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dc.contributor.authorCan, K. U.
dc.contributor.authorOka, M.
dc.contributor.authorErkol, Güray
dc.contributor.authorTakahashi, T. T.
dc.date.accessioned2017-01-31T12:50:26Z
dc.date.available2017-01-31T12:50:26Z
dc.date.issued2015
dc.identifier.issn1824-8039en_US
dc.identifier.urihttp://hdl.handle.net/10679/4761
dc.description.abstractThe electromagnetic form factors of the spin-3/2 Ω baryons, namely the Ω, Ω∗c , Ω∗ cc and Ωccc, are calculated in full QCD on 323 x 64 PACS-CS lattices with a pION mass of 156(9) MeV. The electric charge radii and magnetic moments from the E0 and M1 multipole form factors are extracted. Results for the electric quadrupole form factor, E2, are also provided. Quark sector contributions are computed individually for each observable and then combined to obtain the baryon properties. Charm quark contributions are observed to be systematically smaller compared to the strange quark contributions in case of the charge radii and magnetic moments. E2 moments of the Ω∗ cc and Ωccc are estimated significantly enough to show that their electric charge distributions are deformed. Properties of the spin-1/2 counterparts of the Ω∗ cc and Ω∗ cc baryons are also computed and a comparison is presented.en_US
dc.language.isoengen_US
dc.relation.ispartofLATTICE 2015en_US
dc.rightsrestrictedAccess
dc.titleElectromagnetic structure of charmed baryons - extended to spin-3/2en_US
dc.typeConference paperen_US
dc.publicationstatuspublisheden_US
dc.contributor.departmentÖzyeğin University
dc.contributor.authorID(ORCID 0000-0002-7814-7681 & YÖK ID 44764) Erkol, Güray
dc.contributor.ozuauthorErkol, Güray
dc.subject.keywordsApproximation theoryen_US
dc.subject.keywordsCharge distributionen_US
dc.subject.keywordsElectric chargeen_US
dc.subject.keywordsElectric dischargesen_US
dc.subject.keywordsElementary particlesen_US
dc.subject.keywordsHadronsen_US
dc.identifier.scopusSCOPUS:2-s2.0-84988643169
dc.contributor.authorMale1
dc.relation.publicationcategoryConference Paper - International - Institutional Academic Staff


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