000902840 001__ 902840
000902840 005__ 20230217124239.0
000902840 0247_ $$2doi$$a10.1103/PhysRevD.104.094006
000902840 0247_ $$2ISSN$$a0556-2821
000902840 0247_ $$2ISSN$$a1089-4918
000902840 0247_ $$2ISSN$$a1538-4500
000902840 0247_ $$2ISSN$$a1550-2368
000902840 0247_ $$2ISSN$$a1550-7998
000902840 0247_ $$2ISSN$$a2470-0010
000902840 0247_ $$2ISSN$$a2470-0029
000902840 0247_ $$2Handle$$a2128/29220
000902840 0247_ $$2WOS$$aWOS:000718037000013
000902840 037__ $$aFZJ-2021-04597
000902840 082__ $$a530
000902840 1001_ $$0P:(DE-Juel1)176611$$aAnwar, Muhammad Naeem$$b0$$eCorresponding author
000902840 245__ $$aHeavy quark spin partners of the Y ( 4260 ) in coupled-channel formalism
000902840 260__ $$aMelville, NY$$bInst.$$c2021
000902840 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2021-11-05
000902840 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2021-11-01
000902840 3367_ $$2DRIVER$$aarticle
000902840 3367_ $$2DataCite$$aOutput Types/Journal article
000902840 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1638256252_14457
000902840 3367_ $$2BibTeX$$aARTICLE
000902840 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000902840 3367_ $$00$$2EndNote$$aJournal Article
000902840 520__ $$aThe charmoniumlike state Y(4260) is described as predominantly a D1¯D molecule in a coupled-channel quark model [Phys. Rev. D 96, 114022 (2017)]. The heavy quark spin symmetry (HQSS) thus implies the possible emergence of its heavy quark spin partners with molecular configurations as D1¯D∗ and D∗2¯D∗ below these charmed mesons’ thresholds. We analyze the probabilities of various intermediate charmed meson loops for JPC=1−− exotic state Y(4360) and find that the channel D1¯D∗ couples more strongly around its mass regime, and the coupling behavior remains the same even if the mass of Y(4360) is pushed closer to D1¯D∗ threshold. This enlightens that the most favorable molecular scenario for the Y(4360) could be D1¯D∗, and hence it can be interpreted as HQSS partner of the Y(4260). We also find the strong coupling behavior of D∗2¯D∗ channel with the ψ(4415), which makes it a good candidate for a dominant D∗2¯D∗ molecule. We discuss the important decay patterns of these resonances to disentangle their long- and short-distance structures.
000902840 536__ $$0G:(DE-HGF)POF4-5111$$a5111 - Domain-Specific Simulation & Data Life Cycle Labs (SDLs) and Research Groups (POF4-511)$$cPOF4-511$$fPOF IV$$x0
000902840 542__ $$2Crossref$$i2021-11-05$$uhttps://creativecommons.org/licenses/by/4.0/
000902840 588__ $$aDataset connected to DataCite
000902840 7001_ $$0P:(DE-Juel1)190739$$aLu, Yu$$b1$$ufzj
000902840 77318 $$2Crossref$$3journal-article$$a10.1103/physrevd.104.094006$$bAmerican Physical Society (APS)$$d2021-11-05$$n9$$p094006$$tPhysical Review D$$v104$$x2470-0010$$y2021
000902840 773__ $$0PERI:(DE-600)2844732-3$$a10.1103/PhysRevD.104.094006$$gVol. 104, no. 9, p. 094006$$n9$$p094006$$tPhysical review / D$$v104$$x2470-0010$$y2021
000902840 8564_ $$uhttps://juser.fz-juelich.de/record/902840/files/PhysRevD.104.094006.pdf$$yOpenAccess
000902840 909CO $$ooai:juser.fz-juelich.de:902840$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000902840 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)176611$$aForschungszentrum Jülich$$b0$$kFZJ
000902840 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)190739$$aForschungszentrum Jülich$$b1$$kFZJ
000902840 9131_ $$0G:(DE-HGF)POF4-511$$1G:(DE-HGF)POF4-510$$2G:(DE-HGF)POF4-500$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF4-5111$$aDE-HGF$$bKey Technologies$$lEngineering Digital Futures – Supercomputing, Data Management and Information Security for Knowledge and Action$$vEnabling Computational- & Data-Intensive Science and Engineering$$x0
000902840 9141_ $$y2021
000902840 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000902840 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000902840 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search
000902840 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bPHYS REV D : 2016
000902840 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000902840 915__ $$0StatID:(DE-HGF)0110$$2StatID$$aWoS$$bScience Citation Index
000902840 915__ $$0StatID:(DE-HGF)0111$$2StatID$$aWoS$$bScience Citation Index Expanded
000902840 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5
000902840 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000902840 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC
000902840 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences
000902840 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline
000902840 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List
000902840 915__ $$0StatID:(DE-HGF)0570$$2StatID$$aSCOAP3
000902840 920__ $$lyes
000902840 9201_ $$0I:(DE-Juel1)IAS-4-20090406$$kIAS-4$$lTheorie der Starken Wechselwirkung$$x0
000902840 980__ $$ajournal
000902840 980__ $$aVDB
000902840 980__ $$aUNRESTRICTED
000902840 980__ $$aI:(DE-Juel1)IAS-4-20090406
000902840 9801_ $$aFullTexts
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.124.072001
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.scib.2021.04.023
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.122.242001
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.100.014021
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.103.054016
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.100.014031
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.84.054010
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.84.031502
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1140/epja/i2011-11120-6
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1007/JHEP06(2017)158
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.84.114013
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.86.014004
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.84.054002
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.111.132003
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1093/ptep/ptaa104
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/RevModPhys.90.015004
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.98.212001
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.99.142002
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.89.111103
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.91.112007
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.118.092001
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physrep.2020.05.001
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physrep.2016.05.004
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.96.032004
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.99.019903
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.96.114022
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.89.114013
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.94.034021
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.99.094005
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.95.034018
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/0550-3213(69)90039-X
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1140/epjc/s10052-020-8032-5
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/0003-4916(59)90051-X
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.72.094004
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.94.054035
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.69.112002
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.77.055206
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.32.189
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.78.114033
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1140/epjc/s10052-017-5328-1
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.64.094002
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physletb.2007.11.100
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.95.114031
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.80.091101
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.90.074039
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.122.102002
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.17.3090
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.21.313.2
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.21.203
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.72.054026
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.80.014012
000902840 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1002/asna.19272301903