Existence, Uniqueness and Anisotropic-Decay-Caused Lifshitz Tails of the Integrated Density of Surface States for Random Surface Models

TL;DR

This paper investigates the existence, uniqueness, and Lifshitz tail behavior of the integrated density of surface states for random surface Schrödinger operators, highlighting new regimes caused by anisotropic decay of potentials.

Contribution

It establishes the existence and uniqueness of the IDSS for negative energies and introduces a new quantum-classical regime for Lifshitz tails in random surface models.

Findings

Proves existence and uniqueness of IDSS for negative energies.

Identifies Lifshitz tail behavior in three regimes, including a new quantum-classical regime.

Shows anisotropic decay influences the spectral properties of surface states.

Abstract

The current paper is devoted to the study of existence, uniqueness and Lifshitz tails of the integrated density of surface states (IDSS) for Schr\"{o}dinger operators with alloy type random surface potentials. We prove the existence and uniqueness of the IDSS for negative energies, which is defined as the thermodynamic limit of the normalized eigenvalue counting functions of localized operators on strips with sections being special cuboids. Under the additional assumption that the single-site impurity potential decays anisotropically, we also prove that the IDSS for negative energies exhibits Lifshitz tails near the bottom of the almost sure spectrum in the following three regimes: the quantum regime, the quantum-classical/classical-quantum regime and the classical regime. We point out that the quantum-classical/classical-quantum regime is new for random surface models.