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dc.contributor.authorÇağlar, Tolga
dc.contributor.authorBerker, A. Nihat
dc.date.accessioned2019-06-27T08:01:15Z
dc.date.available2019-06-27T08:01:15Z
dc.date.issued2017
dc.identifier.issn2470-0045en_US
dc.identifier.issn2470-0053en_US
dc.identifier.urihttps://hdl.handle.net/20.500.12469/318
dc.identifier.urihttps://doi.org/10.1103/PhysRevE.96.032103
dc.description.abstractThe left-right chiral and ferromagnetic-antiferromagnetic double-spin-glass clock model with the crucially even number of states q = 4 and in three dimensions d = 3 has been studied by renormalization-group theory. We find for the first time to our knowledge four spin-glass phases including conventional chiral and quadrupolar spin-glass phases and phase transitions between spin-glass phases. The chaoses in the different spin-glass phases and in the phase transitions of the spin-glass phases with the other spin-glass phases with the non-spin-glass ordered phases and with the disordered phase are determined and quantified by Lyapunov exponents. It is seen that the chiral spin-glass phase is the most chaotic spin-glass phase. The calculated phase diagram is also otherwise very rich including regular and temperature-inverted devil's staircases and reentrances.en_US]
dc.language.isoengen_US
dc.publisherAmer Physical Soc.en_US
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.subjectN/Aen_US
dc.titlePhase transitions between different spin-glass phases and between different chaoses in quenched random chiral systemsen_US
dc.typearticleen_US
dc.relation.journalPhysical Review Een_US
dc.identifier.issue3
dc.identifier.volume96en_US
dc.departmentFakülteler, Mühendislik ve Doğa Bilimleri Fakültesi, Elektrik-Elektronik Mühendisliği Bölümüen_US
dc.identifier.wosWOS:000409261800003en_US
dc.identifier.doi10.1103/PhysRevE.96.032103en_US
dc.identifier.scopus2-s2.0-85029915044en_US
dc.institutionauthorBerker, A. Nihaten_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.identifier.pmid29346860en_US


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