{"title":"精确测定奇异 Zc(3900) 的极点位置","authors":"Yun-Hua Chen, Meng-Lin Du, Feng-Kun Guo","doi":"10.1007/s11433-023-2408-1","DOIUrl":null,"url":null,"abstract":"<div><p>We perform a unified description of the experimental data of the <i>π</i><sup>+</sup><i>π</i><sup>−</sup> and <i>J/ψπ</i><sup>±</sup> invariant mass spectra for <i>e</i><sup>+</sup><i>e</i><sup>−</sup> → <i>J/ψπ</i><sup>+</sup><i>π</i><sup>−</sup> and the <i>D</i><sup>0</sup><i>D</i><sup>*−</sup> mass spectrum for <i>e</i><sup>+</sup><i>e</i><sup>−</sup> → <i>D</i><sup>0</sup><i>D</i><sup>*−</sup><i>π</i><sup>+</sup> at <i>e</i><sup>+</sup><i>e</i><sup>−</sup> center-of-mass energies 4.23 and 4.26 GeV. The analysis takes into account open-charm meson loops that contain triangle singularities, the <span>\\(J/\\psi\\pi-D{\\bar D}^*\\)</span> coupled-channel interaction respecting unitarity, and the strong <span>\\(\\pi\\pi-K{\\bar K}\\)</span> final state interaction using dispersion relations. The analysis leads to a precise determination of the <i>Z</i><sub><i>c</i></sub>(3900) pole with the pole mass and width (3880.7 ± 1.7<sub>stat</sub> ± 22.4<sub>syst</sub>) MeV and (35.9 ± 1.4<sub>stat</sub> ± 15.3<sub>syst</sub>) MeV, respectively, and hints at that the <span>\\(D{\\bar D}^*\\)</span> molecular and non-molecular components are of similar importance in the <i>Z</i><sub><i>c</i></sub>(3900) formation.</p></div>","PeriodicalId":774,"journal":{"name":"Science China Physics, Mechanics & Astronomy","volume":"67 9","pages":""},"PeriodicalIF":6.4000,"publicationDate":"2024-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Precise determination of the pole position of the exotic Zc(3900)\",\"authors\":\"Yun-Hua Chen, Meng-Lin Du, Feng-Kun Guo\",\"doi\":\"10.1007/s11433-023-2408-1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We perform a unified description of the experimental data of the <i>π</i><sup>+</sup><i>π</i><sup>−</sup> and <i>J/ψπ</i><sup>±</sup> invariant mass spectra for <i>e</i><sup>+</sup><i>e</i><sup>−</sup> → <i>J/ψπ</i><sup>+</sup><i>π</i><sup>−</sup> and the <i>D</i><sup>0</sup><i>D</i><sup>*−</sup> mass spectrum for <i>e</i><sup>+</sup><i>e</i><sup>−</sup> → <i>D</i><sup>0</sup><i>D</i><sup>*−</sup><i>π</i><sup>+</sup> at <i>e</i><sup>+</sup><i>e</i><sup>−</sup> center-of-mass energies 4.23 and 4.26 GeV. The analysis takes into account open-charm meson loops that contain triangle singularities, the <span>\\\\(J/\\\\psi\\\\pi-D{\\\\bar D}^*\\\\)</span> coupled-channel interaction respecting unitarity, and the strong <span>\\\\(\\\\pi\\\\pi-K{\\\\bar K}\\\\)</span> final state interaction using dispersion relations. The analysis leads to a precise determination of the <i>Z</i><sub><i>c</i></sub>(3900) pole with the pole mass and width (3880.7 ± 1.7<sub>stat</sub> ± 22.4<sub>syst</sub>) MeV and (35.9 ± 1.4<sub>stat</sub> ± 15.3<sub>syst</sub>) MeV, respectively, and hints at that the <span>\\\\(D{\\\\bar D}^*\\\\)</span> molecular and non-molecular components are of similar importance in the <i>Z</i><sub><i>c</i></sub>(3900) formation.</p></div>\",\"PeriodicalId\":774,\"journal\":{\"name\":\"Science China Physics, Mechanics & Astronomy\",\"volume\":\"67 9\",\"pages\":\"\"},\"PeriodicalIF\":6.4000,\"publicationDate\":\"2024-08-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Science China Physics, Mechanics & Astronomy\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s11433-023-2408-1\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Science China Physics, Mechanics & Astronomy","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s11433-023-2408-1","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Precise determination of the pole position of the exotic Zc(3900)
We perform a unified description of the experimental data of the π+π− and J/ψπ± invariant mass spectra for e+e− → J/ψπ+π− and the D0D*− mass spectrum for e+e− → D0D*−π+ at e+e− center-of-mass energies 4.23 and 4.26 GeV. The analysis takes into account open-charm meson loops that contain triangle singularities, the \(J/\psi\pi-D{\bar D}^*\) coupled-channel interaction respecting unitarity, and the strong \(\pi\pi-K{\bar K}\) final state interaction using dispersion relations. The analysis leads to a precise determination of the Zc(3900) pole with the pole mass and width (3880.7 ± 1.7stat ± 22.4syst) MeV and (35.9 ± 1.4stat ± 15.3syst) MeV, respectively, and hints at that the \(D{\bar D}^*\) molecular and non-molecular components are of similar importance in the Zc(3900) formation.
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