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Related papers: Heavy quark spin selection rules in meson-antimeso…

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With a quark level interaction, we give a unified description of the loosely bound molecular systems composed of the heavy flavor hadrons $(\bar{D},\bar{D}^*)$, $(\Lambda_c, \Sigma_c, \Sigma_c^*)$, and $(\Xi_c, \Xi_c^\prime,\Xi_c^*)$. Using…

High Energy Physics - Phenomenology · Physics 2022-07-13 Kan Chen , Rui Chen , Lu Meng , Bo Wang , Shi-Lin Zhu

We present recent results in semileptonic and non-leptonic exclusive $B_c$ decays to charmonium states both in $S$-wave, $J/\psi$ and $\eta_c$, and in $P$-wave, $\chi_{cJ}$ and $h_c$. The analysis, based on the heavy quark spin symmetry…

High Energy Physics - Phenomenology · Physics 2023-11-10 Nicola Losacco

The binding system of a hadron and a nucleus is a topic of great interest for investigating the hadron properties. In the heavy-flavor region, the attraction between a $P(=\bar{D},B)$ meson and a nucleon $N$ can appear, where the $PN-P^\ast…

Nuclear Theory · Physics 2019-08-14 Yasuhiro Yamaguchi , Shigehiro Yasui

We discuss the possible existence of exotic dibaryons with a heavy antiquark, being realized three-body systems, Dbar^(*)NN and B^(*)NN. These are genuinely exotic states with no quark-antiquark annihilation. We consider the heavy quark…

Nuclear Theory · Physics 2019-08-14 Yasuhiro Yamaguchi , Shigehiro Yasui , Atsushi Hosaka

Identifying a zero-range exchange of vector mesons as the driving force for the s-wave scattering of pseudo-scalar mesons off the baryon ground states, a rich spectrum of molecules is formed. We argue that chiral symmetry and large-$N_c$…

High Energy Physics - Phenomenology · Physics 2017-08-23 M. F. M. Lutz , J. Hofmann

The interaction of the charmed baryon and the anticharmed meson is assumed to be realized by exchanging a scalar meson of $f_0(500)$, and then these systems are studied by solving the Schrodinger equation, respectively. When the pentaquarks…

High Energy Physics - Phenomenology · Physics 2025-07-01 Bao-Xi Sun

It is suggested that the recently reported charged charmoniumlike resonance $Z_c(4100)$ and the previously observed $Z_c(4200)$ are two states of hadrocharmonium, related by the charm quark spin symmetry in the same way as the lowest…

High Energy Physics - Phenomenology · Physics 2018-12-05 M. B. Voloshin

In present work, we systematically calculate the mass spectra of open charm and bottom tetraquarks $q q\bar q \bar Q$ within an extended relativized quark model. The four-body relativized Hamiltonians including the Coulomb potential,…

High Energy Physics - Phenomenology · Physics 2020-11-04 Qi-Fang Lü , Dian-Yong Chen , Yu-Bing Dong

We investigated systematically whether the S-wave ($\bar{Q}q$) meson and the ($Q\bar{q}$) meson may form S-wave bound states in a chiral SU(3) quark model by solving the resonating group method equation. Here $Q=c$ or $b$ and $q=u$, $d$ or…

High Energy Physics - Phenomenology · Physics 2009-08-20 Yan-Rui Liu , Zong-Ye Zhang

Multiquark systems appear less frequently than mesons and baryons despite the enormous world-wide experimental effort that has been made during the last two decades. In this work, we will propose a possible explanation for that fact,…

High Energy Physics - Phenomenology · Physics 2024-03-25 M. C. Gordillo , J. Segovia

We present the first calculation of tensor and axial-tensor mesons with total spin $J\geq2$ within the Covariant Spectator Theory. We employ a refined quark-antiquark interaction kernel that incorporates the momentum dependence of the…

Nuclear Theory · Physics 2026-04-07 Elmar P. Biernat , Alfred Stadler

Stimulated by the observation of $\Lambda_c(2910)^+$ by the Belle Collaboration, the $S$-wave $qqq\bar{q}c~(q=u~\text{or}~d)$ pentaquark systems with $I$ = 0, $J^P$ = $\frac{1}{2}^-,~\frac{3}{2}^- and~\frac{5}{2}^-$ are investigated in the…

High Energy Physics - Phenomenology · Physics 2022-11-23 Ye Yan , Xiaohuang Hu , Yuheng Wu , Hongxia Huang , Jialun Ping , Youchang Yang

We investigate the possible deuteron-like molecules composed of a pair of charmed spin-$\frac{3}{2}$ baryons, or one charmed baryon and one charmed antibaryon within the one-boson-exchange (OBE) model. For the spin singlet and triplet…

High Energy Physics - Phenomenology · Physics 2019-03-27 Bin Yang , Lu Meng , Shi-Lin Zhu

We develop a moment QCD sum rule method augmented by fundamental inequalities to study the existence of exotic doubly hidden-charm/bottom tetraquark states made of four heavy quarks. Using the compact diquark-antidiquark configuration, we…

High Energy Physics - Phenomenology · Physics 2017-09-08 Wei Chen , Hua-Xing Chen , Xiang Liu , T. G. Steele , Shi-Lin Zhu

We consider the recently suggested model for some resonances near the open charm threshold as bound states of charmonium inside excited light mesons. It is argued in the soft-wall holographic model of QCD that such states of heavy…

High Energy Physics - Theory · Physics 2009-01-16 S. Dubynskiy , A. Gorsky , M. B. Voloshin

Very recently, the LHCb Collaboration reported a fully charmed tetraquark state $X(6900)$ in the invariant mass spectrum of $J/\psi$ pairs. If one $J/\psi$ meson is replaced with a fully charmed baryon, we obtain a fully charmed pentaquark…

High Energy Physics - Phenomenology · Physics 2021-04-13 Hong-Tao An , Kan Chen , Zhan-Wei Liu , Xiang Liu

The properties of pentaquarks containing a heavy anti-quark and strange quarks are studied in the bound state picture. In the flavor SU(3) limit, there are many pentaquark states with the same binding energy. When the SU(3) symmetry…

High Energy Physics - Phenomenology · Physics 2009-10-28 Chi-Keung Chow

In this work, an Effective Field Theory (EFT) incorporating light SU(3)-flavour and heavy quark spin symmetry is used to describe charmed meson-antimeson bound states. At Lowest Order (LO), this means that only contact range interactions…

High Energy Physics - Phenomenology · Physics 2013-09-30 C. Hidalgo-Duque , J. Nieves , M. Pavón Valderrama

We present RBC heavy-light meson spectroscopy with quenched DBW2 gauge configurations at lattice cutoff of about 3 GeV. Both heavy and light quarks are described by domain-wall fermions (DWF). The heavy quark mass ranges between 0.1 and 0.4…

High Energy Physics - Lattice · Physics 2019-08-15 HueyWen Lin , Shigemi Ohta , Norikazu Yamada

Using effective Lagrangians constrained by the heavy quark spin symmetry and chiral symmetry, for the light quarks, we analyze the $D^0 D^0\pi^+$, $\bar{D}^0D^0\pi^0$ and $D^0\bar{D}^{*0}$ invariant mass spectra. Performing a simultaneous…

High Energy Physics - Phenomenology · Physics 2024-12-30 Di Guo , Qin-He Yang , Ling-Yun Dai , A. P. Szczepaniak
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