Defect theory under steady illuminations and applications

Abstract

Illumination has been long known to affect semiconductor defect properties during either growth or operating processes. Current theories of studying the illumination effects on defects usually have the assumption of unaffected formation energies of neutral defects as well as defect transition energy levels, and use the quasi-Fermi levels to describe behaviors of excess carriers with conclusions at variance. In this work, we first propose a method to simulate steady illumination conditions, based on which we demonstrate that formation energies of neutral defects and defect transition energy levels are insensitive to illumination. Then, we show that optical and thermal excitation of electrons can be seen equivalent with each other to reach a steady electron distribution in a homogeneous semiconductor. Consequently, the electron distribution can be characterized using just one effective temperature T^{′} and one universal Fermi level E_{F}^{^{′}} for a homogeneous semiconductor under continuous and steady illuminations, which can be seen as a combination of quasiequilibrium electron system with T^{′} and a lattice system with T. Using these concepts, we uncover the universal mechanisms of illumination effects on charged defects by treating the band-edge states explicitly on the same footing as the defect states. We find that the formation energies of band-edge “defect” states shift with increased T^{′} of electrons, thus affecting the E_{F}^{^{′}}, changing defect ionic probabilities, and affecting concentrations of charged defects. We apply our theory to study the illumination effects on the doping behaviors in GaN:Mg and CdTe:Sb, obtaining results in accordance with experimental observations. More interesting experimental defect-related phenomena under steady illuminations are expected to be understood from our theory.