{"title":"Can the newly reported \nPcs(4459)\n be a strange hidden-charm \nΞcD¯*\n molecular pentaquark?","authors":"Rui Chen","doi":"10.1103/PHYSREVD.103.054007","DOIUrl":null,"url":null,"abstract":"Stimulated by the $P_{cs}(4459)$ reported by the LHCb Collaboration, we perform a single $\\Xi_c\\bar{D}^*$ channel and a coupled $\\Xi_c\\bar{D}^*/\\Xi_c^*\\bar{D}/\\Xi_c^{\\prime}\\bar{D}^*/\\Xi_c^*\\bar{D}^*$ channel analysis by using a one-boson-exchange model. Our results indicate that the newly $P_{cs}(4459)$ cannot be a pure $\\Xi_c\\bar{D}^*$ molecular state, but a coupled $\\Xi_c\\bar{D}^*/\\Xi_c^*\\bar{D}/\\Xi_c^{\\prime}\\bar{D}^*/\\Xi_c^*\\bar{D}^*$ bound state with $I(J^P)=0(3/2^-)$, where the $\\Xi_c\\bar{D}^*$ and $\\Xi_c^*\\bar{D}$ components are dominant. Meanwhile, we find the interactions from the $\\Xi_c^{\\prime}\\bar{D}^*$ system with $0(1/2^-)$, the $\\Xi_c^{*}\\bar{D}$ system with $1(3/2^-)$, and the $\\Xi_c^{*}\\bar{D}^*$ system with $1(1/2^-)$ are strongly attractive, where one can expect possible strange hidden-charm molecular or resonant structures near the these thresholds with the assigned quantum numbers.","PeriodicalId":8457,"journal":{"name":"arXiv: High Energy Physics - Phenomenology","volume":"40 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2020-11-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"27","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv: High Energy Physics - Phenomenology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1103/PHYSREVD.103.054007","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 27
Abstract
Stimulated by the $P_{cs}(4459)$ reported by the LHCb Collaboration, we perform a single $\Xi_c\bar{D}^*$ channel and a coupled $\Xi_c\bar{D}^*/\Xi_c^*\bar{D}/\Xi_c^{\prime}\bar{D}^*/\Xi_c^*\bar{D}^*$ channel analysis by using a one-boson-exchange model. Our results indicate that the newly $P_{cs}(4459)$ cannot be a pure $\Xi_c\bar{D}^*$ molecular state, but a coupled $\Xi_c\bar{D}^*/\Xi_c^*\bar{D}/\Xi_c^{\prime}\bar{D}^*/\Xi_c^*\bar{D}^*$ bound state with $I(J^P)=0(3/2^-)$, where the $\Xi_c\bar{D}^*$ and $\Xi_c^*\bar{D}$ components are dominant. Meanwhile, we find the interactions from the $\Xi_c^{\prime}\bar{D}^*$ system with $0(1/2^-)$, the $\Xi_c^{*}\bar{D}$ system with $1(3/2^-)$, and the $\Xi_c^{*}\bar{D}^*$ system with $1(1/2^-)$ are strongly attractive, where one can expect possible strange hidden-charm molecular or resonant structures near the these thresholds with the assigned quantum numbers.