Investigations of Λ states with spin-parity 3 ± 2

dc.authoridAzizi, Kazem/0000-0003-3741-2167
dc.authorscopusid17345170000
dc.authorscopusid24391488900
dc.authorscopusid6508230150
dc.contributor.authorSaraç Oymak, Yasemin
dc.contributor.authorSarac, Y.
dc.contributor.authorSundu, H.
dc.contributor.otherPhysics Group
dc.date.accessioned2024-07-05T15:50:43Z
dc.date.available2024-07-05T15:50:43Z
dc.date.issued2024
dc.departmentAtılım Universityen_US
dc.department-temp[Azizi, K.] Univ Tehran, Dept Phys, North Karegar Ave, Tehran 14395547, Iran; [Azizi, K.] Dogus Univ, Dept Phys, TR-34775 Istanbul, Turkiye; [Azizi, K.] Inst Res Fundamental Sci IPM, Sch Particles & Accelerators, POB 19395-5531, Tehran, Iran; [Sarac, Y.] Atilim Univ, Elect & Elect Engn Dept, TR-06836 Ankara, Turkiye; [Sundu, H.] Istanbul Medeniyet Univ, Dept Phys Engn, TR-34700 Istanbul, Turkiyeen_US
dc.descriptionAzizi, Kazem/0000-0003-3741-2167en_US
dc.description.abstractThe present study provides spectroscopic investigations of spin-32 A baryons with both positive and negative parities. The analysis mainly focuses on three states, namely 1P, 2P, and 2S, and corresponding masses are calculated using the QCD sum rule method. To implement the method, we apply two types of interpolating currents with octet and singlet quantum numbers and compare the corresponding results with the reported masses of experimentally observed states. From the comparisons, it is extracted that the results of interpolating current with octet quantum numbers are in good agreement with the experimentally measured masses. The masses obtained with this interpolating current are m = 1513.64 +/- 8.76 MeV for 1P state with JP = 3 -, m' = 1687.91 +/- 0.31 MeV for 2P state with JP = 3 - and m = 1882.37 +/- 11.95 MeV for 2S state with JP = 3 + and they are consistent with the experimental masses of A(1520), A(1690), and A(1890), respectively, which confirm their spin-parity quantum numbers. Besides, we calculate the corresponding current coupling constants, which are utilized as inputs in the calculations of different form factors defining the widths of the states under study.en_US
dc.description.sponsorshipIran National Science Foundation, INSF, (4025036)en_US
dc.description.sponsorshipIran National Science Foundation (INSF) [4025036]en_US
dc.description.sponsorshipK. A. is grateful to Iran National Science Foundation (INSF) for the partial financial support provided under the elites Grant No. 4025036.en_US
dc.description.woscitationindexScience Citation Index Expanded
dc.identifier.citation0
dc.identifier.doi10.1103/PhysRevD.109.074028
dc.identifier.issn2470-0010
dc.identifier.issn2470-0029
dc.identifier.issue7en_US
dc.identifier.scopus2-s2.0-85191607477
dc.identifier.scopusqualityQ1
dc.identifier.urihttps://doi.org/10.1103/PhysRevD.109.074028
dc.identifier.volume109en_US
dc.identifier.wosWOS:001246467800001
dc.identifier.wosqualityQ1
dc.language.isoenen_US
dc.publisherAmer Physical Socen_US
dc.relation.ispartofPhysical Review Den_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.subject[No Keyword Available]en_US
dc.titleInvestigations of Λ states with spin-parity 3 ± 2en_US
dc.typeArticleen_US
dspace.entity.typePublication
relation.isAuthorOfPublication76c2e6e0-40bb-4e6f-b776-53c925ab44d4
relation.isAuthorOfPublication.latestForDiscovery76c2e6e0-40bb-4e6f-b776-53c925ab44d4
relation.isOrgUnitOfPublication2682824b-512d-4a4e-8498-5b5719f606fe
relation.isOrgUnitOfPublication.latestForDiscovery2682824b-512d-4a4e-8498-5b5719f606fe

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