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Machine Learning Potentials for Hydrogen Absorption in TiCr$_2$ Laves Phases

Materials Science 2025-11-25 v2

Abstract

The energetics of hydrogen absorption in C15 cubic and C14 hexagonal TiCr2_2Hx_x Laves phases is investigated for 0<x60 < x \le 6 with density functional theory (DFT) and machine learning interatomic potentials (MLIPs). The MLIPs are trained with configurations generated through a series of active-learning schemes. Basin-hopping Monte Carlo (BHMC) simulations based on the MLIPs predict minimum-energy hydrogen configurations, along with enthalpies of formation and hydrogen orderings. The obtained phase transformations at 0 K agree well with the experiments at low temperatures. The hydrogen solubility limits in the low-concentration α\alpha phases at 0 K are predicted to be x=1.0x = 1.0 and x=1.5x = 1.5 for the C15 and the C14 phases, respectively. At these concentrations, C15 TiCr2_2H shows the CcCc monoclinic symmetry, while C14 TiCr2_2H1.5_{1.5} shows the Ama2Ama2 orthorhombic symmetry, both of which have not been reported for this system. The first and the second hydride phases, i.e., β\beta and β\beta', at 0 K are found around x=3x = 3 and x=4x = 4, respectively, for both the C15 and the C14 phases. In the second-hydride β\beta' phases, C15 TiCr2_2H4_4 shows the I41/aI4_1/a tetragonal symmetry, while C14 TiCr2_2H4_4 shows the R3ˉcR\bar3c rhombohedral symmetry. Hydrogen repulsion are found to extend to edge-sharing interstices, affecting the hydrogen ordering. Furthermore, the 6h26h_2 A2_2B2_2 interstices are found to be energetically substantially more preferable for C14 TiCr2_2Hx_x than the other A2_2B2_2 interstices at low hydrogen concentrations, influencing the hydrogen-occupation trend.

Keywords

Cite

@article{arxiv.2503.22824,
  title  = {Machine Learning Potentials for Hydrogen Absorption in TiCr$_2$ Laves Phases},
  author = {Pranav Kumar and Fritz Körmann and Blazej Grabowski and Yuji Ikeda},
  journal= {arXiv preprint arXiv:2503.22824},
  year   = {2025}
}
R2 v1 2026-06-28T22:38:36.682Z