Axial, planar-diagonal, body-diagonal fields on the cubic-spin spin glass in d=3: A plethora of ordered phases under finite fields

dc.authorscopusid 57219631900
dc.authorscopusid 58685682100
dc.authorscopusid 6701401118
dc.contributor.author Berker, Ahmet Nihat
dc.contributor.author Sarman, Deniz
dc.contributor.author Berker, A. Nihat
dc.contributor.other Electrical-Electronics Engineering
dc.date.accessioned 2024-10-15T19:40:34Z
dc.date.available 2024-10-15T19:40:34Z
dc.date.issued 2024
dc.department Kadir Has University en_US
dc.department-temp [Artun, E. Can; Berker, A. Nihat] TUBITAK Res Inst Fundamental Sci, TR-41470 Kocaeli, Turkiye; [Artun, E. Can; Berker, A. Nihat] Kadir Has Univ, Fac Engn & Nat Sci, TR-34083 Istanbul, Turkiye; [Sarman, Deniz] Bogazici Univ, Dept Phys, TR-34342 Istanbul, Turkiye; [Berker, A. Nihat] MIT, Dept Phys, Cambridge, MA 02139 USA en_US
dc.description.abstract A nematic phase, previously seen in the d = 3 classical Heisenberg spin-glass system, occurs in the n-component cubic-spin spin-glass system, between the low-temperature spin-glass phase and the hightemperature disordered phase, for number of spin components n >= 3, in spatial dimension d = 3, thus constituting a liquid-crystal phase in a dirty (quenched-disordered) magnet. Furthermore, under application of a variety of uniform magnetic fields, a veritable plethora of phases is found. Under uniform magnetic fields, 17 different phases and two spin-glass phase diagram topologies (meaning the occurrences and relative positions of the many phases), qualitatively different from the conventional spin-glass phase diagram topology, are seen. The chaotic rescaling behaviors and their Lyapunov exponents are calculated in each of these spin-glass phase diagram topologies. These results are obtained from renormalization-group calculations that are exact on the d = 3 hierarchical lattice and, equivalently, approximate on the cubic spatial lattice. Axial, planar-diagonal, or body-diagonal finite-strength uniform fields are applied to n = 2 and 3 component cubic-spin spin-glass systems in d=3. en_US
dc.description.sponsorship Kadir Has University Doctoral Studies Scholarship Fund; Academy of Sciences of Turkey (TUEBA) en_US
dc.description.sponsorship Support by the Kadir Has University Doctoral Studies Scholarship Fund and by the Academy of Sciences of Turkey (TUEBA) is gratefully acknowledged. en_US
dc.description.woscitationindex Science Citation Index Expanded
dc.identifier.citationcount 0
dc.identifier.doi 10.1103/PhysRevE.110.034123
dc.identifier.issn 2470-0045
dc.identifier.issn 2470-0053
dc.identifier.issue 3 en_US
dc.identifier.scopus 2-s2.0-85204582129
dc.identifier.scopusquality Q2
dc.identifier.uri https://doi.org/10.1103/PhysRevE.110.034123
dc.identifier.uri https://hdl.handle.net/20.500.12469/6373
dc.identifier.volume 110 en_US
dc.identifier.wos WOS:001317697300002
dc.identifier.wosquality Q1
dc.language.iso en en_US
dc.publisher Amer Physical Soc en_US
dc.relation.publicationcategory Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı en_US
dc.rights info:eu-repo/semantics/closedAccess en_US
dc.scopus.citedbyCount 0
dc.subject [No Keyword Available] en_US
dc.title Axial, planar-diagonal, body-diagonal fields on the cubic-spin spin glass in d=3: A plethora of ordered phases under finite fields en_US
dc.type Article en_US
dc.wos.citedbyCount 0
dspace.entity.type Publication
relation.isAuthorOfPublication db2f6241-4861-48d5-b8ca-f0482a4d86b3
relation.isAuthorOfPublication.latestForDiscovery db2f6241-4861-48d5-b8ca-f0482a4d86b3
relation.isOrgUnitOfPublication 12b0068e-33e6-48db-b92a-a213070c3a8d
relation.isOrgUnitOfPublication.latestForDiscovery 12b0068e-33e6-48db-b92a-a213070c3a8d

Files