Spin-Glass Phases and Multichaos in the Ashkin–Teller Model

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2026

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Elsevier Ltd

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Yes

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Abstract

The global phase diagram of the Ashkin–Teller spin glass is calculated in d=3 spatial dimensions by renormalization-group theory. Depending on the value of the positive or negative four-spin interaction, qualitatively different topologies are found for the spin-glass phase diagram in the usual variables of temperature and fraction of antiferromagnetic nearest-neighbor interactions. Two different spin-glass phases occur. Both spin-glass phases are chaotic. One spin-glass exhibits phase reentrance that is reverse from the reentrances seen in previous spin-glass phase diagrams. Seven different phases: Ferromagnetic and antiferromagnetic, entropic ferromagnetic and entropic antiferromagnetic, spin-glass and entropic spin-glass, and disordered phases occur. The entropic ferromagnetic phase unusually but understandably occurs at temperatures above one spin-glass phase. A random disorder line is identified and no phase transition occurs on this line. Our calculation is exact on the d = 3 hierarchical lattice and Migdal–Kadanoff approximate on the cubic lattice. © 2025 Elsevier Ltd.

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Keywords

Ashkin–Teller Spin-Glass in D=3, Chaotic Renormalization-Group Trajectories, Entropic Ferromagnetism and Antiferromagnetism, Qualitatively Different Phase Diagram Topologies, Renormalization-Group Theory, Two Different Chaotic Spin-Glasses, Lyapunov Exponents, Statistical Mechanics (cond-mat.stat-mech), FOS: Physical sciences, Disordered Systems and Neural Networks (cond-mat.dis-nn), Disordered Systems and Neural Networks, Statistical Mechanics

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Chaos Solitons & Fractals

Volume

202

Issue

Start Page

117458

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