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首页> 外文期刊>Journal of Physics, G. Nuclear and Particle Physics: An Institute of Physics Journal >The B -> K* transition form factors within the QCD light-cone sum rules and their application to the semi-leptonic decay B -> K* mu(+)mu(-)
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The B -> K* transition form factors within the QCD light-cone sum rules and their application to the semi-leptonic decay B -> K* mu(+)mu(-)

机译:QCD视锥和规则中的B-> K *过渡形状因子及其在半轻子衰变中的应用B-> K * mu(+)mu(-)

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We present a detailed calculation on the B -> K* transition form factors (TFFs), A(0,1,2), V and T-1,T-2,T-3, within the QCD light-cone sum rules (LCSRs). To suppress the contributions from high-twist light-cone distribution amplitudes, we adopt a right-handed chiral correlator to do the LCSR calculation. In the resultant LCSRs for the TFFs, the transverse leading-twist distribution amplitude phi(perpendicular to)(2;K) provides over 90% contribution, thus those TFFs provide good platforms for testing the property of phi(perpendicular to)(2;K*), We suggest a model for phi(perpendicular to)(2;K*), in which two parameters B-2;K*(perpendicular to) and C-2;K*(perpendicular to) dominantly control its longitudinal distribution. With a proper choice of B-2;K*(perpendicular to), and our predictions on B -> K* TFFs are consistent with those of lattice QCD predictions. As an application, we also calculate the branching fraction of the B-meson rare decay B -> K*mu(+)mu(-). The predicted differential branching fraction, dB/dq(2)(B -> K* mu(+)mu(-)) is consistent with the LHCb and Belle measurements within errors. After integrating over the allowable q(2)-region, we get the branching fraction, B(B -> K*mu(+)mu(-)) = (1.088(-0.205)(+0.261)) x 10(-6), where the errors are squared average of the mentioned error sources. When the precision of experimental measurements or the other source of theoretical uncertainties for this process have been further improved in the future, we may get a definite conclusion on the behavior of phi(perpendicular to)(2;K*).
机译:我们在QCD视锥总和规则内,对B-> K *过渡形状因子(TFF),A(0,1,2),V和T-1,T-2,T-3进行了详细的计算(LCSR)。为了抑制高扭转锥分布幅度的贡献,我们采用右旋手性相关器进行LCSR计算。在所得的TFF的LCSR中,横向前向扭曲分布幅度phi(垂直于)(2; K)贡献了90%以上,因此,这些TFF为测试phi(垂直于)(2; K)的特性提供了良好的平台。 K *),我们建议建立phi(垂直于)(2; K *)的模型,其中两个参数B-2; K *(垂直于)和C-2; K *(垂直于)控制其纵向分配。通过适当选择B-2; K *(垂直于),我们对B-> K * TFF的预测与点阵QCD的预测一致。作为应用,我们还计算了B介子罕见衰变B-> K * mu(+)mu(-)的分支分数。预测的差分分支分数dB / dq(2)(B-> K * mu(+)mu(-))与LHCb和Belle测量值在误差范围内一致。在允许的q(2)区域上积分后,我们得到分支分数B(B-> K * mu(+)mu(-))=(1.088(-0.205)(+ 0.261))x 10(- 6),其中误差是上述误差源的平方均值。当将来进一步提高该过程的实验测量精度或其他理论不确定性来源时,我们可以得出关于phi(垂直于)(2; K *)的行为的肯定结论。

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