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Related papers: Factorization and Nonfactorization in B Decays

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A careful quark-diagram analysis shows that a number of two-body nonleptonic $B$ decays can occur through the so-called hairpin diagram, a QCD loop-induced graph different from penguin in final-state hadronization of valence quarks. Using…

High Energy Physics - Phenomenology · Physics 2010-11-01 Dongsheng Du , Zhi-zhong Xing

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

A leading-power factorization formula for weight functions relating the B to Xs gamma photon spectrum to arbitrary partial decay rates in B to Xu l nu is derived. These weight functions are independent of the hadronic shape function and…

High Energy Physics - Phenomenology · Physics 2009-11-11 Bjorn O Lange

We study charmless two-body baryonic B decays in a diagramatic approach. Relations on decay amplitudes are obtained. In general there are more than one tree and more than one penguin amplitudes. The number of independent amplitudes can be…

High Energy Physics - Phenomenology · Physics 2009-11-10 Chun-Khiang Chua

Charmless hadronic decays of B mesons to a vector meson (V) and a tensor meson (T) are analyzed in the frameworks of both flavor SU(3) symmetry and generalized factorization. We also make comments on B decays to two tensor mesons in the…

High Energy Physics - Phenomenology · Physics 2014-11-17 C. S. Kim , B. H. Lim , Sechul Oh

The parameters $\chi_{1,2}$, which measure nonfactorizable soft gluon contributions to hadronic weak decays of mesons, are updated by extracting them from the data of $D,\,B\to PP,~VP$ decays ($P$: pseudoscalar meson, $V$: vector meson). It…

High Energy Physics - Phenomenology · Physics 2016-09-01 Hai-Yang Cheng

We develop perturbative QCD formalism for three-body nonleptonic $B$ meson decays. Leading contributions are identified by defining power counting rules for various topologies of amplitudes. The analysis is simplified into the one for…

High Energy Physics - Phenomenology · Physics 2009-11-07 Chuan-Hung Chen , Hsiang-nan Li

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

Motivated by the large rates of $B\rightarrow (\chi_{c0}, \chi_{c2}, h_c)K$ decays observed by the $BABAR$ and Belle collaborations, we investigate the nonfactorizable contributions to these factorization-forbidden decays, which can occur…

High Energy Physics - Phenomenology · Physics 2020-09-01 Ya-Qian Li , Meng-Kun Jia , Zhou Rui

Cabibbo-allowed two-body hadronic weak decays of bottom baryons are analyzed. Contrary to the charmed baryon sector, many channels of bottom baryon decays proceed only through the external or internal W-emission diagrams. Moreover,…

High Energy Physics - Phenomenology · Physics 2009-10-30 Hai-Yang Cheng

Exclusive non-leptonic two-body decays are discussed on the basis of a generalized factorization approach which also includes non-factorizeable contributions. Numerous decay processes can be described satisfactorily. The success of the…

High Energy Physics - Phenomenology · Physics 2009-10-30 Berthold Stech

We compute standard model penguin amplitudes in nonleptonic B-decays to light charmless mesons using tree amplitude data to fix hadronic parameters. The leading calculation is carried out for the alphas(mb) penguin contributions from charm…

High Energy Physics - Phenomenology · Physics 2007-07-17 Ambar Jain , Ira Z. Rothstein , Iain W. Stewart

We study the impact of recent B-factories measurements and upper limit of radiative and semileptonic rare B-decays. We present model independent constraints on the relevant Wilson coefficients and show the impact on the parameter space of…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. Lunghi

A method to extract Wilson coefficients for semi-leptonic $b\rightarrow s$ transition and form factors for the hadronic process $B\rightarrow K^*\mu^+\mu^-$ is suggested. The method is based on data of angular distribution of the process…

High Energy Physics - Phenomenology · Physics 2017-09-08 Bharti Kindra , Namit Mahajan

Two-body weak decays of bottom mesons into two pseudoscalar mesons are examined employing SU(3) flavor symmetry for the nonfactorizable matrix elements. Using certain measured Cabibo-favored modes, we fix the reduced matrix elements and…

High Energy Physics - Phenomenology · Physics 2023-11-22 Maninder Kaur , R. C. Verma

We provide a rigorous basis for factorization for a large class of non-leptonic two-body $B$-meson decays in the heavy-quark limit. The factorization formula incorporates elements of the naive factorization approach and the hard-scattering…

High Energy Physics - Phenomenology · Physics 2009-10-09 M. Beneke , G. Buchalla , M. Neubert , C. T. Sachrajda

We present a study of non-leptonic B-meson decays, partial widths and CP asymmetries, and discuss the possibilities of determining the penguin contributions through less model-dependent phenomenological analyses. In the last section we…

High Energy Physics - Phenomenology · Physics 2010-11-01 A. Deandrea , N. Di Bartolomeo , R. Gatto , F. Feruglio , G. Nardulli

Two pion decays of K mesons, K_L-K_S mass difference, two photon and the Dalitz decays of K_L are studied systematically by assuming that their amplitude is given by a sum of factorizable and non-factorizable ones. The former is estimated…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. Terasaki

We summerize the status of factorization hypothesis in the color-suppressed B meson decays : $B \to J/\psi K^{(*)}$. We present the general formalism for decay rates and polarization fractions with considering all possible non-factorizable…

High Energy Physics - Phenomenology · Physics 2007-05-23 Y. -Y. Keum

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
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