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Three-Qubit Quantum Entanglement For Si (S = 3/2, I = 1/2) Spin System

dc.contributor.authorGun, A.
dc.contributor.authorGencten, A.
dc.date.accessioned2020-06-21T14:30:08Z
dc.date.available2020-06-21T14:30:08Z
dc.date.issued2011
dc.identifier.issn0219-7499
dc.identifier.urihttps://doi.org/10.1142/S0219749911008313
dc.identifier.urihttps://hdl.handle.net/20.500.12712/16984
dc.descriptionWOS: 000297939700006en_US
dc.description.abstractIn quantum information processing, spin-3/2 electron or nuclear spin states are known as two-qubit states. For SI (S = 3/2; I = 1/2) spin system, there are eight three-qubit states. In this study, first, three-qubit CNOT logic gates are obtained. Then three-qubit entangled states are obtained by using the matrix representation of Hadamard and three-qubit CNOT logic gates. By considering single (31)P@C(60) molecule as SI (S = 3/2; I = 1/2) spin system, three-qubit entangled states are also obtained using the magnetic resonance pulse sequences of Hadamard and CNOT logic gates.en_US
dc.language.isoengen_US
dc.publisherWorld Scientific Publ Co Pte Ltden_US
dc.relation.isversionof10.1142/S0219749911008313en_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectThree-qubit statesen_US
dc.subjectthree-qubit CNOTen_US
dc.subjectquantum entanglementen_US
dc.subjectendohedral fullerenesen_US
dc.subjectmagnetic resonance selective pulsesen_US
dc.titleThree-Qubit Quantum Entanglement For Si (S = 3/2, I = 1/2) Spin Systemen_US
dc.typearticleen_US
dc.contributor.departmentOMÜen_US
dc.identifier.volume9en_US
dc.identifier.issue07.Augen_US
dc.identifier.startpage1635en_US
dc.identifier.endpage1642en_US
dc.relation.journalInternational Journal of Quantum Informationen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US


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