$B_c \到B_{s(d)}$形式因子

Laurence J. Cooper, M. Wingate, C. Davies, J. Harrison, J. Komijani
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引用次数: 0

摘要

给出了弱矩阵元$B_c \到$ B_s$和$B_c \到$ B_d$的第一次点阵QCD计算结果。结果来源于在晶格间距在$0.12$ [fm]和$0.06$ [fm]之间的MILC协作规范配置上计算的相关函数,包括高度改进的交错夸克(HISQ)形式体系中的2+1+1动态海夸克。然后提取整个物理$q^2$范围内的形状因子并外推到物理连续体极限。底夸克采用了两种不同的形式:非相对论性QCD (NRQCD)和重hisq。检查这两种方法之间的一致性是对我们在晶格上的重夸克策略的重要测试。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
$B_c \to B_{s(d)}$ form factors
We present results of the first lattice QCD calculations of $B_c \to B_s$ and $B_c \to B_d$ weak matrix elements. Results are derived from correlation functions computed on MILC Collaboration gauge configurations with lattice spacings between $0.12$ [fm] and $0.06$ [fm] including 2+1+1 flavours of dynamical sea quarks in the Highly Improved Staggered Quark (HISQ) formalism. Form factors across the entire physical $q^2$ range are then extracted and extrapolated to the physical-continuum limit. Two different formalisms are employed for the bottom quark: non-relativistic QCD (NRQCD) and heavy-HISQ. Checking agreement between these two approaches is an important test of our strategies for heavy quarks on the lattice.
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