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Journal ArticleDOI

The Dynamics of a Disordered Linear Chain

Freeman J. Dyson
- 15 Dec 1953 - 
- Vol. 92, Iss: 6, pp 1331-1338
TLDR
In this paper, the distribution function of the frequencies of normal modes of vibration of a disordered chain of one-dimensional harmonic oscillators is calculated analytically, in the limit when the chain becomes infinitely long.
Abstract
By a disordered chain we mean a chain of one-dimensional harmonic oscillators, each coupled to its nearest neighbors by harmonic forces, the inertia of each oscillator and the strength of each coupling being a random variable with a known statistical distribution law. A method is presented for calculating exactly the distribution-function of the frequencies of normal modes of vibration of such a chain, in the limit when the chain becomes infinitely long. For some special examples, in which the distribution law of the oscillator parameters is assumed to be of exponential form, the frequency spectra are calculated analytically. The theory applies equally well to a chain of masses connected by elastic springs and making mechanical vibrations, or to an electrical transmission line composed of alternating inductances and capacitances with random characteristics.

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Energy transfer in random systems

TL;DR: In this article, the time development of the emission profile after pulse excitation was calculated for all one and two-phonon processes, including exchange and multipolar site couplings and radiative transfer.
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Physical implications of multi-neighbor activations in the master equation☆

TL;DR: In this article, the authors show how multi-neighbor activations can arise from applications of the master equation to physical models, and how such randomized activation can be solved by homotopy mapping.
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Disordered graphene ribbons as topological multicritical systems

- 14 Nov 2022 - 
TL;DR: In this article , the authors investigated the influence of symmetry-preserving disorder on a multicritical point and showed that the system harbors delocalized states with the localization length diverging at zero energy in a manner consistent with the critical point.
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Nonequilibrium response of a disordered Ising chain

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Inhomogeneous Fixed Point Ensembles Revisited

TL;DR: In this article, the scaling law of the density of states in the Wigner-Dyson and Bogolubov-de Gennes classes of disordered systems was shown to have a finite non-zero value at the mobility edge.
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