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Related papers: Non-factorizable contributions in B decays revisit…

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Using the QCD sum rules technique we study several aspects of the phenomenology of the b-flavoured strange meson $B_s^0$. In particular, we evaluate the mass of the particle, the leptonic constant and the form factors of the decays…

High Energy Physics - Phenomenology · Physics 2009-10-22 P. Blasi , P. Colangelo , G. Nardulli AND N. Paver

Nonfactorizable contributions to exclusive two-body nonleptonic weak decays of heavy mesons arising from color octet currents, characterized by the parameter $r_2$, are extracted from the data. It is found that $r_2$ is equal to $\sim…

High Energy Physics - Phenomenology · Physics 2009-10-28 Hai-Yang Cheng

Status of nonfactorizable effects in exclusive hadronic weak decays of $D$ and $B$ mesons is reviewed.

High Energy Physics - Phenomenology · Physics 2007-05-23 Hai-Yang Cheng

We compute important ratios between decay widths of some exclusive two-body nonleptonic and semileptonic B decays, which could be test of factorization hy- pothesis. We also present a summary of the expressions of the decay widths and…

High Energy Physics - Phenomenology · Physics 2011-05-17 J. H. Muñoz , N. Quintero

We show -- by explicit computation of first-order corrections -- that the QCD factorization approach previously applied to hadronic two-body decays and to form factor ratios also allows us to compute non-factorizable corrections to…

High Energy Physics - Phenomenology · Physics 2010-03-26 M. Beneke , Th. Feldmann , D. Seidel

Exclusive nonleptonic bottom meson decays are studied in the covariant osillator quark model using the factorization assumption. The main feature of this model is that it can simultaniously be applied to both heavy to heavy and heavy to…

High Energy Physics - Phenomenology · Physics 2009-10-31 Rukmani Mohanta , Anjan K. Giri , Mohinder P. Khanna , Muneyuki Ishida , Shin Ishida , Masuho Oda

Many known models, which generally use a factorization hypothesis, give a poor account of the decays B into J/psi + K(*). Usually there is a free overall factor, which is fit to the data, so that tests of the models rely upon ratios. The…

High Energy Physics - Phenomenology · Physics 2009-09-25 Carl E. Carlson , J. Milana

I briefly introduce the theoretical frameworks for studies of two-body hadronic $B$ meson decays, which include the factorization assumption, the QCD-improved factorization, the perturbative QCD, the soft-collinear effective theory, the…

High Energy Physics - Phenomenology · Physics 2014-11-20 Hsiang-nan Li

Two-body non-leptonic decays of B mesons into PT and VT modes are calculated using the non-relativistic quark model of Isgur et al.. The predictions obtained for $B \to \pi D^*_2, \rho D_2^*$ are a factor of $3\sim 5$ below present…

High Energy Physics - Phenomenology · Physics 2016-09-06 G. Lopez Castro , J. H. Munoz

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

We discuss applications of the perturbative QCD approach in the exclusive non-leptonic two body B-meson decays. We briefly review its ingredients and some important theoretical issues on the factorization approaches. PQCD results are…

High Energy Physics - Phenomenology · Physics 2011-07-19 Y. -Y. Keum

I explain how various aspects of factorization in exclusive b decays can be studied with mesons having a small decay constant or spin greater than one.

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Diehl

We briefly review the status of factorization in $b$-decays. We discuss several experimental tests of its nature and stress their importance. We show that decays into mesons which have small decay constants or spin greater than one…

High Energy Physics - Phenomenology · Physics 2009-11-07 Gudrun Hiller

We analyze charmless two-body non-leptonic B decays $B \to PP, PV$ under the framework of factorization assisted topological amplitude approach, where $P(V)$ denotes a light pseudoscalar (vector) meson. Compared with the conventional flavor…

High Energy Physics - Phenomenology · Physics 2017-03-08 Si-Hong Zhou , Qi-An Zhang , Wei-Ran Lyu , Cai-Dian Lü

Available experimental data on decay rate and polarization are used to investigate non-factorization contribution to processes of the kind $B \rightarrow K \psi$, and $B \rightarrow K^* \psi$ using five theoretical models for the…

High Energy Physics - Phenomenology · Physics 2008-02-03 A. N. Kamal , F. M. Al-Shamali

We analyze charmless two-body non-leptonic $B$ decays under the framework of factorization assisted topological amplitude approach. Unlike the conventional flavor diagram approach, we consider flavor $SU(3)$ breaking effect assisted by…

High Energy Physics - Phenomenology · Physics 2017-05-30 Cai-Dian Lu , Si-Hong Zhou

This thesis examines the non-leptonic B-decays within QCD factorisation and beyond, to challenge the assumptions and limitations of the method. We analyse the treatment of the distribution amplitudes of light mesons and present a new model…

High Energy Physics - Phenomenology · Physics 2007-05-23 Angelique N. Talbot

We discuss nonfactorizable $1/N_c$ contributions in the amplitudes of non-leptonic exclusive decays of the type $B\rightarrow D\pi$ ($N_c$ is the number of colors). In a certain kinematical limit rather reliable estimates are possible. It…

High Energy Physics - Phenomenology · Physics 2010-11-01 B. Blok , M. Shifman

We use operator product expansion and QCD light-cone sum rules to estimate the amplitude of the decay $B \to J/\psi K $ taking into account leading nonfactorizable contributions. The result is very similar to the estimate obtained earlier…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Khodjamirian , R. Rückl

We analyze quasi-two-body charmless $B$ decays $B_{(s)} \to P_1 V \to P_1 P_2 P_3$ with $V$ representing a vector resonant, and $P_{1,2,3}$ as a light pseudo-scalar meson, pion, kaon or $\eta^{(\prime)}$. The intermediate processes $B_{(s)}…

High Energy Physics - Phenomenology · Physics 2023-07-12 Si-Hong Zhou , Xin-Xia Hai , Run-Hui Li , Cai-Dian Lu