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The $D_{s0}^*(2317)^+$ decay to $D_s^+π^0$ and $D_s^{*+}γ$

Pei-Sen Su, Wen-Tao Lyu, Wei-Hong Liang, Eulogio Oset

TL;DR

This work analyzes the decays of $D_{s0}^*(2317)^+$ to $D_s^+\pi^0$ and $D_s^{*+}\gamma$ within a molecular picture generated by coupled channels $D^0K^+$, $D^+K^0$, $D_s^+\eta$, and $D_s^+\pi^0$ using a local hidden gauge interaction with vector-meson exchange. The strong width is obtained via both a coupled-channel loop and a triangle mechanism, yielding $\Gamma(D_{s0}^*\to D_s^+\pi^0)\approx 70\ \mathrm{keV}$, while the radiative width is computed including charged-current, contact, and anomalous contributions, giving $\Gamma(D_{s0}^*\to D_s^{*+}\gamma)\approx 1.33\ \mathrm{keV}$ with anomalous terms being negligible. The ratio $R = \Gamma_{\gamma}/\Gamma_{\pi^0}$ is $\approx 0.019$, below the Belle-II measurement of $R = (7.14 \pm 0.70 \pm 0.23) \times 10^{-2}$, indicating a tension that calls for precise independent measurements of both decay widths. The results support a molecular interpretation with a substantial $DK$ component but do not resolve the discrepancy with experiment, emphasizing the need for improved data to clarify the $D_{s0}^*(2317)^+$ structure.

Abstract

We study the strong decay of $D_{s0}^*(2317)^+$ to $D_s^+ π^0$ considering the coupled channels of $D^0 K^+, D^+ K^0, D_s^+ η$ and $D_s^+ π^0$ within a picture for the interaction based on the local hidden gauge approach. We also address the problem of the radiative decay to $D_s^{*+} γ$, using the same information obtained from the molecular picture. We obtain a strong width of the $D_{s0}^*(2317)^+$ of about $71 \,\rm keV$ and a radiative decay of $1.3 \,\rm keV$. The anomalous terms for the radiative decay are considered for the first time, but they are found negligible. We make a thorough discussion of this and other results to the light of the recent measurement of Belle for the ratio of these two decay modes, and make a call for the precise measurement of the two decay widths independently to clarify the present situation concerning the nature of of the $D_{s0}^*(2317)^+$ state.

The $D_{s0}^*(2317)^+$ decay to $D_s^+π^0$ and $D_s^{*+}γ$

TL;DR

This work analyzes the decays of to and within a molecular picture generated by coupled channels , , , and using a local hidden gauge interaction with vector-meson exchange. The strong width is obtained via both a coupled-channel loop and a triangle mechanism, yielding , while the radiative width is computed including charged-current, contact, and anomalous contributions, giving with anomalous terms being negligible. The ratio is , below the Belle-II measurement of , indicating a tension that calls for precise independent measurements of both decay widths. The results support a molecular interpretation with a substantial component but do not resolve the discrepancy with experiment, emphasizing the need for improved data to clarify the structure.

Abstract

We study the strong decay of to considering the coupled channels of and within a picture for the interaction based on the local hidden gauge approach. We also address the problem of the radiative decay to , using the same information obtained from the molecular picture. We obtain a strong width of the of about and a radiative decay of . The anomalous terms for the radiative decay are considered for the first time, but they are found negligible. We make a thorough discussion of this and other results to the light of the recent measurement of Belle for the ratio of these two decay modes, and make a call for the precise measurement of the two decay widths independently to clarify the present situation concerning the nature of of the state.

Paper Structure

This paper contains 12 sections, 61 equations, 7 figures, 3 tables.

Figures (7)

  • Figure 1: Diagrammatic representation of vector exchange as a source of the interaction between two pseudoscalars.
  • Figure 2: Diagrams entering the evaluation of the coupling of $D_{s0}(2317)^+$ to $D_s^+ \pi^0$, with the momenta of the particles in parenthesis.
  • Figure 3: Diagrams involved in the $D_{s0}^{*}(2317)^+$ decay to $D_s^{*+} \gamma$, involving the charge coupling of the photons to the mesons. In parenthesis the momenta of the particles.
  • Figure 4: Diagrams for the charge coupling of a photon to a meson.
  • Figure 5: Meson in flight $(a)$ and contact term $(b)$ required by gauge invariance.
  • ...and 2 more figures