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首页> 外文期刊>The journal of high energy physics >The B ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ overline{B} $$end{document} π form factors from QCD and their impact on |V ub |
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The B ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ overline{B} $$end{document} π form factors from QCD and their impact on |V ub |

机译:<内联公式id =“IEQ1”> <替代方案> B ˉ DocumentClass [12pt] {minimal} usepackage {ammath} usepackage {isysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {supmeek} setLength { oddsidemargin} { - 69pt} begin {document} $$ overline {b} $$ end {document} <内联图xlink:href =“13130_2021_16134_ARTICLE_IEQ1.gif”/> π表单因子 QCD及其对<斜斜体> | v <斜体> Ub |

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摘要

A bstract We revisit light-cone sum rules with pion distribution amplitudes to determine the full set of local B ˉ documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ overline{B} $$end{document} → π form factors. To this end, we determine all duality threshold parameters from a Bayesian fit for the first time. Our results, obtained at small momentum transfer q ~(2), are extrapolated to large q ~(2)where they agree with precise lattice QCD results. We find that a modification to the commonly used BCL parametrization is crucial to interpolate the scalar form factor between the two q ~(2)regions. We provide numerical results for the form factor parameters — including their covariance — based on simultaneous fit of all three form factors to both the sum rule and lattice QCD results. Our predictions for the form factors agree well with measurements of the q ~(2)spectrum of the semileptonic decay B ˉ 0 → π + ? ? ν ˉ ? documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$ {overline{B}}^0o {pi}^{+}{mathrm{ell}}^{-}{overline{u}}_{mathrm{ell}} $$end{document} . From the world average of the latter we obtain | V _( ub )| = (3 . 77 ± 0 . 15) · 10~( ? 3), which is in agreement with the most recent inclusive determination at the 1 σ level.
机译:甲bstract我们重新审视与π介子分布幅值光锥求和规则,以确定完整的一组局部B的ˉ的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} {usepackage mathrsfs} {usepackage upgreek} setlength { oddsidemargin} { - 69pt} {开始文档} $$ 划线{B} $$ {端文档}→π形状因子。为此,我们从一个贝叶斯适合首次确定所有二元性阈值参数。我们的研究结果,在小动量传递Q〜(2)中获得,外推到大的Q〜(2),其中它们具有精确的晶格QCD结果一致。我们发现,与通常使用的BCL参数化的修改是至关重要的两个Q〜(2)区域之间插入的标外形。我们为外形参数数值结果 - 包括他们的协方差 - 基于三个形式因素的总和规则和晶格QCD结果两者同时配合。我们对形状因子预测该q〜(2)的半轻衰变乙ˉ0→π+的光谱的测量值吻合很好?还是νˉ? 的DocumentClass [12磅] {最小} usepackage {amsmath} usepackage {wasysym} usepackage {amsfonts} usepackage {amssymb} usepackage {amsbsy} usepackage {mathrsfs} usepackage {upgreek} setlength { oddsidemargin} { -69pt} {开始文档} $$ {划线{B}} ^ 0 到{ PI} ^ {+} { mathrm { ELL}} ^ { - } {划线{ NU}} _ { mathrm { ELL}} $$ {端文档}。从世界平均水平,我们获得后者的| v _(UB)| =(3 77±0。15)·10〜(?3),其与在1个σ水平最近包容确定协议。

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