2006
DOI: 10.1088/0305-4470/39/22/r01
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Rare region effects at classical, quantum and nonequilibrium phase transitions

Abstract: Rare regions, i.e., rare large spatial disorder fluctuations, can dramatically change the properties of a phase transition in a quenched disordered system. In generic classical equilibrium systems, they lead to an essential singularity, the so-called Griffiths singularity, of the free energy in the vicinity of the phase transition. Stronger effects can be observed at zero-temperature quantum phase transitions, at nonequilibrium phase transitions, and in systems with correlated disorder. In some cases, rare reg… Show more

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Cited by 428 publications
(699 citation statements)
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References 293 publications
(564 reference statements)
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“…Furthermore, when k-dependent weighting was also applied, suppressing hubs or making the network disassortative, GP-like regions could be observed in the simulations. A systematic finite scaling study revealed that these power-laws saturate in the N → ∞ thermodynamic limit, suggesting smeared phase transitions [25]. This can be understood via the possibility of embedding even infinite dimensional, active RR-s in networks with d = ∞, leading to finite steady-state density: ρ(t → ∞,N → ∞).…”
Section: Introductionmentioning
confidence: 98%
See 1 more Smart Citation
“…Furthermore, when k-dependent weighting was also applied, suppressing hubs or making the network disassortative, GP-like regions could be observed in the simulations. A systematic finite scaling study revealed that these power-laws saturate in the N → ∞ thermodynamic limit, suggesting smeared phase transitions [25]. This can be understood via the possibility of embedding even infinite dimensional, active RR-s in networks with d = ∞, leading to finite steady-state density: ρ(t → ∞,N → ∞).…”
Section: Introductionmentioning
confidence: 98%
“…An independent cause is related to arbitrarily large (l < N), active rare-regions (RR) with long lifetimes: τ ∝ exp(l) in the inactive phase (λ λ c ). In the region λ 0 c < λ < λ c , where λ 0 c is the critical point of the impure system, a so-called Griffiths phase (GP) [24,25] develops, with algebraic density decay ρ ∝ t −α , α being a nonuniversal exponent. At and below the λ 0 c rare clusters may still form, with an over-average mean degree, which are locally supercritical at a given λ and induce a slower-than-exponential but fasterthan-power-law decay of the global density.…”
Section: Introductionmentioning
confidence: 99%
“…Ref. [56] for a review. At some phase transitions, such as the quantum phase transition from a magnetically disordered to a magnetically ordered phase in the random transverse-field Ising spin chain, the leading divergences near the phase transition are due to such Griffiths effects [57].…”
Section: Introductionmentioning
confidence: 99%
“…The action is given by the DBI for the probe D5-brane, and takes the form 6) where the tilde and the dot denote a partial derivative with respect to z and x respectively. The equations of motion for χ(z, x) and φ(z, x) follow readily from this action, and they have been written explicitly in the appendix of [24].…”
Section: Jhep07(2016)091mentioning
confidence: 99%
“…At the theoretical level it poses important questions as the existence and nature of disordered quantum critical points [5,6], and the possibility of disorder-induced metal to insulator phase transitions for strongly interacting systems.…”
Section: Introductionmentioning
confidence: 99%