Λ<i><sub>b</sub></i>(6146)<SUP>0</SUP> state newly observed by LHCb

dc.authoridAzizi, Kazem/0000-0003-3741-2167
dc.authorscopusid17345170000
dc.authorscopusid24391488900
dc.authorscopusid6508230150
dc.authorwosidSundu, Hayriye/A-5128-2018
dc.authorwosidSarac, Yasemin/AAN-1696-2020
dc.authorwosidAzizi, Kazem/ABE-4757-2021
dc.contributor.authorAzizi, K.
dc.contributor.authorSarac, Y.
dc.contributor.authorSundu, H.
dc.contributor.otherPhysics Group
dc.date.accessioned2024-07-05T15:38:43Z
dc.date.available2024-07-05T15:38:43Z
dc.date.issued2020
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-34722 Istanbul, Turkey; [Sarac, Y.] Atilim Univ, Elect & Elect Engn Dept, TR-06836 Ankara, Turkey; [Sundu, H.] Kocaeli Univ, Dept Phys, TR-41380 Izmit, Turkeyen_US
dc.descriptionAzizi, Kazem/0000-0003-3741-2167en_US
dc.description.abstractWe 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.citation18
dc.identifier.doi10.1103/PhysRevD.101.074026
dc.identifier.issn2470-0010
dc.identifier.issn2470-0029
dc.identifier.issue7en_US
dc.identifier.scopus2-s2.0-85084526943
dc.identifier.scopusqualityQ1
dc.identifier.urihttps://doi.org/10.1103/PhysRevD.101.074026
dc.identifier.urihttps://hdl.handle.net/20.500.14411/3142
dc.identifier.volume101en_US
dc.identifier.wosWOS:000527127700003
dc.identifier.wosqualityQ1
dc.institutionauthorSaraç Oymak, Yasemin
dc.language.isoenen_US
dc.publisherAmer Physical Socen_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.titleΛ<i><sub>b</sub></i>(6146)<SUP>0</SUP> state newly observed by LHCben_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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