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PreprintCC BY 4.0arXiv

Crystal forming ability of amorphous refractory metals under nanoindentation: a molecular dynamics study

Abstract

Amorphous refractory metal coatings combine high hardness with chemical inertness, yet their metastability makes them prone to mechanically induced crystallisation (devitrification) under contact loading, and how readily such a glass re-orders to its parent body centred cubic (bcc) crystal is unknown across the refractory series. We prepared amorphous V, Nb, Mo, Ta and W by melt quenching to 300 K, benchmarked each interatomic potential against ab initio liquid radial distribution functions and self-diffusion coefficients, and probed them by large scale molecular dynamics nanoindentation. Indentation drives a localised amorphous to bcc transformation by bulk nucleation, growth and coalescence. A crystal forming ability (CFA), the maximum slope of the sigmoidal bcc fraction versus depth curve, spans about a factor of four and decreases as V > Mo > Nb > Ta > W; it falls with indenter velocity as CFA scales as v^(-m), with a mean exponent of 1.08, so CFA.v is nearly constant and the transformation rate is almost velocity independent. Transforming atoms carry excess non affine displacement and local shear strain, not hydrostatic pressure, marking a shear associated displacive pathway; the bulk driving force is largest for the most resistant element, W, so resistance tracks cohesive bond strength rather than the thermodynamic driving force. Early bcc like order correlates with the sharpness and depth of the transition, whereas the mechanical work to half transformation correlates with the peak density of persistent bcc clusters. A cluster population balance links nucleation, growth and coalescence to a terminal microstructure whose completeness does not follow the CFA order.

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BibTeX
@misc{dwivedi2026crystal,
  title = {{Crystal forming ability of amorphous refractory metals under nanoindentation: a molecular dynamics study}},
  author = {Prashant Dwivedi and Alberto Fraile and Tomas Polcar},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2607.26881},
  eprint = {2607.26881},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2607.26881},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Crystal forming ability of amorphous refractory metals under nanoindentation: a molecular dynamics study
AU  - Prashant Dwivedi
AU  - Alberto Fraile
AU  - Tomas Polcar
PY  - 2026
DA  - 2026/10/27
PB  - arXiv
DO  - 10.48550/arxiv.2607.26881
UR  - https://arxiv.org/abs/2607.26881
AB  - Amorphous refractory metal coatings combine high hardness with chemical inertness, yet their metastability makes them prone to mechanically induced crystallisation (devitrification) under contact loading, and how readily such a glass re-orders to its parent body centred cubic (bcc) crystal is unknown across the refractory series. We prepared amorphous V, Nb, Mo, Ta and W by melt quenching to 300 K, benchmarked each interatomic potential against ab initio liquid radial distribution functions and self-diffusion coefficients, and probed them by large scale molecular dynamics nanoindentation. Indentation drives a localised amorphous to bcc transformation by bulk nucleation, growth and coalescence. A crystal forming ability (CFA), the maximum slope of the sigmoidal bcc fraction versus depth curve, spans about a factor of four and decreases as V > Mo > Nb > Ta > W; it falls with indenter velocity as CFA scales as v^(-m), with a mean exponent of 1.08, so CFA.v is nearly constant and the transformation rate is almost velocity independent. Transforming atoms carry excess non affine displacement and local shear strain, not hydrostatic pressure, marking a shear associated displacive pathway; the bulk driving force is largest for the most resistant element, W, so resistance tracks cohesive bond strength rather than the thermodynamic driving force. Early bcc like order correlates with the sharpness and depth of the transition, whereas the mechanical work to half transformation correlates with the peak density of persistent bcc clusters. A cluster population balance links nucleation, growth and coalescence to a terminal microstructure whose completeness does not follow the CFA order.
ER  -