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Disorder-induced rounding of certain quantum phase transitions.

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TLDR
The influence of quenched disorder on quantum phase transitions in systems with overdamped dynamics is studied and the behavior based on Lifshitz-tail arguments is discussed and illustrated by simulations of a model system.
Abstract
We study the influence of quenched disorder on quantum phase transitions in systems with over-damped dynamics. For Ising order-parameter symmetry disorder destroys the sharp phase transition by rounding because a static order parameter can develop on rare spatial regions. This leads to an exponential dependence of the order parameter on the coupling constant. At finite temperatures the static order on the rare regions is destroyed. This restores the phase transition and leads to a double-exponential relation between critical temperature and coupling strength. We discuss the behavior based on Lifshitz-tail arguments and illustrate the results by simulations of a model system.

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Fermi-liquid instabilities at magnetic quantum phase transitions

TL;DR: In this article, the authors discuss the instabilities of the Fermi-liquid state of conduction electrons in metals with particular emphasis on magnetic quantum critical points, with the aim of assessing the validity of presently available theory.
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Quantum phase transitions

TL;DR: A review of quantum phase transitions in condensed matter physics can be found in this article, where the authors introduce important concepts of phase transitions and discuss the interplay of quantum and classical fluctuations near criticality.
Journal ArticleDOI

Rare region effects at classical, quantum and nonequilibrium phase transitions

Thomas Vojta
- 16 May 2006 - 
TL;DR: In this paper, a unified framework for rare region effects at weakly disordered classical, quantum and nonequilibrium phase transitions based on the effective dimensionality of the rare regions is presented.
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How Generic Scale Invariance Influences Quantum and Classical Phase Transitions

TL;DR: In this article, the authors discuss a paradigm that has become of increasing importance in the theory of quantum phase transitions, namely, the coupling of the order-parameter fluctuations to other soft modes and the resulting impossibility of constructing a simple Landau-Ginzburg-Wilson theory in terms of order parameter only.
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Emergence of coherence and the dynamics of quantum phase transitions

TL;DR: This work investigates in detail how coherence emerges when an initially incoherent Mott insulating system enters the superfluid regime and performs a largely certified analog quantum simulation of this strongly correlated system reaching beyond the regime of free quasiparticles.
References
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Journal ArticleDOI

Quantum phase transitions

TL;DR: The universe itself is thought to have passed through several phase transitions as the high-temperature plasma formed by the big bang cooled to form the world as we know it today as mentioned in this paper.
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Quantum critical phenomena

TL;DR: In this paper, the authors proposed an approach to the study of critical phenomena in quantum-mechanical systems at zero or low temperatures, where classical free-energy functionals of the Landau-Ginzburg-Wilson sort are not valid.
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Effect of random defects on the critical behaviour of Ising models

TL;DR: In this article, a cumulant expansion is used to calculate the transition temperature of simple-square Ising models with random-bond defects, and the results are -Tc-1 dTc/dx mod x=0.329 compared with the mean-field value of one.
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Nonanalytic Behavior Above the Critical Point in a Random Ising Ferromagnet

TL;DR: In this paper, it was shown that in a class of randomly diluted Ising ferromagnets the magnetization fails to be an analytic function of the field at a range of temperatures above that at which spontaneous magnetization first appears.
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Continuous quantum phase transitions

TL;DR: In this paper, a scaling analysis of Josephson-junction arrays and quantum Hall-effect systems is presented, where the authors derive scaling forms for the finite-temperature behavior, which turns out to be described by the theory of finite size scaling.