2010
DOI: 10.1063/1.3521288
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Edge effects in some perturbations of the Gaussian unitary ensemble

Abstract: A bordering of GUE matrices is considered, in which the bordered row consists of zero mean complex Gaussians N[0, σ/2] + iN[0, σ/2] off the diagonal, and the real Gaussian N[µ, σ/ √ 2] on the diagonal. We compute the explicit form of the eigenvalue probability function for such matrices, as well as that for matrices obtained by repeating the bordering. The correlations are in general determinantal, and in the single bordering case the explicit form of the correlation kernel is computed. In the large N limit it… Show more

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Cited by 7 publications
(6 citation statements)
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“…Notice from Fig. 2 that, in the case shown, pairs of eigenvalues split-off or separate [32,33] from the bulk continuous distribution at the small end of the spectrum. These separated eigenvalues include the smallest nonzero one.…”
mentioning
confidence: 80%
“…Notice from Fig. 2 that, in the case shown, pairs of eigenvalues split-off or separate [32,33] from the bulk continuous distribution at the small end of the spectrum. These separated eigenvalues include the smallest nonzero one.…”
mentioning
confidence: 80%
“…The minimization problem would then amount to studying the maximal eigenvalue of a rank-one random perturbation of GOE, which attracted a considerable interest recently, see e.g. [36,37,38,39] and whose large deviation functional is known explicitly [40]. In contrast, the problem with magnetic field is not a simple eigenvalue problem but is equivalent to a much less studied class of quadratic eigenvalue problems [2].…”
Section: Lagrange Multiplier Minimization Relation To Rmt In Perturbmentioning
confidence: 99%
“…The analogue of the BBP theorem in the perturbed GUE setting was established by Péché (2006), Desrosiers and Forrester (2006). Bassler, Forrester and Frankel (2010) treat an interesting generalization and mention some applications to physics. We consider a simple additive rank one perturbation of the GOE obtained by shifting the mean of every entry by the same constant µ/ √ n. By orthogonal invariance, this has the same effect on the spectrum as shifting the (1,1) entry by √ n µ.…”
Section: Introductionmentioning
confidence: 98%