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dc.contributor.authorFerretti, J.
dc.contributor.authorSantopinto, E.
dc.date.accessioned2020-04-24T09:19:55Z
dc.date.available2020-04-24T09:19:55Z
dc.date.issued2020
dc.identifier.citationFerretti, J., & Santopinto, E. (2020). Hidden-charm and bottom tetra- and pentaquarks with strangeness in the hadro-quarkonium and compact tetraquark models. <i>Journal of High Energy Physics</i>, <i>2020</i>(4), Article 119. <a href="https://doi.org/10.1007/JHEP04(2020)119" target="_blank">https://doi.org/10.1007/JHEP04(2020)119</a>
dc.identifier.otherCONVID_35279096
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/68668
dc.description.abstractIn two recent papers, we used the hadro-quarkonium model to study the properties of hidden-charm and bottom tetraquarks and pentaquarks. Here, we extend the previous results and calculate the masses of heavy-quarkonium-kaon/hyperon systems. We also compute the spectrum of hidden-charm and bottom tetraquarks with strangeness in the compact tetraquark (diquark-antidiquark) model. If heavy-light exotic systems with non-null strangeness content were to be observed experimentally, it might be possible to distinguish among the large variety of available theoretical pictures for tetra- and pentaquark states and, possibly, rule out those which are not compatible with the data.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherSpringer; Societa Italiana di Fisica
dc.relation.ispartofseriesJournal of High Energy Physics
dc.rightsCC BY 4.0
dc.subject.otherphenomenological models
dc.subject.otherQCD phenomenology
dc.titleHidden-charm and bottom tetra- and pentaquarks with strangeness in the hadro-quarkonium and compact tetraquark models
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202004242881
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn1126-6708
dc.relation.numberinseries4
dc.relation.volume2020
dc.type.versionpublishedVersion
dc.rights.copyright© The Authors. Article funded by SCOAP3.
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber320062
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1007/JHEP04(2020)119
dc.relation.funderResearch Council of Finlanden
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundinginformationThis work was supported by the U.S. Department of Energy (Grant No. DE-FG-02-91ER40608) and the Academy of Finland, Project No. 320062.
dc.type.okmA1


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