Junko

机构信息

Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA.

出版信息

Phys Rev Lett. 2004 Apr 23;92(16):162001. doi: 10.1103/PhysRevLett.92.162001. Epub 2004 Apr 22.

Abstract

Capitalizing on recent advances in lattice QCD, we present a calculation of the leptonic decay constants f(B(s)) and f(D(s)) that includes effects of one strange sea quark and two light sea quarks via an improved staggered action. By shedding the quenched approximation and the associated lattice scale uncertainty, lattice QCD greatly increases its predictive power. Nonrelativistic QCD is used to simulate heavy quarks with masses between 1.5m(c) and m(b). We arrive at the following results: f(B(s))=260+/-7+/-26+/-8+/-5 and f(D(s))=290+/-20+/-29+/-29+/-6 MeV. The first quoted error is the statistical uncertainty, and the rest estimate the sizes of higher order terms neglected in this calculation. All of these uncertainties are systematically improvable by including another order in the weak coupling expansion, the nonrelativistic expansion, or the Symanzik improvement program.

摘要

利用格点量子色动力学(lattice QCD)的最新进展,我们给出了轻子衰变常数$f(B(s))$和$f(D(s))$的计算结果,该计算通过改进的交错作用包含了一个奇异海夸克和两个轻海夸克的效应。通过摒弃淬火近似和相关的格点尺度不确定性,格点量子色动力学大大提高了其预测能力。非相对论量子色动力学用于模拟质量在$1.5m_c$和$m_b$之间的重夸克。我们得到以下结果:$f(B(s)) = 260 \pm 7 \pm 26 \pm 8 \pm 5$以及$f(D(s)) = 290 \pm 20 \pm 29 \pm 29 \pm 6$兆电子伏特。第一个引用的误差是统计不确定性,其余的则估计了此计算中忽略的高阶项的大小。通过在弱耦合展开、非相对论展开或Symanzik改进程序中包含更高阶项,所有这些不确定性都可以系统地得到改进。

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