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Charmless decays B -> PP, PV, and effects of new strong and electroweak penguins in Topcolor-assisted Technicolor model

机译:无魅力衰弱B - > pp,pV,以及新强和弱电的影响   Topcolor辅助Technicolor模型中的企鹅

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摘要

Based on the low energy effective Hamiltonian with generalized factorization,we calculate the new physics contributions to the branching ratios andCP-violating asymmetries of the two-body charmless hadronic decays $B \to PP,PV$ from the new strong and electroweak penguin diagrams in the TC2 model. Thetop-pion penguins dominate the new physics corrections, and both new gluonicand electroweak penguins contribute effectively to most decay modes. Fortree-dominated decay modes $B \to \pi \pi, \rho \pi, etc,$ the new physicscorrections are less than 10%. For decays $B \to K^{(*)} \pi$, $K^{(*)} \eta$,$etc$, the new physics enhancements can be rather large (from $- 70%$ to $\sim200%$) and are insensitive to the variations of $N_c^{eff}$, $k^2$, $\eta$ and$m_{\tilde{\pi}}$ within the reasonable ranges. For decays $B^0 \to \phi \pi$,$\phi \eta^{(')}$, $K^* \bar{K}^0$ and $\rho^+ K^0$, $\delta {\cal B}$ isstrongly $N_c^{eff}-$dependent: varying from -90% to $\sim 1680%$ in the rangeof $N_c^{eff}=2-\infty$. The new physics corrections to the CP-violatingasymmetries ${\cal A}_{CP}$ vary greatly for different B decay channels. Forfive measured CP asymmetries of $B \to K \pi, K \eta', \omega \pi$ decays,$\delta {\cal A}_{CP}$ is only about 20% and will be masked by largetheoretical uncertainties. The new physics enhancements to interesting $B \to K\eta'$ decays are significant in size ($\sim 50%$), insensitive to thevariations of input parameters and hence lead to a plausible interpretation forthe unexpectedly large $B \to K \eta'$ decay rates. The TC2 model predictionsfor branching ratios and CP-violating asymmteries of all fifty seven $B \to PP,PV$ decay modes are consistent with the available data within one or twostandard deviations.
机译:基于具有广义因式分解的低能量有效哈密顿量,我们根据新的强企鹅图和电弱企鹅图,计算了两体无魅力强子衰变$ B \到PP,PV $的分支比和CP违反对称性的新物理贡献。 TC2模型。 toptop-pion企鹅主导了新的物理校正,而新的gluonic和电弱企鹅都对大多数衰减模式做出了有效贡献。对于以树为主导的衰减模式$ B \到\ pi \ pi,\ rho \ pi等,$新的物理校正小于10%。对于衰落$ B \ to K ^ {(*)} \ pi $,$ K ^ {(*)} \ eta $,$ etc $,新的物理增强可能会很大(从$-70%$到$ \ sim200%$),并且对$ N_c ^ {eff} $,$ k ^ 2 $,$ \ eta $和$ m _ {\ tilde {\ pi}} $在合理范围内的变化不敏感。对于衰减$ B ^ 0 \至\ phi \ pi $,$ \ phi \ eta ^ {('}} $,$ K ^ * \ bar {K} ^ 0 $和$ \ rho ^ + K ^ 0 $, $ \ delta {\ cal B} $与$ N_c ^ {eff}-$密切相关:从-90%到$ \ sim 1680%$在$ N_c ^ {eff} = 2- \ infty $范围内变化。对于CP违反对称性$ {\ cal A} _ {CP} $,新的物理校正对于不同的B衰减通道有很大的不同。 $ B \到K \ pi,K \ eta',\ omega \ pi $衰减的五个测得CP不对称性,$ \ delta {\ cal A} _ {CP} $仅约20%,并且会被较大的理论不确定性掩盖。对有趣的$ B \ to K \ eta'$衰变的新的物理增强在大小上非常重要($ \ sim 50%$),对输入参数的变化不敏感,因此导致对意外大的$ B \ to K的合理解释\ eta'$衰减率。 TC2模型对所有57个B到PP,PV $衰减模式的分支比和违反CP的不对称性的预测与一个或两个标准偏差内的可用数据一致。

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