Strong-Randomness Phenomena in Quantum Ashkin-Teller Models


The N-color quantum Ashkin-Teller spin chain is a prototypical model for the study of strong-randomness phenomena at first-order and continuous quantum phase transitions. In this paper, we first review the existing strong-disorder renormalization group approaches to the random quantum Ashkin-Teller chain in the weak-coupling as well as the strong-coupling regimes. We then introduce a novel general variable transformation that unifies the treatment of the strong-coupling regime. This allows us to determine the phase diagram for all color numbers N, and the critical behavior for all N ≠ 4. In the case of two colors, N = 2, a partially ordered product phase separates the paramagnetic and ferromagnetic phases in the strong-coupling regime. This phase is absent for all N > 2, i.e., there is a direct phase boundary between the paramagnetic and ferromagnetic phases. In agreement with the quantum version of the Aizenman-Wehr theorem, all phase transitions are continuous, even if their clean counterparts are of first order. We also discuss the various critical and multicritical points. They are all of infinite-randomness type, but depending on the coupling strength, they belong to different universality classes.



Research Center/Lab(s)

Center for High Performance Computing Research

Keywords and Phrases

Critical Behaviour; Disordered Systems; First-Order Phase Transition; Quantum Phase Transition

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Document Type

Article - Journal

Document Version


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© 2015 Institute of Physics - IOP Publishing, All rights reserved.

Publication Date

01 Oct 2015