# Anderson localization of two-dimensional massless pseudospin-1 Dirac particles in a correlated random one-dimensional scalar potential

## TL;DR

This paper investigates how correlated disorder affects Anderson localization of two-dimensional massless pseudospin-1 Dirac particles, deriving analytical and numerical results for localization length across various regimes and parameters.

## Contribution

It provides the first detailed analysis of disorder correlation effects on localization length for pseudospin-1 Dirac particles, including analytical formulas and scaling regimes.

## Key findings

- Localization length diverges as incident angle approaches zero.
- Localization length depends non-monotonically on disorder correlation length.
- Multiple scaling regimes are identified depending on disorder strength and energy.

## Abstract

We study theoretically Anderson localization of two-dimensional massless pseudospin-1 Dirac particles in a random one-dimensional scalar potential. We focus explicitly on the effect of disorder correlations, considering a short-range correlated dichotomous random potential at all strengths of disorder. We also consider a $\delta$-function correlated random potential at weak disorder. Using the invariant imbedding method, we calculate the localization length in a numerically precise way and analyze its dependencies on incident angle, disorder correlation length, disorder strength, energy, wavelength and average potential over a wide range of parameter values. In addition, we derive analytical formulas for the localization length, which are very accurate in the weak and strong disorder regimes. From the Dirac equation, we obtain an expression for the effective wave impedance, using which we explain several conditions for delocalization. We also deduce a condition under which the localization length vanishes. For all cases considered, the localization length depends non-monotonically on the disorder correlation length and diverges as $\theta^{-4}$ as the incident angle $\theta$ goes to zero. As the disorder strength is varied from zero to infinity, we find that there appear three different scaling regimes. As the energy or wavelength is varied from zero to infinity, there appear three or four different scaling regimes with different exponents, depending on the value of the average potential. The crossovers between different scaling regimes are explained in terms of the disorder correlation effect.