Surface states, Friedel oscillations, and spin accumulation in p-doped semiconductors

TL;DR

This paper investigates how localized surface states in p-doped semiconductors contribute to spin accumulation and Friedel oscillations near boundaries under charge current, revealing detailed quantum and many-body effects.

Contribution

It provides an exact quantum mechanical solution for boundary states in the Luttinger model and links localized states to surface spin accumulation and oscillations.

Findings

Localized surface states contribute to spin accumulation.

Friedel oscillations with three distinct periods are observed.

Total spin accumulation follows a specific mass ratio formula.

Abstract

We consider a hole-doped semiconductor with a sharp boundary and study the boundary spin accumulation in response to a charge current. First, we solve exactly a single-particle quantum mechanics problem described by the isotropic Luttinger model in half-space and construct an orthonormal basis for the corresponding Hamiltonian. It is shown that the complete basis includes two types of eigenstates. The first class of states contains conventional incident and reflected waves, while the other class includes localized surface states. Second, we consider a many-body system in the presence of a charge current flowing parallel to the boundary. It is shown that the localized states contribute to spin accumulation near the surface. We also show that the spin density exhibits current-induced Friedel oscillations with three different periods determined by the Fermi momenta of the light and heavy holes. We find an exact asymptotic expression for the Friedel oscillations far from the boundary. We also calculate numerically the spin density profile and compute the total spin accumulation, which is defined as the integral of the spin density in the direction perpendicular to the boundary. The total spin accumulation is shown to fit very well the simple formula S ~(1 - m_L/m_H)^2, where m_L and m_H are the light- and heavy-hole masses. The effects of disorder are discussed. We estimate the spin relaxation time in the Luttinger model and argue that spin physics cannot be described within the diffusion approximation.