Λ<i><sub>b</Sub>< State Newly Observed by Lhcb

dc.authorid Azizi, Kazem/0000-0003-3741-2167
dc.authorscopusid 17345170000
dc.authorscopusid 24391488900
dc.authorscopusid 6508230150
dc.authorwosid Sundu, Hayriye/A-5128-2018
dc.authorwosid Sarac, Yasemin/AAN-1696-2020
dc.authorwosid Azizi, Kazem/ABE-4757-2021
dc.contributor.author Azizi, K.
dc.contributor.author Sarac, Y.
dc.contributor.author Sundu, H.
dc.contributor.other Physics Group
dc.date.accessioned 2024-07-05T15:38:43Z
dc.date.available 2024-07-05T15:38:43Z
dc.date.issued 2020
dc.department Atılım University en_US
dc.department-temp [Azizi, K.] Univ Tehran, Dept Phys, North Karegar Ave, Tehran 14395547, Iran; [Azizi, K.] Dogus Univ, Dept Phys, TR-34722 Istanbul, Turkey; [Sarac, Y.] Atilim Univ, Elect & Elect Engn Dept, TR-06836 Ankara, Turkey; [Sundu, H.] Kocaeli Univ, Dept Phys, TR-41380 Izmit, Turkey en_US
dc.description Azizi, Kazem/0000-0003-3741-2167 en_US
dc.description.abstract We study the bottom Lambda(b)(6146)(0) baryon, newly discovered by the LHCb Collaboration. By adopting an interpolating current of (L-rho, L-lambda) = (0, 2) type and D-wave nature with spin-parity quantum numbers J(P) = 3/2(+) for this heavy bottom baryon, we calculate its mass and residue. Using these spectroscopic parameters, we also investigate its dominant decays Lambda(b)(6146)(0) -> Sigma(b)pi and Lambda(b)(6146)(0) -> Sigma(*)(b)pi and estimate the width of Lambda(b)(6146)(0) obtained via these channels. The obtained mass, m(Lambda b) = (6144 +/- 68) MeV is in accord nicely with the experimental data. The width obtained via the dominant channels is also consistent with the experimental data of LHCb collaboration. We calculate the spectroscopic parameters and the same decay channels for the c-partner of Lambda(b)(6146)(0) state, namely Lambda(c)(2860)(+), as well. We compare the obtained results with the existing theoretical predictions as well as experimental data. The results indicate that the state Lambda(b)(6146)(0) and its charmed-partner Lambda(c)(2860)(+) can be considered as 1D-wave baryons with J(P) = 3/2(+). en_US
dc.identifier.citationcount 18
dc.identifier.doi 10.1103/PhysRevD.101.074026
dc.identifier.issn 2470-0010
dc.identifier.issn 2470-0029
dc.identifier.issue 7 en_US
dc.identifier.scopus 2-s2.0-85084526943
dc.identifier.scopusquality Q1
dc.identifier.uri https://doi.org/10.1103/PhysRevD.101.074026
dc.identifier.uri https://hdl.handle.net/20.500.14411/3142
dc.identifier.volume 101 en_US
dc.identifier.wos WOS:000527127700003
dc.identifier.wosquality Q1
dc.institutionauthor Saraç Oymak, Yasemin
dc.language.iso en en_US
dc.publisher Amer Physical Soc en_US
dc.relation.publicationcategory Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı en_US
dc.rights info:eu-repo/semantics/openAccess en_US
dc.scopus.citedbyCount 18
dc.subject [No Keyword Available] en_US
dc.title Λ<i><sub>b</Sub>< State Newly Observed by Lhcb en_US
dc.type Article en_US
dc.wos.citedbyCount 17
dspace.entity.type Publication
relation.isAuthorOfPublication 76c2e6e0-40bb-4e6f-b776-53c925ab44d4
relation.isAuthorOfPublication.latestForDiscovery 76c2e6e0-40bb-4e6f-b776-53c925ab44d4
relation.isOrgUnitOfPublication 2682824b-512d-4a4e-8498-5b5719f606fe
relation.isOrgUnitOfPublication.latestForDiscovery 2682824b-512d-4a4e-8498-5b5719f606fe

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