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Related papers: Charmless $\bar{B}_s\to VV$ Decays in QCD Factoriz…

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In this study, the nonleptonic two-body $B$ decays into two tensor mesons (including $a_2(1320)$, $K^*_2(1430)$, $f_2(1270)$, $f^\prime_2(1525)$, denoted generically as $T$) are investigated in the QCD factorization approach. The branching…

High Energy Physics - Phenomenology · Physics 2025-04-15 Ya-Bing Zuo , Jia-Yu Zou , Shi-Yu Liang , Ming-Ge Li , Shan-Shan Hu

The QCD$\times$QED factorization is studied for two-body non-leptonic and semi-leptonic $B$ decays with heavy-light final states. These non-leptonic decays, like $\bar{B}^0_{(s)}\to D^+_{(s)} \pi^-$ and $\bar{B}_d^0 \to D^+ K^-$, are among…

High Energy Physics - Phenomenology · Physics 2021-11-17 Martin Beneke , Philipp Böer , Gael Finauri , K. Keri Vos

Two body non-leptonic decays: are investigated. Baryon form factors of the heavy quark effective theory are employed. Form factors for renormalization in full QCD are also considered. We find that contributions of the non-factorizable terms…

High Energy Physics - Phenomenology · Physics 2007-05-23 Gurpreet Sidana

Within the framework of perturbative QCD approach based on $k_T$ factorization, we studied 40 $B_c \to DS$ decay modes in the leading order and leading power, where "S" stands for the light scalar meson. Under two different scenarios (S1…

High Energy Physics - Phenomenology · Physics 2018-03-28 Zhi-Tian Zou , Ying Li , Xin Liu

Using the next-to-leading order QCD-corrected effective Hamiltonian, charmless exclusive nonleptonic decays of the $B_s$ meson into $\eta$ or $\eta'$ are calculated within the generalized factorization approach. Nonfactorizable…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Tseng

The study of charmless two-body decays of B mesons is currently one of the hottest topics in B physics. QCD factorization provides the theoretical framework for a systematic analysis of such decays. A global fit to B->pi K,pi pi branching…

High Energy Physics - Phenomenology · Physics 2010-11-23 Matthias Neubert

Two body nonleptonic weak decays of bottom mesons to a pseudoscalar meson and an axial-vector meson involving charmed states are studied using the non-relativistic quark model. We calculate the branching ratios of these decays by employing…

High Energy Physics - Phenomenology · Physics 2017-08-11 Neelesh Sharma , Rohit Dhir

Although the two-body charmed decays $B_{(s)} \to \bar D_{(s)}^{(*)}P$ and $\bar D_{(s)}^{(*)}V$, where $P$($V$) denotes a light pseudoscalar(vector) meson, are CKM suppressed comparing with the $B_{(s)} \to D_{(s)}^{(*)}P$ and $…

High Energy Physics - Phenomenology · Physics 2009-11-25 Hao Zou , Run-Hui Li , Xiao-Xia Wang , Cai-Dian Lu

We calculate $\bar{B}_s^0\to \phi$ translation form factors $V$, $A_0$, $A_1$, $A_2$ based on QCD sum rule and study the nonleptonic two-body decay of $\bar{B}_s^0\to J/\psi \phi$ with the form factors obtained. We calculate the…

High Energy Physics - Phenomenology · Physics 2020-08-26 Ying-Quan Peng , Mao-Zhi Yang

Motivated by extensive new high-precision experimental data, we present an updated analysis of the two-body charm decays $D \to PV$ (with $P =\pi,K, \eta^{(\prime)}$ and $V =\rho, K^*, \omega, \phi$) within the factorization-assisted…

High Energy Physics - Phenomenology · Physics 2025-11-14 Hui Zheng , Jia-Rui Dong , Si-Hong Zhou

The $\bar{B}_{q}^{\ast}$ ${\to}$ $DP$, $DV$ weak decays are studied with the perturbative QCD approach, where $q$ $=$ $u$, $d$ and $s$; $P$ and $V$ denote the ground $SU(3)$ pseudoscalar and vector meson nonet. It is found that the…

High Energy Physics - Phenomenology · Physics 2017-08-28 Junfeng Sun , Jie Gao , Yueling Yang , Qin Chang , Na Wang , Gongru Lu , Jinshu Huang

The branchings fractions of the rare $B_s$ decays are calculated in the framework of the QCD-motivated relativistic quark model. The form factors of the weak $B_s$ transitions to light mesons are expressed through the overlap integral of…

High Energy Physics - Phenomenology · Physics 2015-06-17 R. N. Faustov , V. O. Galkin

We analyzed the nonleptonic decays $B/B_s\to \psi(2S) V $ with $V=(\rho, \omega, K^{*}, \phi)$ by employing the perturbative QCD (PQCD) factorization approach. Here the branching ratios, the $CP$ asymmetries and the complete set of…

High Energy Physics - Phenomenology · Physics 2017-09-18 Zhou Rui , Ya Li , Zhen-Jun Xiao

Motivated by the rapid development of heavy flavor physics experiment, we study the tree-dominated nonleptonic $\bar{B}_{u,d,s}^* \to D_{u,d,s}^*V$~($V=D^{*-},D_s^{*-},K^{*-},{\rho}^-$) decays within the factorization approach. The relevant…

High Energy Physics - Phenomenology · Physics 2019-09-18 Qin Chang , Yunyun Zhang , Xiaonan Li

We make a systematic investigation on the two-body nonleptonic decays $B_c\rightarrow J/\Psi(\eta_c),M$ by employing the perturbative QCD approach based on $k_T$ factorization, where $M$ is a light pseudoscalar or vector or a heavy charmed…

High Energy Physics - Phenomenology · Physics 2015-01-06 Zhou Rui , Zhi-Tian Zou

In this work, we investigate those $B_{c}\rightarrow D^{(*)}T$ decays in perturbative QCD approach, based on $k_T$ factorization, where T denotes a light tensor meson. For all decays considered in this work, there are no contributions from…

High Energy Physics - Phenomenology · Physics 2013-09-11 Zhi-Tian Zou , Xin Yu , Cai-Dian Lu

Two-body decays of B mesons are studied by decomposing their amplitude into a sum of factorizable and non-factorizable ones. The former is estimated by using the naive factorization while the latter is calculated by using a hard pion (or…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Terasaki

We calculate the hard-scattering kernels relevant to the negative-helicity decay amplitude in B decays to two vector mesons in the framework of QCD factorisation. We then perform a comprehensive analysis of the 34 B->VV decays, including…

High Energy Physics - Phenomenology · Physics 2008-11-26 Martin Beneke , Johannes Rohrer , Deshan Yang

In this paper, with the framework of (p)NRQCD and SCET, the processes $B_c\to M_1 M_2$ are investigated. Here $M_{1(2)}$ denotes the light charmless meson, such as $\pi$, $\rho$, $K$ or $K^*$. Based on the SCET power counting rules, the…

High Energy Physics - Phenomenology · Physics 2015-12-21 Wan-Li Ju , Tianhong Wang , Yue Jiang , Han Yuan , Guo-Li Wang

Within the factorization-assisted topological-amplitude approach, we study the two-body charmed $B$ meson decays $B_{u,d,s} \to D^{(*)}M$, with $M$ denoting a light pseudoscalar (or vector) meson. The meson decay constants and transition…

High Energy Physics - Phenomenology · Physics 2016-04-13 Si-Hong Zhou , Yan-Bing Wei , Qin Qin , Ying Li , Fu-Sheng Yu , Cai-Dian Lu