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Related papers: $X_0(2866)$ as a $D^*\bar{K}^*$ molecular state

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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 revisit, improve and complete some recent estimates of the $0^{+}$ and $1^-$ open charm $(\bar c \bar d)(us)$ tetraquarks and the corresponding molecules masses and decay constants from QCD spectral sum rules (QSSR) by using QCD Laplace…

High Energy Physics - Phenomenology · Physics 2020-12-29 R. M. Albuquerque , S. Narison , D. Rabetiarivony , G. Randriamanatrika

The spectrum of the $c qq$ baryons contains a few states whose nature is not clearly a three-quark composite and which might have a sizable baryon-meson component. Examples include the $\Sigma_c(2800)$ or the $\Lambda_c(2940)$. Here we…

High Energy Physics - Phenomenology · Physics 2024-10-22 Mao-Jun Yan , Fang-Zheng Peng , Manuel Pavon Valderrama

We have studied the meson-baryon $S-$wave interaction, using coupled channels, in the isoscalar hidden-charm strange sector and $J^P = 1/2^-,3/2^-$ and $5/2^-$. We impose constraints of heavy quark spin symmetry in the interaction and…

High Energy Physics - Phenomenology · Physics 2020-01-09 C. W. Xiao , J. Nieves , E. Oset

We have calculated the mass spectra for the $\bar{D}_s^{(*)}D^{(*)}$ molecular states and $sc\bar q\bar c$ tetraquark states with $J^P=0^+, 1^+, 2^+$. The masses of the axial-vector $\bar{D}_sD^{*}$, $\bar{D}_s^{*}D$ molecular states and…

High Energy Physics - Phenomenology · Physics 2021-09-02 Qi-Nan Wang , Wei Chen , Hua-Xing Chen

Using the vector-exchange interaction in the local hidden gauge approach, which in the light quark sector generates the chiral Lagrangian, and has produced realistic results for $\Omega_c, \Xi_c, \Xi_b$ and the hidden charm pentaquark…

High Energy Physics - Phenomenology · Physics 2020-08-26 J. M. Dias , Qi-Xin Yu , Wei-Hong Liang , Zhi-Feng Sun , Ju-Jun Xie , E. Oset

We study exotic mesons with double charm and bottom flavor, whose quark configuration is \bar{Q}\bar{Q}qq. This quark configuration has no annihilation process of quark and antiquark, and hence is a genuinely exotic states. We take a…

High Energy Physics - Phenomenology · Physics 2013-05-30 Shunsuke Ohkoda , Yasuhiro Yamaguchi , Shigehiro Yasui , Kazutaka Sudoh , Atsushi Hosaka

Recently LHCb predicted spin 1 and spin 3 states D* s1(2860) and D* s3(2860) which are studied through their strong decays, and are assigned to fit the 13D1and 13D3 states in the charm spectroscopy. In this paper,using the heavy quark…

High Energy Physics - Phenomenology · Physics 2016-11-07 Pallavi Gupta , Alka Upadhyay

The doubly charmed tetraquark $T_{cc}$ has been reported by the LHCb experiment in 2022, and a lot of theoretical studies has been conducted. The small binding energy measured from $D^{\ast + }D^0$ threshold indicates that $T_{cc}$ is a…

High Energy Physics - Phenomenology · Physics 2026-03-16 Manato Sakai , Yasuhiro Yamaguchi

We discuss a possible interpretation of the open charm mesons $D_{s0}^*(2317)$, $D_{s1}(2460)$ and the hidden charm mesons X(3872), Y(3940) and Y(4140) as hadron molecules. Using a phenomenological Lagrangian approach we review the strong…

High Energy Physics - Phenomenology · Physics 2010-01-13 Thomas Gutsche , Tanja Branz , Amand Faessler , Ian Woo Lee , Valery E. Lyubovitskij

We analyze two recent reactions of Belle, producing $D\bar D$ and $D\bar D^*$ states that have an enhancement of the invariant $D\bar D$, $D\bar D^*$ mass distribution close to threshold, from the point of view that they might be indicative…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Gamermann , E. Oset

In this talk we summarize our latest results on the study of three-body systems with explicit/hidden charm and with strangeness. In particular, we focus on the $K D D $ and $K D\bar D^*$ systems, where a charm $+2$, isospin $1/2$ and…

High Energy Physics - Phenomenology · Physics 2019-12-05 Xiu-Lei Ren , Brenda B. Malabarba , L. S. Geng , K. P. Khemchandani , A. Martinez Torres

In the $B^+\to D^+ D^-K^+$ decay, LHCb has reported the observation of the open-charm exotic states $X_{0,1}^0\equiv X_{0,1}(2900)^0$ with four different quark flavors~$(ud\bar s \bar c)$, where the subscripts (0,1) denote the spins. To…

High Energy Physics - Phenomenology · Physics 2021-08-24 Yu-Kuo Hsiao , Yao Yu

The $\Lambda_c(2940)$, an open-charm baryon discovered in 2006, has sparked interest due to its ``low mass puzzle'', paralleling the $X(3872)$ in the charmoniumlike sector. Both states challenge conventional hadronic interpretations, with…

High Energy Physics - Phenomenology · Physics 2025-09-19 Ping Chen , Zi-Le Zhang , Yu Zhuge

This contribution to the SQM2024 conference covers the molecular hypothesis for the internal structure of some open and hidden charm states. The use of effective theories that incorporate heavy-quark spin symmetry, combined with…

High Energy Physics - Phenomenology · Physics 2024-10-02 Juan M. Torres-Rincon

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

Two charm-strange mesons, the $D_{s1}^*(2710)$ and the $D_{sJ}^*(2860)$, have recently been observed by several experiments. There has been speculation in the literature that the $D_{s1}^*(2710)$ is the $2^3S_1(c\bar{s})$ state and the…

High Energy Physics - Phenomenology · Physics 2014-04-23 Stephen Godfrey , Ian T. Jardine

This study investigates the three-body decay process $B^+ \to D^{*+} D^- K^+$, aiming to explore the possible origins of $T^*_{\bar{c}\bar{s}0}(2870)^0$ and $\chi_{c1}(3872)$ as intermediate states. Within the molecular state framework,…

High Energy Physics - Phenomenology · Physics 2025-08-20 Zuo-Ming Ding , Qi Huang , Jun He

We study three newly observed D(2550), D(2610), and D(2760) by the BaBar Collaboration utilizing the mass spectra and investigating the strong decays. Our calculation indicates that D(2610) is an admixture of $2^3S_1$ and $1^3D_1$ with…

High Energy Physics - Phenomenology · Physics 2010-12-02 Zhi-Feng Sun , Jie-Sheng Yu , Xiang Liu , Takayuki Matsuki

We perform a systematic study of the possible molecular states composed of a pair of heavy mesons such as $D^{(*)}D^{(*)}$, $D^{(*)}\bar{D}^{(*)}$ in the framework of the one-boson-exchange model. The exchanged bosons include the…

High Energy Physics - Phenomenology · Physics 2025-08-19 Jia-Liang Lu , Mao Song , Peng Wang , Jian-You Guo , Gang Li , Xuan Luo
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