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arXiv 0709.0137hep-phhep-ex
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强子无粲B衰变B-> AP

Hadronic charmless B decays B-> AP

Hai-Yang Cheng, Kwei-Chou Yang

摘要:

在QCD分解框架下研究了B介子到赝标和轴矢量介子的两体强子衰变。用QCD求和规则方法计算了$^3P_1$和$^1P_1$轴矢量介子的光锥分布振幅。由于G宇称的存在,在SU(3)极限下,在夸克和反夸克动量分数交换下,$^3P_1$($^1P_1$)介子的手征偶两部分子光锥分布振幅是对称的(反对称的).对于手性奇数LCD,则相反。主要结果如下:(1)对$a_1^\pm(1260)π^\mp$、$b_1^\pm(1235)π^\mp$、$b_1^0(1235)π^-$、$a_1^+K^-$和$b_1^+K^-$模式的预测率与数据吻合良好。然而,天真地期望的比率$Br(B^-\to a_1^0π^-)/Br(\ov B^0\to a_1^+π^-)\leq 1$、$Br(B^-\to a_1^-π^0)/Br(\ov B^0\to a_1^-π^+)\sim {1\over 2}$和$Br(B^-\to b_1^0K^-)/Br(\ov B^0\to b_1^+K^-)\sim {1\over 2}$没有被实验证实。这应该通过改进这些衰变的测量来澄清。(ii)由于$\bar B\to b_1K$衰变接收相当大的湮灭贡献,它们的速率对企鹅项和湮灭项之间的干扰很敏感。$Br(\bar B^0\to b_1^+K^-)$的测量意味着相消干涉,这反过来表明$B\to b_1$和$B\to a_1$转变的形状因子具有相反的符号。(iii)需要诸如弱湮灭之类的大功率校正来解释企鹅主导模式$K_1^-(1270)π^+$和$K_1^-(1400)π^+$的观测速率。

英文摘要:

The two-body hadronic decays of B mesons into pseudoscalar and axial vector mesons are studied within the framework of QCD factorization. The light-cone distribution amplitudes (LCDAs) for $^3P_1$ and $^1P_1$ axial-vector mesons have been evaluated using the QCD sum rule method. Owing to the G-parity, the chiral-even two-parton light-cone distribution amplitudes of the $^3P_1$ ($^1P_1$) mesons are symmetric (antisymmetric) under the exchange of quark and anti-quark momentum fractions in the SU(3) limit. For chiral-odd LCDAs, it is other way around. The main results are the following: (i) The predicted rates for $a_1^\pm(1260)π^\mp$, $b_1^\pm(1235)π^\mp$, $b_1^0(1235)π^-$, $a_1^+K^-$ and $b_1^+K^-$ modes are in good agreement with the data. However, the naively expected ratios $Br(B^-\to a_1^0π^-)/Br(\ov B^0\to a_1^+π^-)\leq 1$, $Br(B^-\to a_1^-π^0)/Br(\ov B^0\to a_1^-π^+)\sim {1\over 2}$ and $Br(B^-\to b_1^0K^-)/Br(\ov B^0\to b_1^+K^-)\sim {1\over 2}$ are not borne out by experiment. This should be clarified by the improved measurements of these decays. (ii) Since the $\bar B\to b_1K$ decays receive sizable annihilation contributions, their rates are sensitive to the interference between penguin and annihilation terms. The measurement of $Br(\bar B^0\to b_1^+K^-)$ implies a destructive interference which in turn indicates that the form factors for $B\to b_1$ and $B\to a_1$ transitions are of opposite signs. (iii) Sizable power corrections such as weak annihilation are needed to account for the observed rates of the penguin-dominated modes $K_1^-(1270)π^+$ and $K_1^-(1400)π^+$.

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