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The conventional color-singlet model was challenged by the recent data on quarkonium production. Discrepancies in production rates were observed at the Tevatron, at LEP, and in fixed-target experiments. The newly advocated color-octet…

High Energy Physics - Phenomenology · Physics 2009-09-01 Kingman Cheung , Wai-Yee Keung , Tzu Chiang Yuan

In this work, we investigate the $\Upsilon(10753)\to\Upsilon(1^3D_J)\eta$ ($J=1,2,3$) processes, where the $\Upsilon(10753)$ is assigned as a conventional bottomonium under the $4S$-$3D$ mixing scheme. Our result shows that the concerned…

High Energy Physics - Phenomenology · Physics 2022-06-29 Yu-Shuai Li , Zi-Yue Bai , Xiang Liu

Properties of bottomonia (Upsilon, chi_b and Upsilon') in the Quark-Gluon Plasma (QGP) are investigated by assessing inelastic reaction rates and their interplay with open-bottom states (b-quarks or B-mesons) and color-screening. The latter…

High Energy Physics - Phenomenology · Physics 2008-11-26 L. Grandchamp , S. Lumpkins , D. Sun , H. van Hees , R. Rapp

Differential cross sections for eta photoproduction off protons have been measured at E_gamma = 1.6 - 2.4 GeV in the backward direction. A bump structure has been observed above 2.0 GeV in the total energy. No such bump is observed in cross…

In this work we evaluate the cross section of the process $e^+e^-\to J/\psi \eta_c$ at energy $\sqrt{s}\approx 10.6$ GeV in the Bethe-Salpeter formalism. To simplify our calculation, the heavy quark limit is employed. Without taking the…

High Energy Physics - Phenomenology · Physics 2008-04-08 Xin-Heng Guo , Hong-Wei Ke , Xue-Qian Li , Xing-Hua Wu

We compute the magnetic dipole transitions between low lying Heavy Quarkonium states in a model independent way. We use the weak-coupling version of the effective field theory named potential NRQCD with the static potential exactly…

High Energy Physics - Phenomenology · Physics 2014-11-26 Antonio Pineda , J. Segovia

Mechanism of di-pion transitions $nS\to n'S\pi\pi(n=3,2; n'=2,1)$ in bottomonium and charmonium is studied with the use of the chiral string-breaking Lagrangian allowing for the emission of any number of $\pi(K,\eta),$ and not containing…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yu. A. Simonov

The production of eta' mesons in photon- and hadron-induced reactions has been revisited in view of the recent additions of high-precision data to the world data base. Based on an effective Lagrangian approach, we have performed a combined…

Nuclear Theory · Physics 2015-03-20 F. Huang , H. Haberzettl , K. Nakayama

As double heavy quarkonia, charmonium and bottomonium are generally considered to have small relativistic corrections and can be treated using nonrelativistic models. However, this is not always the case. In this paper, we employ the…

High Energy Physics - Phenomenology · Physics 2026-03-03 Su-Yan Pe , Wei Li , Wen-Yuan Ke , Yi-Yi Rui , Qiang Li , Guo-Li Wang

Within the nonrelativistic quantum chromodynamics framework, we make a comprehensive study on the exclusive production of excited charmonium and bottomonium in $e^+e^-\to \gamma^*/Z^0 \to|(Q\bar{Q})[n]\rangle +\gamma$ ($Q=c$ or $b$ quarks)…

High Energy Physics - Phenomenology · Physics 2022-02-09 Qi-Li Liao , Jun Jiang , Peng-Cheng Lu , Gu Chen

We calculate the cross section for the production of $\eta$-mesons via \mbox{$\Delta N \to N N \eta$} in a relativistic One-Boson-Exchange-Model. Using this cross section we then determine the probability for the production of an…

Nuclear Theory · Physics 2009-10-28 W. Peters , U. Mosel , A. Engel

We study the Upsilon(3S,2S)->eta Upsilon(1S) and Upsilon(3S,2S)->pi+pi- Upsilon(1S) transitions with 122 million Upsilon(3S) and 100 million Upsilon(2S) mesons collected by the BaBar detector at the PEP-II asymmetric energy e+e- collider.…

High Energy Physics - Experiment · Physics 2013-05-29 The BABAR Collaboration , J. P. Lees , others

We compute hadronic transitions between heavy quarkonium states with two, or one, pion/eta particles in the final state. We use the multipole expansion but not the twist expansion. The latter cannot be justified for the energy release of…

High Energy Physics - Phenomenology · Physics 2019-09-19 Antonio Pineda , Jaume Tarrús Castellà

In this paper, the production rates of quarkonia eta_c, J/psi, eta_b, Upsilon, B_c and B_c^* through W boson decay at the LHC are calculated, at the leading order in both the QCD coupling constant and in v, the typical velocity of the heavy…

High Energy Physics - Phenomenology · Physics 2015-05-27 Cong-Feng Qiao , Li-Ping Sun , De-Shan Yang , Rui-Lin Zhu

For the flavor-singlet heavy quark system of bottomonia, we compute the masses of the ground state mesons in four different channels, namely, pseudo-scalar ($\eta_{b}(1S)$), vector ($\Upsilon(1S)$), scalar ($\chi_{b_0}(1P)$) and axial…

Nuclear Theory · Physics 2018-09-26 K. Raya , M. A. Bedolla , J. J. Cobos-Martínez , A. Bashir

We study exclusive charmonium and bottomonium production in ultra-peripheral heavy-ion collisions and electron-ion collisions within the dipole picture. We employ heavy quarkonium light-front wavefunctions obtained within the basis…

Nuclear Theory · Physics 2019-08-28 Guangyao Chen , Yang Li , Kirill Tuchin , James Vary

In the paper, the inclusive production of heavy quarkonium $\eta_Q$ ($Q=b$ or $c$) via $Z$ boson decays within the framework of nonrelativistic QCD effective theory are studied. The contributions from the leading color-singlet and…

High Energy Physics - Phenomenology · Physics 2021-10-04 Xu-Chang Zheng , Chao-Hsi Chang , Xing-Gang Wu , Xu-Dong Huang , Guang-Yu Wang

The near-threshold photo-productions of heavy quarkonia are important ways to test the QCD-inspired models and to constrain the gluon distribution of nucleon in the large x region. Investigating the various models, we choose a photon-gluon…

High Energy Physics - Phenomenology · Physics 2020-04-02 Yu Xu , Yaping Xie , Rong Wang , Xurong Chen

I discuss exclusive production of the $\eta'$, $J/\psi$, and $\chi_c(0^+)$ mesons in $pp$ and $p \bar p$ collisions at high energies. QCD diffractive mechanisms as well as nondiffractive mechanisms are discussed. Different unintegrated…

Nuclear Theory · Physics 2008-05-06 Antoni Szczurek

We have searched for the bottomonium eta_b(1S) via the hindered magnetic dipole (M1) photon transition Upsilon(3S) -> gamma eta_b(1S). No evidence for such a transition is found in the data sample of 4.7 x 10^6 Upsilon(3S)'s collected with…

High Energy Physics - Experiment · Physics 2007-05-23 A. H. Mahmood , CLEO Collaboration