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B_s → D_sℓν form factors and the fragmentation fraction ratio f_s/f_d

机译:B_S→D_Sℓν形式因子和碎片分数比F_S / F_D

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We present a lattice quantum chromodynamics determination of the scalar and vector form factors for the B_s → D_sℓν decay over the full physical range of momentum transfer. In conjunction with future experimental data, our results will provide a new method to extract |V_(cb)|, which may elucidate the current tension between exclusive and inclusive determinations of this parameter. Combining the form factor results at nonzero recoil with recent HPQCD results for the B → Dlν form factors, we determine the ratios f_0~(B_s→D_s)(M_π~2)/f_0~(B→D) (M_K~2) = 1.000(62) and f_0~(B_s→D_s)(M(M_π~2) = 1.006(62). These results give the fragmentation fraction ratios f_s/f_d = 0.310(30)_(stat)(21)_(syst)(6)_(theor)(38)_(latt) and f_s/f_d = 0.307(16)_(stat)(21)_(syst)(23)_(theor) (44)_(latt), respectively. The fragmentation fraction ratio is an important ingredient in experimental determinations of Bs meson branching fractions at hadron colliders, in particular for the rare decay B(B_s →μ~+μ ~-). In addition to the form factor results, we make the first prediction of the branching fraction ratio R(D_S) = B(Bs → D_sτν)/B(B_s → D_sℓv) = 0.301(6), where ℓ is an electron or muon. Current experimental measurements of the corresponding ratio for the semileptonic decays of B mesons disagree with Standard Model expectations at the level of nearly four standard deviations. Future experimental measurements of R(D_s) may help understand this discrepancy.
机译:我们呈现了晶格量子色动力学测定的标量和向量形式因子的序列→D_sℓν衰减在全物理转移的全物理范围内。与未来的实验数据结合使用,我们的结果将提供一种提取的新方法(CB)|,该方法可以阐明该参数的独有和包容性决定之间的电流张力。将Form因素结果与最近的B→DLν形式因子的HPQCD结果相结合,确定比率F_0〜(B_S→D_S)(M_π〜2)/ f_0〜(b→d)(m_k〜2)= 1.000(62)和f_0〜(b_s→d_s)(m(m_π〜2)= 1.006(62)。这些结果给出了碎片分数比f_s / f_d = 0.310(30)_(stat)(21)_(styst )(6)_(您)(38)_(latt)和f_s / f_d = 0.307(16)_(stat)(21)_(stys)(23)_(steor)(44)_(latt),分别。碎裂级分比是强子煤机Bs Meson分支级分的实验测定中的重要成分,特别是对于罕见的衰减B(b_s→μ〜+μ〜 - )。除了表单因素结果,我们制造分支级分比R(D_S)= B(BS→D_Sτν)/ B(B_S→D_SℓV)= 0.301(6)的第一预测,其中ℓ是电子或μ子。当前的半智能比率的实验测量值B斯顿的衰减不同意标准模型期望,在近四个标准偏差的水平上。未来的经验R(D_S)的实体测量可能有助于理解这种差异。

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  • 来源
    《Physical Review D 》 |2017年第12期| 114506.1-114506.18| 共18页
  • 作者单位

    New High Energy Theory Center and Department of Physics and Astronomy Rutgers The StateUniversity of New Jersey 136 Frelinghuysen Road Piscataway New Jersey 08854 USA Department of Physics and Astronomy University of Utah Salt Lake City Utah 84112 USA;

    Department of Physics and Astronomy University of Utah Salt Lake City Utah 84112 USA Ohio Supercomputer Center 1224 Kinnear Road Columbus Ohio 43212 USA;

    School of Physics and Astronomy University of Glasgow Glasgow G12 8QQ United Kingdom Department of Physics and Astronomy College of William and Mary Williamsburg Virginia 23187 USA;

    Laboratory of Elementary Particle Physics Cornell University Ithaca New York 14853 USA;

    Department of Physics The Ohio State University Columbus Ohio 43210 USA;

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