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dc.contributor.authorARIK, M
dc.contributor.authorCELIK, S
dc.date.accessioned2025-01-09T20:14:06Z
dc.date.available2025-01-09T20:14:06Z
dc.date.issued1993
dc.identifier.issn0170-9739
dc.identifier.urihttps://doi.org/10.1007/BF01555843
dc.identifier.urihttps://hdl.handle.net/20.500.14124/8735
dc.description.abstractWe discuss the parametrization of quantum groups in terms of independent operators. We find that this consideration leads to the parametrization of SU(q)(2) in terms of a q-oscillator plus a commuting phase. The commuting phase is naturally identified with the subgroup U(1)and the remaining coset SU(q)(2)/U(1)=CP(q)(1) consists of a q-oscillator. For unitary quantum groups SU(q)(n), the analogous construction results in the quantum projective space SU(q)(n + 1)/U(q)(n)=CP(q)(n) being identified with the n-dimensional q-oscillator. This yields a nonlinear action of the quantum group SU(q)(n + 1) on the n-dimensional q-oscillator.en_US
dc.language.isoengen_US
dc.publisherSpringer Verlagen_US
dc.relation.ispartofZeitschrift Fur Physik C-Particles and Fieldsen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.titleUNITARY QUANTUM GROUPS, QUANTUM PROJECTIVE SPACES AND Q-OSCILLATORSen_US
dc.typearticleen_US
dc.authoridCelik, Salih/0000-0002-6590-1032
dc.departmentMimar Sinan Güzel Sanatlar Üniversitesien_US
dc.identifier.doi10.1007/BF01555843
dc.identifier.volume59en_US
dc.identifier.issue1en_US
dc.identifier.startpage99en_US
dc.identifier.endpage103en_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.identifier.wosqualityN/A
dc.identifier.wosWOS:A1993LN25100010
dc.identifier.scopus2-s2.0-0002102336
dc.identifier.scopusqualityQ1
dc.indekslendigikaynakWeb of Scienceen_US
dc.indekslendigikaynakScopusen_US
dc.snmzKA_20250105


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