Triangular lattice gas with first- and second-neighbor exclusions: Continuous transition in the four-state Potts universality class

dc.contributor.authorBartelt, N. C.
dc.contributor.authorEinstein, Theodore L.
dc.date.accessioned2024-03-11T15:55:25Z
dc.date.available2024-03-11T15:55:25Z
dc.date.issued1984
dc.description.abstractUsing phenomenological renormalization (transfer-matrix scaling), we have reexamined the phase transition of a triangular lattice gas with particles having both nearest- and second-nearest-neighbor exclusions. Widely accepted classical studies indicated that disordering of the ordered (p(2x2)) state is first order. In contradiction, we show that the transition is second order; its exponents are consistent with the four-state Potts model universality class, in accord with its Landau-Ginzburg-Wilson Hamiltonian classification.
dc.description.urihttps://doi.org/10.1103/PhysRevB.30.5339
dc.identifierhttps://doi.org/10.13016/fsgx-gbj6
dc.identifier.citationBartelt, N. C. & Einstein, T. L., Triangular lattice gas with first- and second-neighbor exclusions: Continuous transition in the four-state Potts universality class. Physical Review B, 30, 9, 5339-5341, 1984.
dc.identifier.urihttp://hdl.handle.net/1903/32349
dc.publisherAmerican Physical Society
dc.titleTriangular lattice gas with first- and second-neighbor exclusions: Continuous transition in the four-state Potts universality class
dc.typeArticle

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