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      Random Matrix Theory and Classical Statistical Mechanics. I. Vertex Models

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          Abstract

          A connection between integrability properties and general statistical properties of the spectra of symmetric transfer matrices of the asymmetric eight-vertex model is studied using random matrix theory (eigenvalue spacing distribution and spectral rigidity). For Yang-Baxter integrable cases, including free-fermion solutions, we have found a Poissonian behavior, whereas level repulsion close to the Wigner distribution is found for non-integrable models. For the asymmetric eight-vertex model, however, the level repulsion can also disappearand the Poisson distribution be recovered on (non Yang--Baxter integrable) algebraic varieties, the so-called disorder varieties. We also present an infinite set of algebraic varieties which are stable under the action of an infinite discrete symmetry group of the parameter space. These varieties are possible loci for free parafermions. Using our numerical criterion we have tested the generic calculability of the model on these algebraic varieties.

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          General Lattice Model of Phase Transitions

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            Two-dimensional quantum spin Hamiltonians: Spectral properties

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              Shape Analysis of the Level Spacing Distribution around the Metal Insulator Transition in the Three Dimensional Anderson Model

              We present a new method for the numerical treatment of second order phase transitions using the level spacing distribution function \(P(s)\). We show that the quantities introduced originally for the shape analysis of eigenvectors can be properly applied for the description of the eigenvalues as well. The position of the metal--insulator transition (MIT) of the three dimensional Anderson model and the critical exponent are evaluated. The shape analysis of \(P(s)\) obtained numerically shows that near the MIT \(P(s)\) is clearly different from both the Brody distribution and from Izrailev's formula, and the best description is of the form \(P(s)=c_1\,s\exp(-c_2\,s^{1+\beta})\), with \(\beta\approx 0.2\). This is in good agreement with recent analytical results.
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                Author and article information

                Journal
                17 September 1996
                Article
                10.1103/PhysRevE.55.5380
                cond-mat/9609157
                5ca8b0ab-cce8-4052-82d7-b238bfcc0f81
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                25 pages, 7 PostScript Figures
                cond-mat

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