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Related papers: Isospin quantum number of D_{s0}^+(2317)

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By studying the decays D_{s0}^+(2317) --> D_s^+ pi^0 and D_s^{*+} gamma, It is shown that its assignment to the I_3=0 component of iso-triplet scalar four-quark mesons is favored. Productions of its neutral and doubly charged partners are…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kunihiko Terasaki

Although assigning D_{s0}^+(2317) to the I_3=0 component of iso-triplet four-quark mesons is favored by experiments, its neutral and doubly charged partners have not yet been observed. It is discussed why they were not observed in inclusive…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kunihiko Terasaki

A brief overview of charm scalar resonances is given. It is demonstrated that experimental data on the D_s^{*+}gamma and D_s^+pi^0 decays of D_{s0}^+(2317) favor its assignment to the I_3=0 component of iso-triplet four-quark mesons. The…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Terasaki

We use the QCD sum rules to analize the hadronic decay $D_{sJ}^{+}(2317)\to D_s^+\pi^0$, in the hypotesis that the $D_{sJ}^{+}(2317)$ can be identified as a four-quark state. We use a diquak-antidiquark current and work to the order of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Marina Nielsen

The $D_s(2320)$ state recently observed by BaBar in the $D_s^+\pi^0$ channel may be the first of a host of $cq\bar q\bar q$ four-quark states. We give a phenomenological account of the masses and decay modes. The isosinglet $D_s(2320)$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Wei-Shu Hou

It is pointed out that assigning D_{s0}^+(2317) to an iso-triplet tetra-quark meson is favored by experiments. It also is discussed why its neutral and doubly charged partners have never been observed in inclusive e^+e^- annihilation. To…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kunihiko Terasaki

Decays of hidden-charm scalar tetra-quark mesons as the partners of D_{s0}(2317) which has successfully been assigned to the iso-triplet scalar tetra-quark [c,n][sbar,nbar]_{I=1} meson are studied. Because OZI-rule allowed strong decays are…

High Energy Physics - Phenomenology · Physics 2009-03-12 Kunihiko Terasaki

Taking $D_{s0}^{*}(2317)^{+ }$ as a conventional $c\bar s$ meson, we calculate its dominant strong and electromagnetic decays in the framework of the Bethe-Salpeter method. Our results are $\Gamma(D_{s0}^{*+}\to D_s^+\pi^0) =…

High Energy Physics - Phenomenology · Physics 2023-06-27 Meng Han , Wei Li , Su-Yan Pei , Ting-Ting Liu , Guo-Li Wang

We consider a possible interpretation of the new charm-strange meson Ds0*(2317) as a hadronic molecule - a bound state of D and K mesons. Using an effective Lagrangian approach we calculate the strong Ds0* to Ds pi0 and radiative Ds0* to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amand Faessler , Thomas Gutsche , Valery E. Lyubovitskij , Yong-Liang Ma

The internal structure of the charm-strange mesons $D_{s0}^*(2317)$ and $D_{s1}(2460)$ are subject of intensive studies. Their widths are small because they decay dominantly through isospin-breaking hadronic channels $D_{s0}^*(2317)^+\to…

High Energy Physics - Phenomenology · Physics 2023-04-21 Meng-Na Tang , Yong-Hui Lin , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

Through the scattering of light-pseudoscalar mesons ($\pi,K,\eta,\eta'$) off charmed mesons ($D, D_s$), we study the $D^{*}_{s0}(2317)$ state and other relevant charm scalar mesons in a unitarized chiral effective field theory approach. We…

High Energy Physics - Phenomenology · Physics 2015-11-11 Zhi-Hui Guo , Ulf-G. Meißner , De-Liang Yao

Recently, the BES\uppercase\expandafter{\romannumeral3} Collaboration updated the data for the exotic state, $D^{*}_{s0}(2317)$, with a mass of $2318.3\pm1.2\pm1.2$ MeV from the positronium annihilation process. Inspired by the experiment,…

High Energy Physics - Phenomenology · Physics 2025-03-17 Yue Tan , Yuheng Wu , Youchang Yang , Jialun Ping

We construct the effective chiral Lagrangian involving the D--mesons and Goldstone bosons at next-to-leading order taking into account strong as well as electromagnetic interactions. This allows us to disentangle -- to leading order in…

High Energy Physics - Phenomenology · Physics 2008-11-26 Feng-Kun Guo , Christoph Hanhart , Siegfried Krewald , Ulf-G. Meißner

Using data collected with the CLEO~II detector, we have observed the isospin-violating decay $D_s^{*+}\to D_s^+\pi^0$. The decay rate for this mode, relative to the dominant radiative decay, is found to be $\Gamma(D_s^{*+}\to…

High Energy Physics - Experiment · Physics 2008-11-26 CLEO Collaboration , J. Gronberg et al

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

For coupled channels $D^0K^+$, $D^+K^0$, $D_s^+\eta$, and $D_s^+\pi^0$, the $S$-wave scattering amplitudes are constructed taking into account the mixing of the isoscalar resonance $D^*_{s0}(2317)^+$ with nonresonance amplitudes with…

High Energy Physics - Phenomenology · Physics 2025-11-06 N. N. Achasov , G. N. Shestakov

We analyze the hadronic and radiative decay modes of the recently observed $D_{sJ}(2317)$ meson, in the hypothesis that it can be identifield with the scalar $s_\ell^P={1\over 2}^+$ state of $c \bar s$ spectrum ($D_{s0}$). The method is…

High Energy Physics - Phenomenology · Physics 2016-09-06 P. Colangelo , F. De Fazio

We present the formalism for the decay of dynamically generated scalar mesons with open- or hidden-charm and give results for the decay of D^*_{s0} (2317) to \gamma D_s^* plus that of a hidden charm scalar meson state predicted by the…

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

The isospin breaking and radiative decay widths of the positive-parity charm-strange mesons, $D^{*}_{s0}$ and $D_{s1}$, and their predicted bottom-strange counterparts, $B^{*}_{s0}$ and $B_{s1}$, as hadronic molecules are revisited. This is…

High Energy Physics - Phenomenology · Physics 2023-08-28 Hai-Long Fu , Harald W. Grießhammer , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

We study the strong decay of $D_{s0}^*(2317)^+$ to $D_s^+ \pi^0$ considering the coupled channels of $D^0 K^+, D^+ K^0, D_s^+ \eta$ and $D_s^+ \pi^0$ within a picture for the interaction based on the local hidden gauge approach. We also…

High Energy Physics - Phenomenology · Physics 2026-03-17 Pei-Sen Su , Wen-Tao Lyu , Wei-Hong Liang , Eulogio Oset
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