{
 "creator" "Ellad Tadmor"
 "contributor-id" "360c0aed-48ce-45f6-ba13-337f12a531e8"
 "description" "Lennard-Jones (LJ) parameterization for Kr.  The LJ parameters epsilon and sigma are due to Bernardes (1958).  The cutoff radius is set so that phi(rcut)=tol*|phi(rmin)|, where  phi(r) is the LJ potential, 'rcut' is the cutoff radius, 'rmin' is the radius at which phi(r) is a minimum, and 'tol' is a small number.  Here 'tol' is taken to be 1.e-2 for a \"low-precision\".  See the parameter file (.params) for more details."
 "doi" "10.25950/f2c95efc"
 "domain" "openkim.org"
 "extended-id" "LJ_Shifted_Bernardes_1958LowCutoff_Kr__MO_995724792024_003"
 "kim-api-version" "2.0"
 "maintainer-id" "360c0aed-48ce-45f6-ba13-337f12a531e8"
 "model-driver" "LJ_Shifted__MD_498634107543_003"
 "potential-type" "lj"
 "publication-year" "2018"
 "source-citations" [
  {
   "author" "Newton Bernardes"
   "doi" "10.1103/PhysRev.112.1534"
   "issue" "5"
   "journal" "Physical Review"
   "pages" "1534--1539"
   "publisher" "American Physical Society"
   "recordkey" "MO_995724792024_003a"
   "recordtype" "article"
   "title" "Theory of Solid {N}e, {A}, {K}r, and {X}e at 0{K}"
   "volume" "112"
   "year" "1958"
  }
 ]
 "species" [
  "Kr"
 ]
 "title" "Lennard-Jones model (shifted) for Kr with parameters from Bernardes (1958) (low precision cutoff) v003"
}