Analyzing the semileptonic and nonleptonic Bc → J/ψ, ηc decays

被引:1
作者
Biswas, Aritra [1 ,2 ]
Nandi, Soumitra [3 ]
Sahoo, Shantanu [3 ]
机构
[1] Univ Autonoma Barcelona, Barcelona 08193, Spain
[2] Barcelona Inst Sci & Technol, Inst Fis Altes Energies IFAE, Campus UAB, Bellaterra 08193, Barcelona, Spain
[3] Indian Inst Technol Guwahati, North Guwahati 781039, Assam, India
关键词
Bottom Quarks; Semi-Leptonic Decays; FORM-FACTORS; SUM-RULES; MESON; QCD;
D O I
10.1007/JHEP01(2025)198
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
This study focuses on the decay of the Bc meson to S-wave charmonia. Starting with lattice inputs on Bc -> J/psi form factors, we have obtained the Bc -> eta c form factors using heavy quark spin symmetry (HQSS) relations between the associated form factors after parametrizing and extracting the possible symmetry breaking corrections. Using the q2 shapes of these form factors, we have computed the branching fractions B\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{B} $$\end{document}(Bc-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}_c<^>{-} $$\end{document} -> eta c & ell;-nu<overline>\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \overline{\nu} $$\end{document}) (with & ell; = tau, mu(e)) and the decay rate distributions and have predicted the Standard model estimate for the observable R(eta c) = Gamma(Bc-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}_c<^>{-} $$\end{document} -> eta c tau-nu<overline>\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \overline{\nu} $$\end{document})/Gamma(Bc-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {B}_c<^>{-} $$\end{document}-> eta c mu-nu<overline>\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \overline{\nu} $$\end{document}) = 0.310 +/- 0.042. In addition, we have estimated the radial wave functions psi BcR\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\psi}_{B_c}<^>R $$\end{document} (0), psi J/psi R\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\psi}_{J/\psi}<^>R $$\end{document} (0) and psi eta cR\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\psi}_{\eta_c}<^>R $$\end{document} (0) at small Bc J/psi eta c quark-antiquark distances from the available information on the form factors from lattice, the lattice inputs on the decay constants fJ/psi, f eta c\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {f}_{\eta_c} $$\end{document}, fBc\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {f}_{B_c} $$\end{document} and experimental data on radiative and rare decays of the J/psi and eta c mesons. To do so, we choose the theory framework of non-relativistic QCD (NRQCD) effective theory. Using our results, we have predicted the branching fractions of a few non-leptonic decays of Bc -> J/psi or eta c and other light mesons. We have also updated the numerical estimates of the cross sections sigma(e+e- -> J/psi eta c, eta c gamma) and predicted the branching fractions of Z boson decays to either J/psi or eta c final states or both.
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