Theoretical studies of defect states in GaTe
Related Experiment Video
Updated: May 30, 2026

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
Published on: November 1, 2013
Zs Rak1, S D Mahanti, Krishna C Mandal
1Department of Physics and Astronomy, Michigan State University, East Lansing, MI 48824, USA.
Abstract:
Using first principle electronic structure calculations within density functional theory and the supercell model, we have investigated the nature and formation energies of defect states associated with Ga and Te vacancies and Ge and Sn substitutional impurities in GaTe. We have also calculated the band structure of pure GaTe for comparison with systems with defects and also to find out the importance of spin-orbit interaction (SOI) on its band structure. We find that the top valence band at the Γ-point shifts up in energy by ∼0.1 eV due to the mixing of Te p(x)-p(y) and p(z) bands, this splitting being considerably smaller than in atoms where it is ∼0.8 eV. From an analysis of charge densities and band structures associated with the defect states, we find that most of them are strongly localized and lie deep in the band gap region. The calculated binding energy of the deep defect state and the ε(-1/-2) transition level associated with the Ga vacancy appears to be in good agreement with experiment. Formation energy calculations suggest that V(Ga) is the preferred intrinsic defect in GaTe.
More Related Videos
Related Concept Videos
Imperfections in Crystal Structure: Stoichiometric Point Defects
MOSFET: Depletion Mode
The primary characteristic of depletion-mode MOSFETs is their ability to conduct current between the drain and source terminals without gate bias. This inherent conductivity arises...
Characteristics of MOSFET
Various vital parameters influence their functionality, which is crucial for theory and electronics applications. First, channel dimensions, precisely length, and width, are pivotal. The size of these channels affects the transistor's ability to carry current and switching speeds; shorter channels typically enable quicker...
Imperfections in Crystal Structure: Point, Line and Plane Defects
Imperfections in Crystal Structure: Non-Stoichiometric Defects
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...

