Stepwise Positional-Orientational Order and the Multicritical-Multistructural Global Phase Diagram of the s=3/2 Ising Model From Renormalization-Group Theory
dc.citation.epage | 9 | en_US |
dc.citation.issueNumber | 6 | en_US |
dc.citation.spage | 1 | en_US |
dc.citation.volumeNumber | 93 | en_US |
dc.contributor.author | Yunus, Ç. | en_US |
dc.contributor.author | Renklioǧlu, B. | en_US |
dc.contributor.author | Keskin, M. | en_US |
dc.contributor.author | Berker, A. N. | en_US |
dc.date.accessioned | 2018-04-12T10:43:37Z | |
dc.date.available | 2018-04-12T10:43:37Z | |
dc.date.issued | 2016 | en_US |
dc.department | Department of Physics | en_US |
dc.description.abstract | The spin-32 Ising model, with nearest-neighbor interactions only, is the prototypical system with two different ordering species, with concentrations regulated by a chemical potential. Its global phase diagram, obtained in d=3 by renormalization-group theory in the Migdal-Kadanoff approximation or equivalently as an exact solution of a d=3 hierarchical lattice, with flows subtended by 40 different fixed points, presents a very rich structure containing eight different ordered and disordered phases, with more than 14 different types of phase diagrams in temperature and chemical potential. It exhibits phases with orientational and/or positional order. It also exhibits quintuple phase transition reentrances. Universality of critical exponents is conserved across different renormalization-group flow basins via redundant fixed points. One of the phase diagrams contains a plastic crystal sequence, with positional and orientational ordering encountered consecutively as temperature is lowered. The global phase diagram also contains double critical points, first-order and critical lines between two ordered phases, critical end points, usual and unusual (inverted) bicritical points, tricritical points, multiple tetracritical points, and zero-temperature criticality and bicriticality. The four-state Potts permutation-symmetric subspace is contained in this model. | en_US |
dc.identifier.doi | 10.1103/PhysRevE.93.062113 | en_US |
dc.identifier.issn | 2470-0045 | |
dc.identifier.uri | http://hdl.handle.net/11693/36539 | |
dc.language.iso | English | en_US |
dc.publisher | American Physical Society | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1103/PhysRevE.93.062113 | en_US |
dc.source.title | Physical Review E | en_US |
dc.subject | Chemical potential | en_US |
dc.subject | Group theory | en_US |
dc.subject | Ising model | en_US |
dc.subject | Lattice theory | en_US |
dc.subject | Statistical mechanics | en_US |
dc.subject | Double critical point | en_US |
dc.subject | Global phase diagrams | en_US |
dc.subject | Migdal-Kadanoff approximation | en_US |
dc.subject | Nearest-neighbor interactions | en_US |
dc.subject | Orientational orderings | en_US |
dc.subject | Renormalization group | en_US |
dc.subject | Renormalization group theory | en_US |
dc.subject | Tetracritical points | en_US |
dc.subject | Phase diagrams | en_US |
dc.title | Stepwise Positional-Orientational Order and the Multicritical-Multistructural Global Phase Diagram of the s=3/2 Ising Model From Renormalization-Group Theory | en_US |
dc.type | Article | en_US |
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