New Λ<i><sub>b</Sub>< State as a 2<i>s</I> Bottom Baryon

dc.authoridAzizi, Kazem/0000-0003-3741-2167
dc.authorscopusid17345170000
dc.authorscopusid24391488900
dc.authorscopusid6508230150
dc.authorwosidSundu, Hayriye/A-5128-2018
dc.authorwosidAzizi, Kazem/ABE-4757-2021
dc.contributor.authorAzizi, K.
dc.contributor.authorSarac, Y.
dc.contributor.authorSundu, H.
dc.contributor.otherPhysics Group
dc.date.accessioned2024-07-05T15:39:31Z
dc.date.available2024-07-05T15:39:31Z
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.abstractAs a result of continuous developments, the recent experimental searches lead to the observations of new particles at different hadronic channels. Among these hadrons are the excited states of the heavy baryons containing single bottom or charmed quark in their valance quark content. The recently observed Lambda(b)(6072)(0) state is one of these baryons and possibly 2S radial excitation of the Lambda(b) state. Considering this information from the experiment, we conduct a QCD sum rule analysis on this state and calculate its mass and current coupling constant considering it as a 2S radially excited Lambda(b) resonance. For completeness, in the analyses, we also compute the mass and current coupling constant for the ground state Lambda(0)(b) and its first orbital excitation. We also consider the Lambda(+)(c) counterpart of each state and attain their mass, as well. The obtained results are consistent with the experimental data as well as existing theoretical predictions.en_US
dc.identifier.citationcount13
dc.identifier.doi10.1103/PhysRevD.102.034007
dc.identifier.issn2470-0010
dc.identifier.issn2470-0029
dc.identifier.issue3en_US
dc.identifier.scopus2-s2.0-85089894866
dc.identifier.scopusqualityQ1
dc.identifier.urihttps://doi.org/10.1103/PhysRevD.102.034007
dc.identifier.urihttps://hdl.handle.net/20.500.14411/3235
dc.identifier.volume102en_US
dc.identifier.wosWOS:000557297800001
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.scopus.citedbyCount11
dc.subject[No Keyword Available]en_US
dc.titleNew Λ<i><sub>b</Sub>< State as a 2<i>s</I> Bottom Baryonen_US
dc.typeArticleen_US
dc.wos.citedbyCount12
dspace.entity.typePublication
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