{ "id": "2210.12992", "version": "v1", "published": "2022-10-24T07:28:23.000Z", "updated": "2022-10-24T07:28:23.000Z", "title": "Further understanding the nature of $a_0(1710)$ in the $D^+_s \\to π^0 K^+ K^0_S$ decay", "authors": [ "Xin Zhu", "Hao-Nan Wang", "De-Min Li", "En Wang", "Li-Sheng Geng", "Ju-Jun Xie" ], "comment": "8 pages, 8 figures", "categories": [ "hep-ph", "hep-ex", "nucl-ex", "nucl-th" ], "abstract": "Based on our previous work about the role of $a_0(1710)$ in the $D_s^+\\to\\pi^+K_S^0K_S^0$ decay [Phy. Rev. D 105, 116010 (2022)], we perform a further theoretical study of $a_0(1710)^+$ in the process $D^+_s \\to \\pi^0 a_0(1710)^+ \\to \\pi^0 K^+ K^0_S$. In addition to $a_0(1710)$, the contributions of $K^*$ and $a_0(980)$ are also taken into account. Firstly, we consider the contributions from the tree diagrams of $K^{*+} \\to K^+\\pi^0$ and $\\bar{K}^{*0} \\to \\pi^0 \\bar{K}^0$. Secondly, we describe the final state interaction of $K\\bar{K}$ in the chiral unitary approach to study the contribution of $a_0(980)$, while the $a_0(1710)$ state is dynamically generated from the $K^*\\bar{K}^*$ interaction, and then decays into $K^+\\bar{K}^0$. Since the final $K^+ K_S^0$ state is in pure isospin $I=1$, the $D_s^+\\to\\pi^0K^+K_s^0$ decay is an ideal process to study the $a_0(1710)^+$ and $a_0(980)^+$ resonances. Based on our theoretical calculations, it is found that the recent experimental measurements on the $K^+K^0_S$, $\\pi^0K^+$, and $\\pi^0 K_S^0$ invariant mass distributions can be well reproduced, which supports the molecular $K^*\\bar{K}^*$ nature of the scalar $a_0(1710)$ resonance.", "revisions": [ { "version": "v1", "updated": "2022-10-24T07:28:23.000Z" } ], "analyses": { "keywords": [ "chiral unitary approach", "invariant mass distributions", "contribution", "final state interaction", "pure isospin" ], "note": { "typesetting": "TeX", "pages": 8, "language": "en", "license": "arXiv", "status": "editable" } } }