Strong-randomness infinite-coupling phase in a random quantum spin chain
arXiv:1310.4864 · doi:10.1103/PhysRevB.89.014401
Abstract
We study the ground-state phase diagram of the Ashkin-Teller random quantum spin chain by means of a generalization of the strong-disorder renormalization group. In addition to the conventional paramagnetic and ferromagnetic (Baxter) phases, we find a partially ordered phase characterized by strong randomness and infinite coupling between the colors. This unusual phase acts, at the same time, as a Griffiths phase for two distinct quantum phase transitions both of which are of infinite-randomness type. We also investigate the quantum multi-critical point that separates the two-phase and three-phase regions; and we discuss generalizations of our results to higher dimensions and other systems.
9 pages, 6 eps figures, final version as published
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- Strong-randomness phenomena in quantum Ashkin-Teller models
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- Numerical evidence of the double-Griffiths phase of the random quantum Ashkin-Teller chain
- Monte Carlo simulations of the disordered three-color quantum Ashkin-Teller chain
- Numerical evidence of a super-universality of the 2D and 3D random quantum Potts models
- Numerical evidences of a universal critical behavior of 2D and 3D random quantum clock and Potts models
- Improved Matrix Product Operator Renormalization Group: application to the N-color random Ashkin-Teller chain
- Emerging critical behavior at a first-order phase transition rounded by disorder
- Large Disorder Renormalization Group Study of the Anderson Model of Localization
- Smeared phase transition in the dissipative random quantum Ashkin-Teller model