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Related papers: Nonfactorizable $B\to\chi_{c0}K$ decay and QCD fac…

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The $B_{c}^{\ast}$ ${\to}$ $B_{u,d,s}V$, $B_{u,d,s}P$ decays are investigated with the QCD factorization approach, where $V$ and $P$ denote the ground $SU(3)$ vector and pseudoscalar mesons, respectively. The $B_{c}^{\ast}$ ${\to}$…

High Energy Physics - Phenomenology · Physics 2017-05-29 Junfeng Sun , Yueling Yang , Na Wang , Qin Chang , Gongru Lu

We study exclusive non-leptonic two-body $B_c\to(D_{(s)},\eta_c,B_{(s)})+F$ decays with $F$(pseudoscalar or vector meson) being factored out in QCD factorization approach. The non-leptonic decay amplitudes are related to the product of…

High Energy Physics - Phenomenology · Physics 2009-12-14 Ho-Meoyng Choi , Chueng-Ryong Ji

The decay modes of the type $B \rightarrow \pi \, \pi $ are dynamically different. For the case $\bar{B_{d}^0} \rightarrow \, \pi^+ \pi^- $ there is a substantial factorized contribution which dominates. In contrast, the decay mode…

High Energy Physics - Phenomenology · Physics 2011-03-22 Jan O. Eeg , Teresa Palmer

Using the form factors obtained from holographic AdS/QCD and QCD sum rules, we predict the differential branching ratio and longitudinal polarization fraction for the rare $B\to K^* \nu \bar\nu$ decay. This is an interesting decay channel…

High Energy Physics - Phenomenology · Physics 2018-07-31 Mohammad Ahmady , Alexandre Leger , Zoe McIntyre , Alexander Morrison , Ruben Sandapen

We study the radiative decay B -> gamma l nu_l in the framework of QCD factorization. We demonstrate explicitly that, in the heavy-quark limit and at one-loop order in perturbation theory, the amplitude does factorize, i.e. that it can be…

High Energy Physics - Phenomenology · Physics 2009-10-09 S. Descotes-Genon , C. T. Sachrajda

We update QCD calculations of $B \to \pi, K$ form factors at large hadronic recoil by including the subleading-power corrections from the higher-twist $B$-meson light-cone distribution amplitudes (LCDAs) up to the twist-six accuracy and the…

High Energy Physics - Phenomenology · Physics 2019-01-30 Cai-Dian Lü , Yue-Long Shen , Yu-Ming Wang , Yan-Bing Wei

The rare decays $B^0 \to D_s^- K^+$ and $B^+ \to D_s^+ \bar{K}^0$ can occur only via annihilation type diagrams in the standard model. We calculate these decays in perturbative QCD approach. We found that the calculated branching ratio of…

High Energy Physics - Phenomenology · Physics 2009-01-07 Cai-Dian Lu , Kazumasa Ukai

In perturbative QCD approach, we investigate the $B(B_{s})\rightarrow D_{(s)}(\bar{D}_{(s)})\,T$ and $D_{(s)}^{*}(\bar{D}_{(s)}^{*})\,T$ decays, which include the Cabibbo-Kobayashi-Maskawa (CKM) favored decays and the…

High Energy Physics - Phenomenology · Physics 2013-05-30 Zhi-Tian Zou , Xin Yu , Cai-Dian Lu

We consider the color suppressed (nonfactorizable) amplitude for the decay mode $\bar{B_{d}^0} \rightarrow \pi^0 \pi^{0} $. We treat the $b$-quark in the heavy quark limit and the energetic light ($u,d,s$) quarks within a variant of Large…

High Energy Physics - Phenomenology · Physics 2012-12-10 J. O. Eeg

We present a detailed study of $B\to K_1(1270) \gamma$ and $B\to K_1(1400) \gamma$ decays. Using the light-cone sum rule technique, we calculate the $B\to K_{1A} (1^3P_1)$ and $B\to K_{1B} (1^1P_1)$ tensor form factors, $T_1^{K_{1A}}(0)$…

High Energy Physics - Phenomenology · Physics 2014-11-18 Hisaki Hatanaka , Kwei-Chou Yang

We analyze B -> K H_c (where H_c = eta_c, J/psi, chi_{cJ(J=0,1)}) decays estimating nonfactorizable contributions from the light-cone sum rules (LCSR). Nonfactorizable contributions are sizable for B -> K J/psi and particularly for B -> K…

High Energy Physics - Phenomenology · Physics 2009-11-10 Blazenka Melic

We studied the nonleptonic $B_{c}$ ${\to}$ $BP$, $BV$ decay with the QCD factorization approach. It is found that the Cabibbo favored processes of $B_{c}$ ${\to}$ $B_{s}{\pi}$, $B_{s}{\rho}$, $B_{u}\bar{K}$ are the promising decay channels…

High Energy Physics - Phenomenology · Physics 2015-04-07 Junfeng Sun , Na Wang , Qin Chang , Yueling Yang

Within the QCD factorization approach we compute the amplitudes for annihilation channels of B mesons decays into final states containing two pseudoscalar particles. These decays may be plagued by effects like non-perturbative physics or…

High Energy Physics - Phenomenology · Physics 2011-03-23 A. A. Natale , C. M. Zanetti

In the two-quark model supposition for $K_0^{*}(1430)$, which can be viewed as either the first excited state (scenario I) or the lowest lying state (scenario II), the branching ratios and the direct CP-violating asymmetries for decays…

High Energy Physics - Phenomenology · Physics 2011-06-07 Zhi-Qing Zhang

We calculate the important next-to-leading-order (NLO) contributions to the $B \to K K^*$ decays from the vertex corrections, the quark loops, and the magnetic penguins in the perturbative QCD (pQCD) factorization approach. The pQCD…

High Energy Physics - Phenomenology · Physics 2009-01-14 Zhi-Qing Zhang , Zhen-Jun Xiao

The decay amplitudes for anti-B0 -> Ds+ Ds- and anti-Bs0 -> D+ D- have no factorizable contributions. We suggest that dominant contributions to the decay amplitudes arise from two chiral loop contributions and one soft gluon emission…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. O. Eeg , S. Fajfer , A. Hiorth

We calculate the branching ratios and CP asymmetries for B^0 to pi^+pi^-, B^+ to pi^+pi^0 and B^0 to pi^0pi^0 decays, in a perturbative QCD approach. In this approach, we calculate non-factorizable and annihilation type contributions, in…

High Energy Physics - Phenomenology · Physics 2009-10-31 C. D. Lu , K. Ukai , M. Z. Yang

We report on the search for the factorization suppressed decays B -> chi_c0 K(*) and B -> chi_c2 K(*), with chi_c0 and chi_c2 decaying into J/psi gamma. We use a sample of 124 million BBbar events collected with the BABAR detector at the…

High Energy Physics - Experiment · Physics 2007-05-23 B. Aubert , BABAR Collaboration

We point out that the decay mode D^0 -> K^0 \bar{K^0} has no factorizable contribution. In the chiral perturbation language, treating D^0 as heavy, the O(p) contribution is zero. We calculate the nonfactorizable chiral loop contributions of…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. O. Eeg , S. Fajfer , J. Zupan

We carry out a comprehensive analysis of the full set of $\bar{B}_q \to D_q^{(*)}$ form factors for spectator quarks $q=u,d,s$ within the framework of the Heavy-Quark Expansion (HQE) to order $\mathcal{O}(\alpha_s, 1/m_b, 1/m_c^2)$. In…

High Energy Physics - Phenomenology · Physics 2020-05-20 Marzia Bordone , Nico Gubernari , Martin Jung , Danny van Dyk
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