Delocalization and quantum diffusion of random band matrices in high dimensions I: Self-energy renormalization

TL;DR

This paper proves delocalization of eigenvectors and quantum diffusion behavior in high-dimensional random band matrices, using self-energy renormalization techniques for Gaussian models with potential extension to non-Gaussian cases.

Contribution

It introduces a self-energy renormalization method to analyze eigenvector delocalization and quantum diffusion in high-dimensional random band matrices.

Findings

Most bulk eigenvectors are delocalized with localization length comparable to system size.

The Fourier transform of the Green's function exhibits a quadratic dispersion relation.

Quantum diffusion criterion is validated for the model in high dimensions.

Abstract

We consider Hermitian random band matrices $H=(h_{xy})$ on the $d$-dimensional lattice $(\mathbb Z/L\mathbb Z)^d$. The entries $h_{xy}$ are independent (up to Hermitian conditions) centered complex Gaussian random variables with variances $s_{xy}=\mathbb E|h_{xy}|^2$. The variance matrix $S=(s_{xy})$ has a banded structure so that $s_{xy}$ is negligible if $|x-y|$ exceeds the band width $W$. In dimensions $d\ge 8$, we prove that, as long as $W\ge L^\epsilon$ for a small constant $\epsilon>0$, with high probability most bulk eigenvectors of $H$ are delocalized in the sense that their localization lengths are comparable to $L$. Denote by $G(z)=(H-z)^{-1}$ the Green's function of the band matrix. For ${\mathrm Im}\, z\gg W^2/L^2$, we also prove a widely used criterion in physics for quantum diffusion of this model, namely, the leading term in the Fourier transform of $\mathbb E|G_{xy}(z)|^2$ with respect to $x-y$ is of the form $({\mathrm Im}\, z + a(p))^{-1}$ for some $a(p)$ quadratic in $p$, where $p$ is the Fourier variable. Our method is based on an expansion of $T_{xy}=|m|^2 \sum_{\alpha}s_{x\alpha}|G_{\alpha y}|^2$ and it requires a self-energy renormalization up to error $W^{-K}$ for any large constant $K$ independent of $W$ and $L$. We expect that this method can be extended to non-Gaussian band matrices.