2000
DOI: 10.1103/physrevb.61.3960
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Index distribution of random matrices with an application to disordered systems

Abstract: We compute the distribution of the number of negative eigenvalues (the index) for an ensemble of Gaussian random matrices, by means of the replica method. This calculation has important applications in the context of statistical mechanics of disordered systems, where the second derivative of the potential energy (the Hessian) is a random matrix whose negative eigenvalues measure the degree of instability of the energy surface. An analysis of the probability distribution of the Hessian index is therefore releva… Show more

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Cited by 40 publications
(89 citation statements)
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“…This result reveals that, in order to access the index fluctuations in this case, one needs to compute the next-order contribution to G N (μ,0) for large N . The same situation arises in the replica approach for the GOE ensemble [7]. We present in the next section explicit results for the mean and the variance of the index for specific random graph models in the regime |λ| > 0.…”
Section: The Characteristic Function Of the Index Distributionmentioning
confidence: 96%
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“…This result reveals that, in order to access the index fluctuations in this case, one needs to compute the next-order contribution to G N (μ,0) for large N . The same situation arises in the replica approach for the GOE ensemble [7]. We present in the next section explicit results for the mean and the variance of the index for specific random graph models in the regime |λ| > 0.…”
Section: The Characteristic Function Of the Index Distributionmentioning
confidence: 96%
“…(1) is recovered in the regime of small fluctuations, with a variance that grows as σ 2 ln N for large N . The prefactor σ 2 is given by σ 2 = 1/π 2 for both Gaussian [7,[10][11][12] and Wishart [13] random matrices, independently of λ, while σ 2 = 2/π 2 for Cauchy random matrices [14]. This logarithmic behavior of the variance apparently reflects the repulsion between neighboring levels [16], which imposes a constraint on the total number of eigenvalues that fit in a finite region of the spectrum.…”
Section: Introductionmentioning
confidence: 99%
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“…[30], in analogy with what happens in mean field models [31,32]: the vanishing as T approaches T c of the mean intensive number of negative directions (intensive index) of stationary points of the potential energy, n s (T ). Numerical simulations [33,34,35,36,37,38] found that n s (T ) decreases with decreasing T , and fits were performed to show that n s (T c ) = 0 [33,34,35].…”
Section: Introductionmentioning
confidence: 99%