      1      2   1.033e-02   0.000e+00          -1    9    2   5.764e+00
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   3.466e-01   9.285e-01   1.049e+00   1.047e+00   1.065e+00   1.125e+00   1.241e+00   1.452e+00   1.602e+00
      1      3   2.668e-02   0.000e+00          -1    9    2   2.232e+00
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   8.104e-01   1.212e+00   1.267e+00   1.243e+00   1.201e+00   1.163e+00   1.157e+00   1.217e+00   1.216e+00
      1      4   1.729e-01   0.000e+00          -1    9    2   4.077e-01
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   5.081e-01   5.279e-01   5.719e-01   5.568e-01   5.151e-01   4.777e-01   4.625e-01   4.575e-01   3.817e-01
      1      5   3.951e-01   0.000e+00          -1    9    2   1.507e-01
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   1.491e-01   1.503e-01   1.246e-01   1.017e-01   8.851e-02   8.183e-02   7.838e-02   7.247e-02   5.188e-02
      2      3   1.635e-02   0.000e+00          -1    9    2   3.642e+00
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   2.251e+00   3.886e+00   4.161e+00   4.103e+00   4.033e+00   4.023e+00   4.152e+00   4.553e+00   4.733e+00
      2      4   1.626e-01   0.000e+00          -1    9    2   4.336e-01
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   1.526e+00   1.584e+00   1.716e+00   1.670e+00   1.545e+00   1.433e+00   1.388e+00   1.373e+00   1.146e+00
      2      5   3.848e-01   0.000e+00          -1    9    2   1.547e-01
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   4.478e-01   4.508e-01   3.737e-01   3.050e-01   2.655e-01   2.455e-01   2.351e-01   2.174e-01   1.558e-01
      3      4   1.463e-01   0.000e+00          -1    9    2   4.821e-01
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   2.541e+00   2.640e+00   2.859e+00   2.784e+00   2.576e+00   2.389e+00   2.313e+00   2.287e+00   1.906e+00
      3      5   3.684e-01   0.000e+00          -1    9    2   1.616e-01
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   7.461e-01   7.513e-01   6.228e-01   5.085e-01   4.426e-01   4.091e-01   3.919e-01   3.624e-01   2.596e-01
      4      5   2.222e-01   0.000e+00          -1    9    2   2.927e-01
   0.000e+00   1.250e-01   2.500e-01   3.750e-01   5.000e-01   6.250e-01   7.500e-01   8.750e-01   1.000e+00
   3.349e+00   2.147e+00   1.704e+00   1.635e+00   1.673e+00   1.693e+00   1.674e+00   1.670e+00   1.508e+00
-1
%filename: k_6.splups
%Theoretical energies: No theoretical energies available - observed energies from .elvlc file used instead.
%Upsilons: Galavis, M.E., Mendoza, C., Zeippen, C.J. 1995, A&ASS 111, 347
%comment: The fits reproduce the original data to within 0.55% over the temperature range 3.0 <= logT <= 5.0.
% produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration
%
%   Peter Young   -   20-Jun-2006
-1
