# Zero mode protection at particle-hole symmetry: a geometric interpretation

## TL;DR

This paper investigates zero modes in particle-hole symmetric systems under strong disorder, revealing a geometric interpretation that links scattering strength to lattice-covering self-avoiding strings and generalizes Dyson's 1953 findings.

## Contribution

It introduces a geometric framework using lattice-covering self-avoiding strings to understand zero mode protection at particle-hole symmetry under strong disorder.

## Key findings

- Strong scattering leads to flat density distributions.
- Weak scattering results in decaying density distributions.
- The approach generalizes Dyson's 1953 delocalized state at band center.

## Abstract

The properties of zero modes in particle-hole symmetric systems are analyzed in the presence of strong random scattering by a disordered environment. The study is based on the calculation of the time-averaged density distribution on a lattice. In particular, a flat distribution is found for strong random scattering. This result is compared with a decaying distribution for weak random scattering by an analysis of the scattering paths. In the calculation we consider the invariant measure of the average two-particle Green's function, which is related to lattice-covering self-avoiding (LCSA) strings. In particular, strong scattering is associated with LCSA loops, whereas weaker scattering is associated with open LCSA strings. Our results are a generalization of the delocalized state observed at the band center of a one-dimensional tight-binding model with random hopping by Dyson in 1953.