Simulating and Understanding Point Defects using Density Functional Theory and Graph Neural Networks

ORAL  · Invited

Abstract

DFT is routinely used to simulate point defects in solids and calculate their formation energies as a function of chemical growth conditions, Fermi level, and defect charge. Defect energy plots help ascertain the donor- and acceptor-type nature of defects, their relative stabilities, their shallow or deep levels, the equilibrium Fermi level, and temperature-dependent defect concentrations [1,2]. The need for large supercells, charge states, and advanced functionals makes defect calculations very expensive, prohibiting their application to massive semiconductor-defect chemical spaces. Combining DFT with machine learning (ML) helps address the computational expense by enabling on-demand predictions of defect energetics and defect levels directly from descriptor-based or structure-based representations.



In this talk, I will discuss my group’s work in developing crystal graph neural network (GNN) models for accelerating point defect simulations [3]. We developed a computational workflow that uses both semi-local and hybrid functionals to generate datasets of native point defects, impurities, dopants, and defect complexes in chalcogenide and halide semiconductors, also accounting for energy-lowering symmetry-broken configurations. GNN-based interatomic potentials trained on this data subsequently enable prediction and optimization of thousands of new point defects and complexes, and identification of the lowest energy defects. Final HSE06 computations with spin-orbit coupling are performed on the most important defects to generate a final computational defect dataset. This scheme was applied for rational discovery and screening of low energy defect structures in dozens of semiconductors belonging to: (a) Cd/Zn-Te/Se/S compositions, relevant for CdTe solar cells, (b) a variety of inorganic halide (e.g., CsPbI3) and chalcogenide (e.g., BaZrS3) perovskites, and (c) zincblende-derived ternary and quaternary chalcogenides (e.g., Cu(In,Ga)S2 and Ag2ZnSnSe4).

*DOE EERE: SETO-SIPS #DE-EE0011158DOE EERE: SETO Award Number 37989US N.R.C. Faculty Development Grant, 31310024M0035

Publication: [1] M.H. Rahman et al., J. Phys. Mater. 8 022001 (2025).
[2] A. Mannodi-Kanakkithodi et al., Patterns. 3, 3, 100450 (2022).
[3] M.H. Rahman et al., APL Machine Learning. 2, 016122 (2024).

Presenters

  • Arun Kumar Mannodi Kanakkithodi

    • Purdue University School of Materials Engineering

Authors

  • Arun Kumar Mannodi Kanakkithodi

    • Purdue University School of Materials Engineering
  • Md Habibur Rahman

    • Purdue University School of Materials Engineering
  • Maitreyo Biswas

    • Purdue University School of Materials Engineering
  • Rushik Desai

    • Purdue University School of Materials Engineering