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Related papers: Annihilation Rates of Heavy $1^{--}$ S-wave Quarko…

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We calculate the annihilation decay rates of the $^3D_2(2^{--})$ and $^3D_3(3^{--})$ charmonia and bottomonia by using the instantaneous Bethe-Salpeter method. The wave functions of states with quantum numbers $J^{PC}=2^{--}$ and $3^{--}$…

High Energy Physics - Phenomenology · Physics 2021-11-05 Tianhong Wang , Hui-Feng Fu , Yue Jiang , Qiang Li , Guo-Li Wang

Two-photon and two-gluon annihilation rates of P-wave scalar charmonium and bottomonium up to third radial excited states are estimated in the relativistic Salpeter method. We solved the full Salpeter equation with a well defined…

High Energy Physics - Phenomenology · Physics 2008-11-26 Guo-Li Wang

Two-photon annihilation rates of $2^+$ tensor charmonium and bottomonium up to third radial excited states are estimated in the relativistic Salpeter method. Full Salpeter equation for $2^+$ tensor state is solved with a well defined…

High Energy Physics - Phenomenology · Physics 2009-12-10 Guo-Li Wang

Two-photon and two-gluon annihilation rates of $\eta_c$, $\eta'_c$, $\eta_b$ and $\eta'_b$ are estimated in the relativistic Salpeter method. By solving the full Salpeter equation with a well defined relativistic wave function, we estimate…

High Energy Physics - Phenomenology · Physics 2011-07-19 C. S. Kim , Taekoon Lee , Guo-Li Wang

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 revisit the heavy quarkonium leptonic decays $\psi(nS) \to \ell^+\ell^-$ and $\Upsilon(nS) \to \ell^+\ell^-$ using the Bethe-Salpeter method. The emphasis is on the relativistic correction. For the $\psi(1S-5S)$ decays, the relativistic…

High Energy Physics - Phenomenology · Physics 2020-06-11 Guo-Li Wang , Xing-Gang Wu

We show that perturbation theory may give reasonable numbers for the decays of the bottomonium and charmonium ground states to $e^+e^-$ and to $\gamma\gamma$. To reach this conclusion it is important to perform the resummation of logs. In…

High Energy Physics - Phenomenology · Physics 2007-05-23 Antonio Pineda

We estimate the decay rates of $\eta_c\rightarrow 2\gamma$, $\eta_c'\rightarrow 2\gamma$, and $J/\psi\rightarrow e^+ e^-$, $\psi^\prime\rightarrow e^+e^-$, by taking into account both relativistic and QCD radiative corrections. The decay…

High Energy Physics - Phenomenology · Physics 2009-10-28 Kuang-Ta Chao , Han-Wen Huang , Jing-Hua Liu , Jian Tang

Within the nonrelativistic QCD (NRQCD) factorization framework, we compute the ${\mathcal O}(\alpha_s v^2)$ corrections to the hadronic decay rate of vector quarkonia, exemplified by $J/\psi$ and $\Upsilon$. Setting both the renormalization…

High Energy Physics - Phenomenology · Physics 2020-11-25 Wen-Long Sang , Feng Feng , Yu Jia

In the framework of instantaneous Bethe-Salpeter equation, according to the $J ^ {PC}$ of quarkonia, we find that their wave functions all contain multiple partial waves, rather than pure waves. In the radiative electromagnetic transitions…

High Energy Physics - Phenomenology · Physics 2024-08-29 Su-Yan Pei , Wei Li , Tianhong Wang , Guo-Li Wang

The $1^1D_2 (c\bar c)$ state is the ground state of spin-singlet D-wave charmonia. Although it has not been found yet, the experimental data accumulate rapidly. This charmonium attracts more and more attention, especially when the BaBar…

High Energy Physics - Phenomenology · Physics 2016-01-05 Tianhong Wang , Guo-Li Wang , Wan-Li Ju , Yue Jiang

We present a calculation of the two-photon and two-gluon widths for the equal mass quarkonium states $^1S_0$, $^3P_0$ and $^3P_2$ of the charmonium and upsilon systems. The approach taken is based on using the full relativistic…

High Energy Physics - Phenomenology · Physics 2011-01-10 James T. Laverty , Stanley F. Radford , Wayne W. Repko

For radially excited heavy quarkonia $ V=\psi(2S) $ and $ \Upsilon(2S) $, the nodal structure of their wave function renders the three-gluon decay $ V\to ggg $ acutely sensitive to relativistic corrections, presenting a longstanding…

High Energy Physics - Phenomenology · Physics 2026-03-12 Chao-Jie Fan , Jun-Kang He

We analyze the relativistic corrections to annihilation rates of S-wave quarkonia within the framework of NRQCD. We show that order v^2 corrections can be expressed in terms of the heavy quark pole mass and the quarkonium mass. The ratio of…

High Energy Physics - Phenomenology · Physics 2010-11-19 Martin Gremm , Anton Kapustin

The decay constant for the vector state of $3S$-level in the heavy $(\bar b c)$-quarkonium is evaluated in the framework of sum rules for the mesonic currents. A scaling relation for the constants of vector quarkonia with different quark…

High Energy Physics - Phenomenology · Physics 2014-11-17 V. V. Kiselev

QCD running coupling constant $\alpha_s(m_c)$ and $\alpha_s(m_b)$ are determined from heavy quarkonia $c\overline{c}$ and $b\overline{b}$ decays. The decay rates of $V\rightarrow 3g$ and $V\rightarrow e^+ e^-$ for $V=J/\psi$ and $\Upsilon$…

High Energy Physics - Phenomenology · Physics 2011-01-27 K. T. Chao , H. W. Huang , Y. Q. Liu

We present new results for the suppression of high transverse momentum charmonium [$J/\psi, \psi(2S)$] and bottomonium [$\Upsilon(1S),\Upsilon(2S),\Upsilon(3S)$] states in Pb+Pb collisions at the Large Hadron Collider. Our theoretical…

High Energy Physics - Phenomenology · Physics 2018-04-04 Samuel Aronson , Evan Borras , Brunel Odegard , Rishi Sharma , Ivan Vitev

We determine the leading-order nonrelativistic quantum chromodynamics (NRQCD) matrix element < O_1 >_Upsilon and the ratio < q^2>_Upsilon, for Upsilon=Upsilon(nS) with n=1, 2, and 3 by comparing the measured values for Gamma[Upsilon -> e^+…

High Energy Physics - Phenomenology · Physics 2011-02-16 Hee Sok Chung , Jungil Lee , Chaehyun Yu

We report evidence for the ground state of bottomonium, eta_b(1S), in the radiative decay Upsilon(3S) --> gamma eta_b in e^+e^- annihilation data taken with the CLEO III detector. Using 6 million Upsilon(3S) decays, and assuming…

We compute the decay rates for the processes $Z\to V+\gamma$, where $Z$ is the $Z$ boson, $\gamma$ is the photon, and $V$ is one of the vector quarkonia $J/\psi$ or $\Upsilon(nS)$, with $n=1$, $2$, or $3$. Our computations include…

High Energy Physics - Phenomenology · Physics 2018-01-24 Geoffrey T. Bodwin , Hee Sok Chung , June-Haak Ee , Jungil Lee
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