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Strong Disorder RG approach - a short review of recent developments
Disordered Systems and Neural Networks · Submitted 20 Jun 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The Strong Disorder RG approach for random systems has been extended in many new directions since our previous review of 2005 [Phys. Rep. 412, 277].
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The abstract, sentence by sentence
The Strong Disorder RG approach for random systems has been extended in many new directions since our previous review of 2005 [Phys. Rep. 412, 277]. The aim of the present colloquium paper is thus to give an overview of these various recent developments. In the field of quantum disordered models, recent progress concern Infinite Disorder Fixed Points for short-ranged models in higher dimensions $d>1$, Strong Disorder Fixed Points for long-ranged models, scaling of the entanglement entropy in critical ground-states and after quantum quenches, the RSRG-X procedure to construct the whole set excited stated and the RSRG-t procedure for the unitary dynamics in Many-Body-Localized Phases, the Floquet dynamics of periodically driven chains, the dissipative effects induced by the coupling to external baths, and Anderson Localization models. In the field of classical disordered models, new applications include the contact process for epidemic spreading, the strong disorder renormalization procedure for general master equations, the localization properties of random elastic networks and the synchronization of interacting non-linear dissipative oscillators.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The Strong Disorder RG approach for random systems has been extended in many new directions since our previous review of 2005 [Phys. Rep. 412, 277]. | background 1.00 | 0.09 | 0.05 | asserted 1.00 |
| s1 | The aim of the present colloquium paper is thus to give an overview of these various recent developments. | contribution 0.92 | 0.14 | 0.07 | asserted 0.89 |
| s2 | In the field of quantum disordered models, recent progress concern Infinite Disorder Fixed Points for short-ranged models in higher dimensions $d>1$, Strong Disorder Fixed Points for long-ranged models, scaling of the entanglement entropy in critical ground-states and after quantum quenches, the RSRG-X procedure to construct the whole set excited stated and the RSRG-t procedure for the unitary dynamics in Many-Body-Localized Phases, the Floquet dynamics of periodically driven chains, the dissipative effects induced by the coupling to external baths, and Anderson Localization models. | contribution 0.76 | 0.07 | 0.09 | asserted 1.00 |
| s3 | In the field of classical disordered models, new applications include the contact process for epidemic spreading, the strong disorder renormalization procedure for general master equations, the localization properties of random elastic networks and the synchronization of interacting non-linear dissipative oscillators. | contribution 0.88 | 0.09 | 0.04 | asserted 0.99 |
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The paper
Original abstract
The Strong Disorder RG approach for random systems has been extended in many new directions since our previous review of 2005 [Phys. Rep. 412, 277]. The aim of the present colloquium paper is thus to give an overview of these various recent developments. In the field of quantum disordered models, recent progress concern Infinite Disorder Fixed Points for short-ranged models in higher dimensions $d>1$, Strong Disorder Fixed Points for long-ranged models, scaling of the entanglement entropy in critical ground-states and after quantum quenches, the RSRG-X procedure to construct the whole set excited stated and the RSRG-t procedure for the unitary dynamics in Many-Body-Localized Phases, the Floquet dynamics of periodically driven chains, the dissipative effects induced by the coupling to external baths, and Anderson Localization models. In the field of classical disordered models, new applications include the contact process for epidemic spreading, the strong disorder renormalization procedure for general master equations, the localization properties of random elastic networks and the synchronization of interacting non-linear dissipative oscillators.
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How the literature uses it
8 arXiv papers cite this in 10 sentences
Papers citing it · 5 sentences without a confident label
Uses its method or tool 1 paper
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We provide numerical evidence for this behavior by using the Strong Disorder Renormalization Group (SDRG) method [ref] (see also [ref] ).
Unusual area-law violation in random inhomogeneous systems · Introduction · 1.00
Cites it as background 4 papers
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As a result, several phenomenological renormalization group (RG) approaches have been proposed [ref] , based on various physical assumptions on thermalization and random matrix theory.
Multiscale entanglement clusters at the many-body localization phase transition · Introduction · 0.91
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The corresponding Infinite Disorder character of the transition is reviewed in [ref] .
Topological phase transitions in random Kitaev $\alpha$-chains · Example $H=H_0+H_1$ · 0.80
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We do not intend to provide a full review of SDRG studies of the TFIM (see Refs. [ref] for a guide to the SDRG literature on this and related systems) but would like to mention two approaches to modified SDRG schemes which drop a number of bonds produced by spin decimations and have strongly influenced this work.
Random geometry at an infinite-randomness fixed point · Two dimensions · 0.99
What it cites · 19 sentences without a confident label
Cites as background 2 papers
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In the presence of interactions, the issue of Many-Body-Localization in isolated random quantum spin chains has attracted a lot of attention recently, as reviewed in [ref] .
Many-body localization, thermalization, and entanglement · Localized and Many-Body-Localized Phases of quantum spin chains · 0.94
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The properties of the Griffiths phases can be interpreted in terms of rare regions, as reviewed in [ref] .
Phases and phase transitions in disordered quantum systems · Griffiths phases - strong disorder fixed points · 0.91
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