Prediction of vacancy defect diffusion paths in high entropy alloys via machine learning on molecular dynamics data

C C. Reimer (Security and Disruptive Technologies, National Research Council of Canada 1 , Ottawa,) P P. Saidi (Canadian Nuclear Laboratories 3 , Chalk River,) C C. Casert (Molecular Foundry, Lawrence Berkeley National Laboratory 4 , Berkeley,) C C. Beeler (Department of Mathematics and Statistics, University of Ottawa 5 , Ottawa,) C C. G. Tetsassi Feugmo (Department of Chemistry, University of Waterloo 7 , Waterloo,) S S. Whitelam (Molecular Foundry, Lawrence Berkeley National Laboratory 4 , Berkeley,) E E. Mansouri (Department of Mechanical and Materials Engineering, Queen’s University 8 , Kingston,) A A. Martinez (Department of Mechanical and Materials Engineering, Queen’s University 8 , Kingston,) L L. Beland (Department of Mechanical and Materials Engineering, Queen’s University 8 , Kingston,) I I. Tamblyn (Department of Physics, University of Ottawa 2 , Ottawa,)

Abstract

Identifying the diffusion path of point defects is a critical step in understanding their evolution and the mechanisms of related phenomena. Defect diffusion occurs at small length and time scales, with impacts on material properties that may continue to evolve over ns to μs, ms, and the continuum scale (s, min, etc., and cm, m, etc.). The time scale accessible to molecular dynamics (MD) simulations is limited by small step sizes, typically in the fs range. Thus, surrogate models of MD simulations through machine learning (ML)-based algorithms are of great interest, especially for complex systems such as high entropy alloys (HEAs). In this work, dynamics governing vacancy migration in HEA were approximated with graph convolutional network (GCN) models as ansatzes for kinetic Monte Carlo (KMC) rate catalogs. Network design considered that diffusion in crystalline solids generally depends on interactions between defects and their immediate neighbor atoms. Graphs represented the vacancy surroundings, MD-generated trajectories provided training and comparison datasets, and unsupervised GCN models approximated interatomic dynamics governing vacancy migration in HEAs as ansatzes for KMC. A proof-of-concept model trained on MD data for the Fe, Ni, Cr, Co, and Cu HEA environment was used with two different neighbor interactions to assess the feasibility of training a GCN to predict vacancy defect transition rates in the HEA environment. The resulting setup rapidly generated MD-formatted synthetic trajectories based on dynamics learned from the MD training set, with a time acceleration of roughly two orders of magnitude and a similar diffusion coefficient to MD observations. Additionally, Nudged Elastic Band (NEB) calculations were performed on randomly generated FeNiCrCoCu HEA structures to determine vacancy migration barriers across nearest-neighbor sites. Transition probabilities for each jump, categorized by atomic type, were extracted from these calculations. NEB-based and GCN-based approaches led to similar outcomes.

Article Details

Volume / Issue Vol. 138, Issue 7
Published August 21, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (10)

C

C. Reimer

Security and Disruptive Technologies, National Research Council of Canada 1 , Ottawa,

P

P. Saidi

Canadian Nuclear Laboratories 3 , Chalk River,

C

C. Casert

Molecular Foundry, Lawrence Berkeley National Laboratory 4 , Berkeley,

C

C. Beeler

Department of Mathematics and Statistics, University of Ottawa 5 , Ottawa,

C

C. G. Tetsassi Feugmo

Department of Chemistry, University of Waterloo 7 , Waterloo,

S

S. Whitelam

Molecular Foundry, Lawrence Berkeley National Laboratory 4 , Berkeley,

E

E. Mansouri

Department of Mechanical and Materials Engineering, Queen’s University 8 , Kingston,

A

A. Martinez

Department of Mechanical and Materials Engineering, Queen’s University 8 , Kingston,

L

L. Beland

Department of Mechanical and Materials Engineering, Queen’s University 8 , Kingston,

I

I. Tamblyn

Department of Physics, University of Ottawa 2 , Ottawa,