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** Atomic data from version 7 of the CHIANTI database **
%Observed energy levels (n=2): Edlen, B. 1983, Physica Scripta, 28, 51
%Observed energy levels (n=3): Artru, M.-C., & W.-U. L. Brillet, 1977, Physica Scripta, 16, 93
%Theoretical energy levels: Witthoeft, M.C., Whiteford, A.D., & Badnell, N.R. 2007, J.Phys.B, 40, 2969
% produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration
%
% E. Landi - May 2007
%filename: si_6.wgfa
%Observed energy levels (n=2): Edlen, B. 1983, Physica Scripta, 28, 51
%Observed energy levels (n=3): Artru, M.-C., & W.-U. L. Brillet, 1977, Physica Scripta, 16, 93
%Theoretical energy levels: Witthoeft, M.C., Whiteford, A.D., & Badnell, N.R. 2007, J.Phys.B, 40, 2969
%Radiative data: Witthoeft, M.C., Whiteford, A.D., & Badnell, N.R. 2007, J.Phys.B, 40, 2969
% produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration
%
% E. Landi - May 2007
%filename: si_6.splups
%Oscillator strengths: Witthoeft, M.C., Whiteford, A.D., & Badnell, N.R. 2007, J.Phys.B, 40, 2969
%Effective collision strengths: Witthoeft, M.C., Whiteford, A.D., & Badnell, N.R. 2007, J.Phys.B, 40, 2969
%comment: effective collision strengths are published for temperatures in the range 3.9 < Log T < 7.7
%comment: effective collision strengths are USED for temperatures in the range 4.5 < Log T < 7.1
%comment: data at very high or very low temperatures were sometimes discarded to improve the fit. At these
temperatures the Si VI abundance is negligible under equilibrium.
% produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration
%
% E. Landi - Mar 2007
2 23
1 2s2.2p5 2P3/2
2 2s2.2p5 2P1/2
100.0
158.5
251.2
398.1
631.0
1000.0
1584.9
2511.9
3981.1
6309.6
10000.0
15848.9
25118.9
39810.7
63095.8
100000.0
158489.2
251188.7
398107.1
630957.6
1000000.0
1584892.5
2511887.0
0
1 2 1.79e-01
0 0 1.79e-01
0 0 1.80e-01
0 0 1.81e-01
0 0 1.82e-01
0 0 1.84e-01
0 0 1.88e-01
0 0 1.93e-01
0 0 2.02e-01
0 0 2.15e-01
0 0 2.36e-01
0 0 2.68e-01
0 0 3.14e-01
0 0 3.73e-01
0 0 4.33e-01
0 0 4.62e-01
0 0 4.59e-01
0 0 4.45e-01
0 0 4.25e-01
0 0 4.01e-01
0 0 3.61e-01
0 0 3.16e-01
0 0 2.66e-01
0 0 0
1 2 2.960e+00
1 4 0.0
2 2 5094.2
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