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Related papers: $M(B^*_c)-M(B_c)$ Splitting from Nonrelativistic R…

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Nonleptonic $B_c$ decays to $P$-wave charmonia and light $\pi^+$, $K^+$, and $\rho^+$, $K^{*+}$ mesons are analysed using factorization. The hadronic form factors parametrizing the $B_c \to \chi_{cJ}(h_c)$ matrix elements are expressed in…

High Energy Physics - Phenomenology · Physics 2023-06-13 Nicola Losacco

High-energy heavy-ion collisions have been suggested as a favorable environment for the production of $B_c$ mesons, due to a much larger abundance of charm and bottom quarks compared to elementary reactions. Motivated by recent CMS data for…

Nuclear Theory · Physics 2026-01-12 Biaogang Wu , Zhanduo Tang , Min He , Ralf Rapp

The recent observation by CDF of Sigma_b^{+-} (uub and ddb) baryons within 2 MeV of the predicted Sigma_b - Lambda_b splitting has provided strong confirmation for the theoretical approach based on modeling the color hyperfine interaction.…

High Energy Physics - Phenomenology · Physics 2007-06-23 Marek Karliner , Boaz Keren-Zur , Harry J. Lipkin , Jonathan L. Rosner

We investigate the form factors of $B_c$ meson into $S$-wave charmonium within the nonrelativistic QCD effective theory and obtain the next-to-leading order relativistic corrections to the form factors, where both the $B_c$ meson and the…

High Energy Physics - Phenomenology · Physics 2017-05-24 Ruilin Zhu , Yan Ma , Xin-Ling Han , Zhen-Jun Xiao

We calculate the mass splittings within the heavy baryon isospin multiplets \Sigma_{c(b)} and \Xi_{c(b)}' in chiral perturbation theory to leading one-loop order. The pattern of the mass splittings in the \Sigma_c iso-triplet, which is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

Semileptonic decay of the $B_c$ meson is studied in the heavy quark limit. The six possible form factors for $B_c \rightarrow B_s (B^0),B_s^* (B^{*0})$ semileptonic decay are determined by two invariant functions. Only one of these…

High Energy Physics - Phenomenology · Physics 2016-09-01 Elizabeth Jenkins , Michael Luke , Aneesh V. Manohar , Martin J. Savage

We determine the masses and decay constants of the pseudoscalar mesons Bs and Bc, and also the masses of the vector mesons Bs^* and Bc^*, in quenched lattice QCD with exact chiral symmetry. For 100 gauge configurations generated with…

High Energy Physics - Lattice · Physics 2011-02-16 TWQCD Collaboration , Ting-Wai Chiu , Tung-Han Hsieh

Recent theoretical and experimental improvements in the determination of charm and bottom quark masses are discussed. The final results, $m_c(3 \text{GeV})=986(13) $MeV and $m_b(m_b)=4163(16) $MeV represent, together with a closely related…

High Energy Physics - Phenomenology · Physics 2010-01-29 Johann H. Kuhn

First results are obtained for B mesons using a heavy propagator calculated using NRQCD, and a light Wilson propagator. Results from 13 quenched configurations of size 16^3 x 48 at \beta = 6.0 give a value for f_{B} of less than 200 Mev and…

High Energy Physics - Lattice · Physics 2012-08-27 UKQCD Collaboration

We explore the application and usefulness of the heavy quark symmetry to describe the weak decays of hadrons (mesons and baryons) containing two heavy quarks. Firstly, we address the internal dynamics of a heavy-heavy bound system with the…

High Energy Physics - Phenomenology · Physics 2016-09-01 Miguel Angel Sanchis-Lozano

We calculate the B-meson decay constants f_B, f_Bs, and their ratio in unquenched lattice QCD using domain-wall light quarks and relativistic b-quarks. We use gauge-field ensembles generated by the RBC and UKQCD collaborations using the…

We determine the inclusive B --> Xc l nu branching fraction, the CKM matrix element |Vcb|, and other heavy-quark parameters from a simultaneous fit to moments of the hadronic-mass and lepton-energy distributions in semileptonic B-meson…

High Energy Physics - Experiment · Physics 2009-09-29 BABAR Collaboration , B. Aubert , R. Barate , D. Boutigny

Lattice QCD calculations of hadronic matrix elements allow one to draw inferences about quark flavor interactions from measurements of hadron decays. Within the context of the Standard Model, the magnitude of the charm-bottom quark coupling…

High Energy Physics - Lattice · Physics 2017-04-04 Matthew Wingate

We reanalyze the perturbative QCD (pQCD) corrections to quarkonium QCD sum rules and extract the heavy quark masses $\overline{m}_{q}(\overline{m}_{q})$ ($q=c,b$). At present, the pQCD corrections to the correlation functions of two…

High Energy Physics - Phenomenology · Physics 2026-05-11 Qing Yu , Hua Zhou , Xing-Gang Wu

By using a single formalism to handle charm, strange and light valence quarks in full lattice QCD for the first time, we are able to determine ratios of quark masses to 1%. For $m_c/m_s$ we obtain 11.85(16), an order of magnitude more…

High Energy Physics - Phenomenology · Physics 2010-04-06 C. T. H. Davies , C. McNeile , K. Y. Wong , E. Follana , R. Horgan , K. Hornbostel , G. P. Lepage , J. Shigemitsu , H. Trottier

We calculate the radiative corrections to the nonleptonic inclusive B decay mode $b\to c ud$ taking into account the charm quark mass. The corrections increase the decay rate by (4--8)\%, depending on the renormalization point. Using these…

High Energy Physics - Phenomenology · Physics 2009-10-28 P. Ball

We present a study of the B spectrum performed in the framework of Heavy Quark Effective Theory expanded to next-to-leading order in 1/m and non-perturbative in the strong coupling. Our analyses have been performed on Nf=2 lattice gauge…

We calculate the semileptonic branching ratio and the charm counting of inclusive $B$ meson decays using the perturbative QCD formalism. For the nonleptonic decays, we employ the modified factorization theorem, in which Wilson coefficients…

High Energy Physics - Phenomenology · Physics 2011-01-25 Chia-Hung V. Chang , Darwin Chang , We-Fu Chang , Hsiang-nan Li , Hoi-Lai Yu

A method for computing electromagnetic properties of hadrons in lattice QCD is described and preliminary numerical results are presented. The electromagnetic field is introduced dynamically, using a noncompact formulation. Employing…

High Energy Physics - Lattice · Physics 2009-10-28 A. Duncan , E. Eichten , H. Thacker

We consider flavor breaking in the the octet and decuplet baryon masses at second order in large-$N$ chiral perturbation theory, where $N$ is the number of QCD colors. We assume that $1/N \sim 1/N_F \sim m_s / \Lambda \gg m_{u,d}/\Lambda,…

High Energy Physics - Phenomenology · Physics 2014-11-17 Paulo F. Bedaque , Markus A. Luty
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