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We consider the nonleptonic B decays $ B \to D^{(*)} D_s(2317)$ and $ B \to D^{(*)} D_s(2460)$, involving the newly discovered $D_s(2317)$ and the $D_s(2460)$ states. We find that experiments indicate disagreement with model calculations of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alakabha Datta , Patrick J. O'Donnell

The \Lambda_c(2940)^+ baryon is studied in a constituent quark model as a molecular state composed by nucleons and D^* mesons. A bound state with the right binding energy is found for the J^\pi=3/2^- channel. The partial widths…

High Energy Physics - Phenomenology · Physics 2015-06-11 P. G. Ortega , D. R. Entem , F. Fernández

Motivated by the recent observations of exotic open-charm tetraquark candidates \(T^a_{c\bar{s}0}(2900)^{++}\) and \(T^a_{c\bar{s}0}(2900)^{0}\), we systematically calculate the mass spectra of \([cq][\bar{s}\bar{q}]\) tetraquarks within a…

High Energy Physics - Phenomenology · Physics 2026-02-13 Zhi-Yuan Chen , Zhe-Hao Cao , You-You Lin , Ji-Ying Wang , Ailin Zhang

The new members of the charm-strange family $D_{sJ}^{*}(2317)$, $D_{sJ}(2460)$ and $D_s(2632)$, which have the surprising properties, are challenging the present models. Many theoretical interpretations have been devoted to this issue. Most…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. X. Zhang , W. L. Wang , Y. -B. Dai , Z. Y. Zhang

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

We investigate the electromagnetic properties of the axial-vector molecular states $D^* K$, $DK^*$, $B^* K$, and $BK^*$, which are used to model the charmed states $D_{s1}^{+}(2460)$, $D_{s1}^{+}(2536)$, and their bottom partners with…

High Energy Physics - Phenomenology · Physics 2025-11-20 U. Özdem

Many hadronic states observed since 2003, especially for the positive-parity charm-strange states $D_{s0}^\ast (2317)$ and $D_{s1}(2460)$, do not conform with the conventional quark model expectations and raise various puzzles in charm…

High Energy Physics - Phenomenology · Physics 2018-09-25 Meng-Lin Du

Mesons with masses below their lowest OZI-allowed strong-decay thresholds have very small widths. Thus, it is usually believed that they can be safely treated as pure quark-antiquark bound states in spectroscopy models. However, unitarised…

High Energy Physics - Phenomenology · Physics 2017-12-14 George Rupp , Eef van Beveren

We determine the quark mass dependence - light and heavy - of the $D_{s0}^*(2317)$ and $D_{s1}(2460)$ properties, such as, mass, coupling to $DK$, scattering lengths and compositeness, from a global analysis of $DK$ energy levels from LQCD.…

High Energy Physics - Phenomenology · Physics 2025-06-23 F. Gil-Domínguez , R. Molina

The observation of the D_{sJ}^*(2317), D_{sJ}(2460), and SELEX D^*_{sJ}(2632) states with properties differing considerably from what was expected has led to a renewed interest in hadron spectroscopy. In addition to these states,…

High Energy Physics - Phenomenology · Physics 2009-11-10 Stephen Godfrey

This paper presents the first study of mesons with a quark and an antiquark with different and finite masses, in a simple confining and chiral invariant quark-antiquark interaction, leading to spontaneous chiral symmetry breaking and to…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Bicudo

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

The resonances $D_{sJ}^*$(2317) and $D_{sJ}$(2460) which are considered to be the $(0^+,1^+)$ doublet composed of charm and strange quarks have been discovered recently. Using the method of Rosner which is based on the factorization…

High Energy Physics - Phenomenology · Physics 2011-07-19 Dae Sung Hwang , Do-Won Kim

We study the possible heavy molecular states composed of a pair of charm mesons in the H and S doublets. Since the P-wave charm-strange mesons $D_{s0}(2317)$ and $D_{s1}(2460)$ are extremely narrow, the future experimental observation of…

High Energy Physics - Phenomenology · Physics 2010-11-24 Lei-Lei Shen , Xiao-Lin Chen , Zhi-Gang Luo , Peng-Zhi Huang , Shi-Lin Zhu , Peng-Fei Yu , Xiang Liu

We study the decay widths of the narrow resonances $D_{sj}^*(2317)$ and $D_{sj}(2460)$ in the chiral quark model, together with the well-known $D^\ast$ and $D_s^*$ mesons. All the parameters in our calculation are taken from Godfrey and…

High Energy Physics - Phenomenology · Physics 2010-11-15 Feng-Lin Wang , Xiao-Lin Chen , Da-Hai Lu , Shi-Lin Zhu , Wei-Zhen Deng

We perform a systematic study of the possible molecular states composed of a pair of heavy mesons such as $D\bar D$, $D^\ast\bar D$, $D^\ast \bar D^\ast$ in the framework of the meson exchange model. The exchanged mesons include the…

High Energy Physics - Phenomenology · Physics 2009-05-26 Xiang Liu , Zhi-Gang Luo , Yan-Rui Liu , Shi-Lin Zhu

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 narrow $D_{s0}^{\ast}$(2317) and broad $D_0^{\ast}$(2300-2400) charmed scalar mesons and their radial excitations are described in a coupled-channel quark model that also reproduces the properties of the light scalar nonet. All…

High Energy Physics - Phenomenology · Physics 2008-11-26 George Rupp , Eef van Beveren

Using the Fixed Center Approximation to Faddeev equations we have investigated the $DKK$ and $DK\bar{K}$ three-body systems, considering that the $DK$ dynamically generates, through its $I=0$ component, the $D^*_{s0}(2317)$ molecule.…

High Energy Physics - Phenomenology · Physics 2017-08-01 V. R. Debastiani , J. M. Dias , E. Oset

In this article, we take the point of view that the charmed scalar meson $D_{s0}(2317)$ be a tetraquark state and devote to calculate its mass within the framework of the QCD sum rules approach in the heavy quark limit. The numerical values…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-Gang Wang , Shao-Long Wan