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Related papers: Molecular components in $\mathbf{D_{s0}^{\ast}(231…

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Within a theoretical framework that accounts for all open-charm mesons, including the $D_0^*(2308)$, the $D_{sJ}^*(2317)$ and the $D_{sJ}(2460)$, we analyze the structure and explore possible quantum number assignments for the…

High Energy Physics - Phenomenology · Physics 2009-02-05 J. Vijande , A. Valcarce , F. Fernandez

We conduct a theoretical study of the $ D_{s1}(2460) \to D_s \pi^+ \pi^- $ decay from the perspective that the $D_{s1}$ is a molecular state, built mostly from the $D^* K$ and $D_s^* \eta$ components. The $D^*$ and $D_s^*$ mesons are…

High Energy Physics - Phenomenology · Physics 2025-02-26 L. Roca , J. M. Dias , E. Oset

Searching for exotic multiquark states and elucidating their nature remains a central topic in understanding quantum chromodynamics--the underlying theory of the strong interaction. Two of the most studied such states are the charm-strange…

High Energy Physics - Phenomenology · Physics 2023-07-26 Tian-Chen Wu , Li-Sheng Geng

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 article, we take the point of view that the charmed mesons $D_{s0}(2317)$ and $D_{s1}(2460)$ with the spin-parity $0^+$ and $1^+$ respectively are the conventional $c\bar{s}$ states, and calculate the strong coupling constants…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-Gang Wang

Inspired by the observation of the $P_{cs} (4459)$ state by LHCb recently, we reexamine the results of the interaction of the $J/\psi \Lambda$ channel with its coupled channels, exploiting the coupled channel unitary approach combined with…

High Energy Physics - Phenomenology · Physics 2021-03-24 C. W. Xiao , J. J. Wu , B. S. Zou

The P-wave charm-strange mesons $D_{s0}(2317)$ and $D_{s1}(2460)$ lie below the $DK$ and $D^\ast K$ threshold respectively. They are extremely narrow because their strong decays violate the isospin symmetry. We study the possible heavy…

High Energy Physics - Phenomenology · Physics 2011-03-18 Bin Hu , Xiao-Lin Chen , Zhi-Gang Luo , Peng-Zhi Huang , Shi-Lin Zhu , Peng-Fei Yu , Xiang Liu

The exploration of energies above the open-flavor threshold in the meson spectra has led to the appearance of unexpected states difficult to accommodate in the naive picture of a bound state of a quark and an antiquark. Many of such states…

High Energy Physics - Phenomenology · Physics 2018-08-29 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernández

We relate the interactions of the $\bar{D}^{(\ast)} K^\ast$ and $D^{(\ast)} K^\ast$ systems to those of $D^{(\ast)}D^{(\ast)}$ and $D^{(\ast)}\bar{D}^{(\ast)}$ respectively, considering the residual strong interactions at the near-threshold…

High Energy Physics - Phenomenology · Physics 2024-02-28 Bo Wang , Kan Chen , Lu Meng , Shi-Lin Zhu

We calculate the masses of the resonances D_{s0}^*(2317) and D_{s1}(2460) as well as their bottom partners as bound states of a kaon and a D^*- and B^*-meson, respectively, in unitarized chiral perturbation theory at next-to-leading order.…

High Energy Physics - Phenomenology · Physics 2011-03-02 Martin Cleven , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

We estimate the partial widths for the radiative and pionic transitions from the $D_{s1}(2460)$ to the $D_{s0}(2317)$ in a molecule scenario, in which the $D_{s1}(2460)$ and $D_{s0}^\ast(2317)$ are considered as hadronic molecule states of…

High Energy Physics - Phenomenology · Physics 2016-05-18 Cheng-Jian Xiao , Dian-Yong Chen , Yong-Liang Ma

The $DK$ interaction is strong enough to form a bound state, the $D_{s0}^*(2317)$. This in turn begs the question of whether there are bound states composed of several charmed mesons and a kaon. Previous calculations indicate that the…

High Energy Physics - Phenomenology · Physics 2019-09-04 Tian-Wei Wu , Ming-Zhu Liu , Li-Sheng Geng , Emiko Hiyama , Manuel Pavon Valderrama

In this talk I present the results obtained using effective field theories in a finite volume from a reanalysis of lattice data on the $KD^{(*)}$ systems, where bound states of $KD$ and $KD^*$ are found and associated with the states…

High Energy Physics - Lattice · Physics 2017-12-29 A. Martinez Torres , E. Oset , S. Prelovsek , A. Ramos

A study of the $D_{sJ}^*(2317)^+$ and $D_{sJ}(2460)^+$ mesons in inclusive $c\bar{c}$ production is presented using 232 ${\rm fb}^{-1}$ of data collected by the BaBar experiment near $\sqrt{s} = 10.6$ \gev. Final states consisting of a…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert

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

The Babar and CLEO collaborations have recently observed states decaying to D_s^+\pi^0 and D_s^{*+}\pi^0 respectively and suggest the possible explanation that they are the missing P-wave c\bar{s} states with J^P=0^+ and 1^+. In this note…

High Energy Physics - Phenomenology · Physics 2010-04-05 Stephen Godfrey

We study the interaction of the $n \bar {D}_{s1}(2460)$ and $n \bar {D}_{s1}(2536)$ systems from the perspective that the $D_{s1}(2460)$ and $D_{s1}(2536)$ states are molecular states of $K D^*$ and $K^*D$, respectively. We use an improved…

High Energy Physics - Phenomenology · Physics 2025-08-11 Breno Agatão , Pedro Brandão , A. Martinez Torres , K. P. Khemchandani , Luciano M. Abreu , E. Oset

We study the experimental $DK$ invariant mass spectra of the reactions $B^+ \to \bar{D}^0 D^0 K^+$, $B^0 \to D^- D^0 K^+$ (measured by the BaBar Collaboration) and $B_s \to \pi^+ \bar{D}^0 K^-$ (measured by the LHCb Collaboration), where an…

High Energy Physics - Phenomenology · Physics 2016-06-22 Miguel Albaladejo , Daisuke Jido , Juan Nieves , Eulogio Oset

We have performed a coupled channel calculation of the $1^{++}$ $c\bar c$ sector including $q\bar q$ and $DD^*$ molecular configurations. The calculation was done within a constituent quark model which successfully describes the meson…

High Energy Physics - Phenomenology · Physics 2015-03-13 P. G. Ortega , J. Segovia , D. R. Entem , F. Fernandez

We investigate the $D_{s0}^\ast(2317)$ meson using lattice QCD and considering correlation functions of several $\bar{c} s$ two-quark and $\bar{c} s (\bar{u} u + \bar{d} d)$ four-quark interpolating fields. These interpolating fields…

High Energy Physics - Lattice · Physics 2020-02-12 Constantia Alexandrou , Joshua Berlin , Jacob Finkenrath , Theodoros Leontiou , Marc Wagner