Global Ashkin-Teller phase diagrams in two and three dimensions: Multicritical bifurcation versus double tricriticality-endpoint
dc.authorid | Kecoglu, Ibrahim/0000-0002-2141-8401 | |
dc.authorid | Berker, A/0000-0002-5172-2172 | |
dc.authorscopusid | 57219371537 | |
dc.authorscopusid | 6701401118 | |
dc.contributor.author | Berker, Ahmet Nihat | |
dc.contributor.author | Berker, A. Nihat | |
dc.date.accessioned | 2024-06-23T21:38:26Z | |
dc.date.available | 2024-06-23T21:38:26Z | |
dc.date.issued | 2023 | |
dc.department | Kadir Has University | en_US |
dc.department-temp | [Kecoglu, Ibrahim] Bogazici Univ, Dept Phys, TR-34342 Istanbul, Turkiye; [Kecoglu, Ibrahim] Bogazici Univ, Dept Math, TR-34342 Istanbul, Turkiye; [Berker, A. Nihat] Kadir Has Univ, Fac Engn & Nat Sci, TR-34083 Istanbul, Turkiye; [Berker, A. Nihat] TUBITAK Res Inst Fundamental Sci, TR-41470 Gebze, Kocaeli, Turkiye; [Berker, A. Nihat] MIT, Dept Phys, Cambridge, MA 02139 USA | en_US |
dc.description | Kecoglu, Ibrahim/0000-0002-2141-8401; Berker, A/0000-0002-5172-2172 | en_US |
dc.description.abstract | The global phase diagrams of the Ashkin-Teller model are calculated in d = 2 and 3 by renormalization-group theory that is exact on the hierarchical lattice and approximate on the recently improved Migdal-Kadanoff procedure. Three different ordered phases occur in the dimensionally distinct phase diagrams that reflect three-fold order-parameter permutation symmetry, a closed symmetry line, and a quasi-disorder line. First- and second-order phase boundaries are obtained. In d = 2, second-order phase transitions meeting at a bifurcation point are seen. In d = 3, first- and second-order phase transitions are separated by tricritical and critical endpoints. | en_US |
dc.description.sponsorship | Academy of Sciences of Turkey (TUEBA) | en_US |
dc.description.sponsorship | Support by the Academy of Sciences of Turkey (TUEBA) is gratefully acknowledged. | en_US |
dc.identifier.citation | 0 | |
dc.identifier.doi | 10.1016/j.physa.2023.129248 | |
dc.identifier.issn | 0378-4371 | |
dc.identifier.issn | 1873-2119 | |
dc.identifier.scopus | 2-s2.0-85173582720 | |
dc.identifier.scopusquality | Q2 | |
dc.identifier.uri | https://doi.org/10.1016/j.physa.2023.129248 | |
dc.identifier.uri | https://hdl.handle.net/20.500.12469/5798 | |
dc.identifier.volume | 630 | en_US |
dc.identifier.wos | WOS:001099292000001 | |
dc.identifier.wosquality | Q2 | |
dc.language.iso | en | en_US |
dc.publisher | Elsevier | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | First and second-order phase transitions | en_US |
dc.subject | Bifurcation, tricritical, critical-end points | en_US |
dc.subject | Exact renormalization-group solution | en_US |
dc.subject | Hierarchical lattices in d=2 and 3 | en_US |
dc.subject | Ashkin-Teller spin model | en_US |
dc.title | Global Ashkin-Teller phase diagrams in two and three dimensions: Multicritical bifurcation versus double tricriticality-endpoint | en_US |
dc.type | Article | en_US |
dspace.entity.type | Publication | |
relation.isAuthorOfPublication | db2f6241-4861-48d5-b8ca-f0482a4d86b3 | |
relation.isAuthorOfPublication.latestForDiscovery | db2f6241-4861-48d5-b8ca-f0482a4d86b3 |