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Related papers: Three body open flavor decays of higher vector cha…

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In the present work, we study the OZI-allowed three body open flavor decay properties of higher vector charmonium and bottomonium states with an extended quark pair creation model. For the bottomonium system, we get that (i) the $BB\pi$ and…

High Energy Physics - Phenomenology · Physics 2019-05-06 Xin-Zhen Weng , Li-Ye Xiao , Wei-Zhen Deng , Xiao-Lin Chen , Shi-Lin Zhu

We calculate the $\Lambda_c\bar{\Lambda}_c$ partial decay width of the excited vector charmonium states around 4.6 GeV with the quark pair creation model. We find that the partial decay width of the $\Lambda_c\bar{\Lambda}_c$ mode can reach…

High Energy Physics - Phenomenology · Physics 2018-08-15 Li-Ye Xiao , Xin-Zhen Weng , Qi-Fang Lü , Xian-Hui Zhong , Shi-Lin Zhu

We compute the in-medium partial decay widths of the bottomonium states to open bottom mesons ($B\bar B$) using a field theoretical model for composite hadrons with quark constituents. These decay widths are calculated by using the explicit…

Nuclear Theory · Physics 2017-08-29 Amruta Mishra , S. P. Misra

The open-charm strong decays of higher charmonium states up to the mass of the $6P$ multiplet are systematically studied in the $^3P_0$ model. The wave functions of the initial charmonium states are calculated in the linear potential (LP)…

High Energy Physics - Phenomenology · Physics 2018-08-16 Long-Cheng Gui , Long-Sheng Lu , Qi-Fang Lü , Xian-Hui Zhong , Qiang Zhao

Two- and three-body decays of $\Upsilon (5S)$ into $BB, $$ BB^*, $ $ B^*B^*,$ $ B_sB_s, $ $B_sB_s^*, $ $B_s^* B_s^*$ and $BB^*\pi, B^*B^*\pi$ are evaluated using the theory, developed earlier for dipion bottomonium transitions. The theory…

High Energy Physics - Phenomenology · Physics 2009-02-19 Yu. A. Simonov , A. I. Veselov

We analyze the decays of the theoretically predicted lowest bottomonium hybrid $H(1P)$ to open bottom two-meson states. We do it by embedding a quark pair creation model into the Born-Oppenheimer framework which allows for a unified,…

High Energy Physics - Phenomenology · Physics 2021-01-26 Roberto Bruschini , Pedro González

The full widths of the vector charmonium and bottomonium hybrid mesons $H_{ \mathrm{c}}$ and $H_{\mathrm{b}}$, characterized by the quantum numbers $1^{ \mathrm{--}}$, are determined by analyzing their dominant strong decay modes:…

High Energy Physics - Phenomenology · Physics 2025-10-30 B. Barsbay

A number of charmonium- and bottomonium-like meson states have been observed that have properties that do not match well to expectations for the simple quark-antiquark substructure suggested by the constituent quark model. Some of them are…

Nuclear Experiment · Physics 2013-07-17 Stephen Lars Olsen

The bottomonium spectrum is the perfect testing ground for the confining potential and unitarisation effects. The bottom quark is about three times heavier than the charm quark, so that $b\bar{b}$ systems probe primarily the short-range…

High Energy Physics - Phenomenology · Physics 2023-02-15 E. van Beveren , G. Rupp

Recent results from the CLEO experiment on decays and partial widths of various bottomonium and charmonium resonances are presented. New measurements of the di-electron partial widths for the 3 bound-state Upsilons and the J/psi are…

High Energy Physics - Experiment · Physics 2007-05-23 T. Ferguson

We systematically investigate the mass spectrum and two-body open-charm strong decays of charmonium states in a coupled-channel model where the $^3P_0$ quark-antiquark pair creation mechanism is employed. The results of masses, mass shifts,…

High Energy Physics - Phenomenology · Physics 2024-08-16 Zi-Long Man , Cheng-Rui Shu , Yan-Rui Liu , Hong Chen

We calculate the decay widths of the charmonium states, $J/\psi$, $\psi (3686)$ and $\psi(3770)$, to $D\bar D$ pairs, as well as the decay width of $D^* \rightarrow D\pi$, in isospin asymmetric strange hadronic matter, using a field…

Nuclear Theory · Physics 2015-08-27 Amruta Mishra , S. P. Misra , W. Greiner

Preliminary results are presented on a search for several exclusive charmless hadronic B decays, from data collected by the BABAR detector near the Upsilon(4S) resonance. These include two-body decay modes h^{+/-}h^{-/+} three-body decay…

High Energy Physics - Experiment · Physics 2007-05-23 Theresa J. Champion

The charmed B decays, $B\to DP, ~D^*P$ and $DV$, are re-analyzed using the latest experimental data, where $P$ and $V$ denote the pseudoscalar meson and vector meson, respectively. We perform global fits under the assumption of flavor SU(3)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Cheng-Wei Chiang , Eibun Senaha

Two-body open charm strong decays of the $2P$ and $3P$ charmonium states are studied by the Bethe-Salpeter(BS) method combined with the $^3P_0$ model. The wave functions and mass spectra of the $2P$ and $3P$ charmonium states are obtained…

High Energy Physics - Phenomenology · Physics 2022-10-12 Zhi-Hui Wang , Guo-Li Wang

In this paper we firstly study various model-independent bounds on lepton flavor violation (LFV) in processes of $J/\Psi$, $\Psi'$ and $\Upsilon$ two-body decays, then calculate their branch ratios % By using the constraints from other…

High Energy Physics - Phenomenology · Physics 2009-11-07 W. J. Huo , T. F. Feng , Y. C. Xing

The dielectron widths of $\Upsilon(nS) (n=1,...,7)$ and vector decay constants are calculated using the Relativistic String Hamiltonian with a universal interaction. For $\Upsilon(nS) (n=1,2,3)$ the dielectron widths and their ratios are…

High Energy Physics - Phenomenology · Physics 2010-02-17 A. M. Badalian , B. L. G. Bakker , I. V. Danilkin

In this work we study the radiative decay widths of vector quarkonia for the process of $J/\psi(nS)\rightarrow\eta_{c}(nS)\gamma$ and $\Upsilon(nS)\rightarrow\eta_{b}(nS)\gamma$ (for principal quantum numbers $n=1, 2, 3$) in the framework…

High Energy Physics - Phenomenology · Physics 2017-07-03 Hluf Negash , Shashank Bhatnagar

We study the partial decay widths of the charmonium states ($J/\psi$, $\psi(3686)$, $\psi(3770)$, $\chi_{c0}$, $\chi_{c2}$) to $D\bar D$ ($D^+D^-$ or $D^0\bar {D^0}$) in isospin asymmetric nuclear matter, in the presence of strong magnetic…

In the light of SU(3) flavor symmetry, the effective interaction Hamiltonian in tensor form is obtained by virtue of group representation theory. The strong and electromagnetic breaking effects are treated as a spurion octet so that the…

High Energy Physics - Phenomenology · Physics 2023-05-17 X. H. Mo , P. Wang , J. Y. Zhang
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