@Comment
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This Model originally published in \cite{OpenKIM-MO:532072268679:000a} is archived in \cite{OpenKIM-MO:532072268679:000, OpenKIM-MD:120291908751:005, tadmor:elliott:2011, elliott:tadmor:2011}.
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\bibliography{kimcite-MO_532072268679_000.bib}
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}

@Misc{OpenKIM-MO:532072268679:000,
  author       = {German D. Samolyuk and Laurent K. Béland and G. Malcolm Stocks and Roger E. Stoller},
  title        = {{EAM} potential ({LAMMPS} cubic hermite tabulation) for the {N}i-{P}d system developed by {S}amolyuk et al. (2016) v000},
  doi          = {10.25950/bbd6e8af},
  howpublished = {OpenKIM, \url{https://doi.org/10.25950/bbd6e8af}},
  keywords     = {OpenKIM, Model, MO_532072268679_000},
  publisher    = {OpenKIM},
  year         = 2022,
}

@Misc{OpenKIM-MD:120291908751:005,
  author       = {Stephen M. Foiles and Michael I. Baskes and Murray S. Daw and Steven J. Plimpton},
  title        = {{EAM} {M}odel {D}river for tabulated potentials with cubic {H}ermite spline interpolation as used in {LAMMPS} v005},
  doi          = {10.25950/68defa36},
  howpublished = {OpenKIM, \url{https://doi.org/10.25950/68defa36}},
  keywords     = {OpenKIM, Model Driver, MD_120291908751_005},
  publisher    = {OpenKIM},
  year         = 2018,
}

@Article{tadmor:elliott:2011,
  author    = {E. B. Tadmor and R. S. Elliott and J. P. Sethna and R. E. Miller and C. A. Becker},
  title     = {The potential of atomistic simulations and the {K}nowledgebase of {I}nteratomic {M}odels},
  journal   = {{JOM}},
  year      = {2011},
  volume    = {63},
  number    = {7},
  pages     = {17},
  doi       = {10.1007/s11837-011-0102-6},
}

@Misc{elliott:tadmor:2011,
  author       = {Ryan S. Elliott and Ellad B. Tadmor},
  title        = {{K}nowledgebase of {I}nteratomic {M}odels ({KIM}) Application Programming Interface ({API})},
  howpublished = {\url{https://openkim.org/kim-api}},
  publisher    = {OpenKIM},
  year         = 2011,
  doi          = {10.25950/ff8f563a},
}

@Article{OpenKIM-MO:532072268679:000a,
  abstract = {Energy transfer between lattice atoms and electrons is an important channel of energy dissipation during displacement cascade evolution in irradiated materials. On the assumption of small atomic displacements, the intensity of this transfer is controlled by the strength of electron–phonon (el–ph) coupling. The el–ph coupling in concentrated Ni-based alloys was calculated using electronic structure results obtained within the coherent potential approximation. It was found that Ni0.5Fe0.5, Ni0.5Co0.5 and Ni0.5Pd0.5 are ordered ferromagnetically, whereas Ni0.5Cr0.5 is nonmagnetic. Since the magnetism in these alloys has a Stoner-type origin, the magnetic ordering is accompanied by a decrease of electronic density of states at the Fermi level, which in turn reduces the el–ph coupling. Thus, the el–ph coupling values for all alloys are approximately 50% smaller in the magnetic state than for the same alloy in a nonmagnetic state. As the temperature increases, the calculated coupling initially increases. After passing the Curie temperature, the coupling decreases. The rate of decrease is controlled by the shape of the density of states above the Fermi level. Introducing a two-temperature model based on these parameters in 10 keV molecular dynamics cascade simulation increases defect production by 10–20% in the alloys under consideration.},
  author = {Samolyuk, G D and B{\'{e}}land, L K and Stocks, G M and Stoller, R E},
  doi = {10.1088/0953-8984/28/17/175501},
  journal = {Journal of Physics: Condensed Matter},
  month = {apr},
  number = {17},
  pages = {175501},
  publisher = {{IOP} Publishing},
  title = {Electron{\textendash}phonon coupling in {N}i-based binary alloys with application to displacement cascade modeling},
  url = {https://doi.org/10.1088/0953-8984/28/17/175501},
  volume = {28},
  year = {2016},
}