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Related papers: $X(4260)$ Revisited: A Coupled Channel Perspective

200 papers

Stimulated by the new evidence of Y(4274) observed in the $J/\psi\phi$ invariant mass spectrum, we first propose the charmonium-like state Y(4274) as the S-wave $D_s\bar{D}_{s0}(2317)+h.c.$ molecular state with $J^P=0^-$, which is supported…

High Energy Physics - Phenomenology · Physics 2015-03-17 Xiang Liu , Zhi-Gang Luo , Shi-Lin Zhu

We study the $Y(4260)$ production mechanism in $e^+e^-$ annihilations in the framework of hadronic molecules and investigate the consequence of such a picture in different decay channels. In the hadronic molecule picture the $Y(4260)$ is…

High Energy Physics - Phenomenology · Physics 2016-10-05 Wen Qin , Si-Run Xue , Qiang Zhao

Charmonium states can decay into pairs of $D$ and $\overline{D}$ mesons if their masses are above the allowed decay thresholds. In general $c\bar{c}$ states near threshold will also undergo mixing with $D\overline{D}$ molecular (or…

High Energy Physics - Lattice · Physics 2010-11-05 Gunnar Bali , Christian Ehmann

Experimentally observed excited strange charmed mesons $D_{s0}^*(2317)^{\pm}$, $D_{s1}(2460)^{\pm}$, $D_{s1}(2536)^{\pm}$, $D_{s2}^*(2573)^{\pm}$, $D_{s1}^*(2700)^{\pm}$, $D_{s1}^*(2860)^{\pm}$, $D_{s3}^*(2860)^{\pm}$, and…

High Energy Physics - Phenomenology · Physics 2021-06-29 Keval Gandhi , Ajay Kumar Rai , Takayuki Matsuki

In this paper, as a continuation of our previous work, we systematically study the mass spectra and OZI-allowed strong decays of the higher $3S$-, $2P$-, $2D$-, and $1F$-wave charmed and charmed-strange mesons within a unified unquenched…

High Energy Physics - Phenomenology · Physics 2026-05-19 Ru-Hui Ni , Jia-Jun Wu , Xian-Hui Zhong

The recent discovery of the $D_{s0}(2590)^+$ meson by the LHCb Collaboration has stimulated the analysis of meson-meson channels effects in the two-body quark-antiquark meson spectrum. This resonance, assigned to the radial excitation of…

High Energy Physics - Phenomenology · Physics 2022-03-09 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernandez

The heavy hadron spectrum is constrained by symmetries, of which two of the most important ones are heavy-quark spin and SU(3)-flavor symmetries. Here we argue that in the molecular picture the $Y(4230)$ (or $Y(4260)$), the $Y(4360)$ and…

High Energy Physics - Phenomenology · Physics 2023-01-06 Fang-Zheng Peng , Mao-Jun Yan , Mario Sánchez Sánchez , Manuel Pavon Valderrama

Inspired by the observation of the doubly charmed tetraquark state $T_{cc}^+$ at the LHCb Collaboration, we systematically study the $S$-wave interactions between a pair of charmed mesons ($D_{1},\,D_{2}^{\ast}$) in the $T$-doublet, where…

High Energy Physics - Phenomenology · Physics 2022-10-19 Fu-Lai Wang , Rui Chen , Xiang Liu

The spectrum of heavy-hadron molecules is constrained by heavy-quark symmetry in its different manifestations. Heavy-quark spin symmetry for instance connects the properties of the ground and excited states of heavy hadrons, while…

High Energy Physics - Phenomenology · Physics 2019-01-01 Ming-Zhu Liu , Fang-Zheng Peng , Mario Sanchez Sanchez , Manuel Pavon Valderrama

Results obtained by various experiments show that the $D_{s0}^{\ast}(2317)$ and $D_{s1}(2460)$ mesons are very narrow states located below the $DK$ and $D^{\ast}K$ thresholds, respectively. This is markedly in contrast with the expectations…

High Energy Physics - Phenomenology · Physics 2016-11-02 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernandez

The $D_{s0}^*(2317) D$ and $D_{s1}^*(2460) D^*$ heavy meson systems can exchange a kaon that is emitted in S-wave owing to the opposite intrinsic parity of the $D_{s0}^*$($D_{s1}^*$) and $D$($D^*$) mesons. As a consequence of the mass…

High Energy Physics - Phenomenology · Physics 2018-09-06 Mario Sanchez Sanchez , Li-Sheng Geng , Jun-Xu Lu , Tetsuo Hyodo , Manuel Pavon Valderrama

In this work, we investigate the decays of meson $X(4160)$ in the molecular frame. By using an effective lagrangian approach, we calculate the widths of $X(4160)\to J/\psi\phi$, $D^*\bar{D}^*$, $D^*\bar{D}$ and $D\bar{D}$ through the…

High Energy Physics - Phenomenology · Physics 2024-09-09 Ruitian Li , Dazhuang He , Xuan Luo , Hao Sun

The experimental observations of $\psi_2(3823)$ and $\psi_3(3842)$ make $D$ wave charmonia family abundant. In the present work, we investigate the hidden charm decay processes of spin triplets of the $D$-wave charmonia with the meson loop…

High Energy Physics - Phenomenology · Physics 2025-01-28 Xiao-Yu Qi , Qi Wu , Xing-Dao Guo , Dian-Yong Chen

A semi-relativistic potential model is adopted to calculate the mass spectra of charmed and charmed-strange meson states up to the $2D$ excitations.The strong decay properties are further analyzed with a chiral quark model by using the…

High Energy Physics - Phenomenology · Physics 2022-03-23 Ru-Hui Ni , Qi Li , Xian-Hui Zhong

In this work, we study the strong decay of the newly observed $P_{cs}(4459)$ assuming that it is a pure $\Xi_c\bar{D}^{*}$ molecular state. Considering two possible spin-parity assignments $J^P=1/2^{-}$ and $J^P=3/2^{-}$ the partial decay…

High Energy Physics - Phenomenology · Physics 2021-11-03 Feng Yang , Yin Huang , Hong Qiang Zhu

In this article, we study the strong decays of the newly observed charmed mesons $D(2550)$, $D(2600)$, $D(2750)$ and $D(2760)$ with the heavy quark effective theory in the leading order approximation, and tentatively identify the…

High Energy Physics - Phenomenology · Physics 2011-02-02 Zhi-Gang Wang

Different experiments have confirmed that the $D_{s0}^{\ast}(2317)$ and $D_{s1}(2460)$ mesons are very narrow states located, respectively, below the $DK$ and $D^{\ast}K$ thresholds. This is markedly in contrast with the expectations of…

High Energy Physics - Phenomenology · Physics 2016-09-08 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernández

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

It is suggested that the resonance $\psi(3770)$ may contain a sizeable ($O(10%)$ in terms of the probability weight factor) four-quark component with the up- and down- quarks and antiquarks in addition to the $c {\bar c}$ pair, which…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. B. Voloshin

In the present work, we adopt a relativistic constituent quark model to depict the charmed strange meson spectroscopy, in which $D_{s0}(2317)$ and $D_{s1}(2460)$ are considered as the $1^3P_0$ and $1P_1^\prime$ charmed strange mesons,…

High Energy Physics - Phenomenology · Physics 2020-04-22 Shao-Feng Chen , Jing Liu , Hai-Qing Zhou , Dian-Yong Chen