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Large Disorder Renormalization Group Study of the Anderson Model of Localization
Disordered Systems and Neural Networks · Submitted 21 May 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that our LDRG scheme flows to infinite disorder, and thus becomes asymptotically exact.
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The abstract, sentence by sentence
We describe a large disorder renormalization group (LDRG) method for the Anderson model of localization in one dimension which decimates eigenstates based on the size of their wavefunctions rather than their energy. We show that our LDRG scheme flows to infinite disorder, and thus becomes asymptotically exact. We use it to obtain the disorder-averaged inverse participation ratio and density of states for the entire spectrum. A modified scheme is formulated for higher dimensions, which is found to be less efficient, but capable of improvement.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We describe a large disorder renormalization group (LDRG) method for the Anderson model of localization in one dimension which decimates eigenstates based on the size of their wavefunctions rather than their energy. | method 0.84 | 0.92 | 0.09 | asserted 1.00 |
| s1 | We show that our LDRG scheme flows to infinite disorder, and thus becomes asymptotically exact. | result 0.91 | 0.95 | 0.51 | asserted 1.00 |
| s2 | We use it to obtain the disorder-averaged inverse participation ratio and density of states for the entire spectrum. | result 0.65 | 0.96 | 0.09 | asserted 1.00 |
| s3 | A modified scheme is formulated for higher dimensions, which is found to be less efficient, but capable of improvement. | limitation 0.74 | 0.94 | 0.05 | asserted 0.97 |
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Original abstract
We describe a large disorder renormalization group (LDRG) method for the Anderson model of localization in one dimension which decimates eigenstates based on the size of their wavefunctions rather than their energy. We show that our LDRG scheme flows to infinite disorder, and thus becomes asymptotically exact. We use it to obtain the disorder-averaged inverse participation ratio and density of states for the entire spectrum. A modified scheme is formulated for higher dimensions, which is found to be less efficient, but capable of improvement.
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