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Localization-delocalization transition for a random block matrix model at the edge

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arxiv 2504.00512 v2 pith:IXKC32TD submitted 2025-04-01 math.PR

classification math.PR
keywords kappamathrmmatrixbulkedgeslocalization-delocalizationrandomspectral
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abstract

Consider a random block matrix model consisting of $D$ random systems arranged along a circle, where each system is modeled by an independent $N\times N$ complex Hermitian Wigner matrix. Neighboring systems interact via an arbitrary deterministic $N\times N$ matrix $A$. In this paper, we extend the localization-delocalization transition previously established in arxiv:2312.07297 for the bulk eigenvalue spectrum to the entire spectrum, including the spectral edges. Let $[E^-,E^+]$ denote the support of the limiting spectral density, and define $\kappa_E:=|E-E^+|\wedge |E-E^-|$ as the distance from a given energy $E \in [E^-, E^+]$ to the spectral edges. We show that for eigenvalues near $E$, the corresponding eigenvectors undergo a localization-delocalization transition when $\|A\|_{\mathrm{HS}}$ crosses the critical threshold $(\kappa_E + N^{-2/3})^{-1/2}$. In the delocalized phase, the extreme eigenvalues asymptotically follow the Tracy-Widom distribution, while in the localized phase, the edge eigenvalue statistics asymptotically match those of $D$ independent GUE ensembles, up to a deterministic shift. Our results recover those of arxiv:2312.07297 in the bulk regime, where $\kappa_E \asymp 1$, and further reveal the presence of mobility edges near $E^\pm$ when $1 \ll \|A\|_{\mathrm{HS}} \ll N^{1/3}$. Specifically, bulk eigenvectors corresponding to energies $E$ with $\kappa_E \gg \|A\|_{\mathrm{HS}}^{-2}$ are delocalized, while those with $\kappa_E \ll \|A\|_{\mathrm{HS}}^{-2}$ are localized.

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Cited by 2 Pith papers

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  1. Anomalous rate of eigenstate thermalisation at singularities of the density of states

    math-ph 2026-07 conditional novelty 8.0 of 10

    For correlated mean-field random matrices, eigenvector overlaps fluctuate at the Haar scale 1/N in the bulk and at regular edges, and at N^{-1/2} variance near cubic-root cusps, disproving the Feingold–Peres inverse-d...

  2. Delocalization of random band matrices at the edge

    math.PR 2025-05 conditional novelty 7.0 of 10

    For random band matrices in dimensions 1 and 2, eigenvectors with energies 2-|E| >> N^{-c} are delocalized, and all eigenvectors are delocalized when the band width exceeds N^{1-d/6}.

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