ovi.dat

 46
** Atomic data from version 7 of the CHIANTI database **
%energy levels: Fuhr, J.R., Kelleher, D.E., Martin, W.C., Musgrove, A., Sugar, J., Wiese, W.L.,
        Dalton, G.R., Dragoset, R.A., Mohr, P.J., Olsen, K., Reader, J., Saloman, E.B., Sansonetti, C.J.,
        Wiersma, G., "NIST Atomic Spectra Database" Ver. 2.0, March 1999, NIST Physical Reference Data.
%theoretical energy levels (n=2,3,4): Badnell, N.R., Pindzola, M.S., 2000, J.Phys.B, 33, 1013
%theoretical energy levels (n=5): Zhang,H.L., Sampson,D.H., Fontes,C.J., 1990, ADNDT, 44, 31.
%Innershell theoretical energy levels: Sampson, D.H., Goett,S.J., 1983, ADNDT, 29, 535
%produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration
%
% E.Landi - Jun 2001
%filename: o_6.wgfa
%energy levels: Fuhr, J.R., et al., "NIST Atomic Spectra Database" Ver. 2.0, 
       March 1999, NIST Physical Reference Data.
%theoretical energy levels (n=2,3,4): Badnell, N.R., Pindzola, M.S., 2000, J.Phys.B, 33, 1013
%theoretical energy levels (n=5): Zhang, H.L., Sampson, D.H., Fontes, C.J., 1990, ADNDT, 44, 31.
%Innershell theoretical energy levels: Sampson, D.H., Goett, S.J., 1983, ADNDT, 29, 535
%oscillator strengths: H.L.Zhang, D.H.Sampson, C.J.Fontes, 1990, ADNDT, 44, 31
%oscillator strengths: Martin, I., Karwowski, J., Diercksen, G.H.F., Barrientos, C., 1993, A&AS, 100, 595.
%Innershell radiative data: Goett, S.J., Sampson, D.H., 1983, ADNDT, 29, 535
%Comment: Other radiative data were calculated using SUPERSTRUCTURE with a 23 configuration model
%A values (autoionizing): Vainshtein, L.A., Safronova, U.I., 1978, ADNDT, 21, 49 and 1980, ADNDT, 25, 311 
                          - updated by U.I. Safronova, 1999
%comment:  unobserved lines
    1   26       -22.5472      3.689e-06      2.419e+07        1S2 2S 2S0.5 -  1s.(2S).2s.2p 4P0.5
    1   28       -22.5401      1.325e-07      2.899e+05        1S2 2S 2S0.5 -  1s.(2S).2s.2p 4P2.5
    2   25       -23.1869      6.745e-03      4.182e+10        1S2 2P 2P0.5 -         1s.2s2 2S0.5
    2   31       -22.4131      6.981e-06      4.632e+07        1S2 2P 2P0.5 -         1s.2p2 4P0.5
    3   25       -23.1898      1.323e-02      8.200e+10        1S2 2P 2P1.5 -         1s.2s2 2S0.5
    3   31       -22.4158      7.072e-07      4.692e+06        1S2 2P 2P1.5 -         1s.2p2 4P0.5
    3   33       -22.4123      4.447e-05      9.836e+07        1S2 2P 2P1.5 -         1s.2p2 4P2.5
%produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration
%
% E. Landi and K.P.Dere - Jun 2001

%filename: o_6.splups
%effective collision strengths (transitions 1 - 2 to 1 - 15): Badnell, N.R., Pindzola, M.S., 2000, J.Phys.B, 33, 1013
%oscillator strengths (levels 1 - 24): H.L. Zhang, D.H. Sampson, C.J. Fontes, 1990, ADNDT, 44, 31
%oscillator strengths innershell (levels 25 - 40): Goett, S.J., Sampson, D.H., 1983, ADNDT, 29, 535
%collision strengths (levels 16 - 24, transitions 2 - 3 to 2 - 24):  H.L. Zhang, D.H. Sampson, C.J. Fontes, 1990, ADNDT, 44, 31
%collision strengths innershell (levels 25 - 40): Goett, S.J., Sampson, D.H., 1983, ADNDT, 29, 535
%comment: the original data from Badnell & Pindzola are provided in LS coupling. These have been transformed into 
    intermediate coupling effective collision strengths according to the statistical weights
%comment: effective collision strengths were provided in the temperature range 4.55 < Log T < 6.85
%produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration
%
% Enrico Landi - Jun 2001
15 23
  1  1s2.2s 2S1/2
  2  1s2.2p 2P1/2
  3  1s2.2p 2P3/2
  4  1s2.3s 2S1/2
  5  1s2.3p 2P1/2
  6  1s2.3p 2P3/2
  7  1s2.3d 2D3/2
  8  1s2.3d 2D5/2
  9  1s2.4s 2S1/2
 10  1s2.4p 2P1/2
 11  1s2.4p 2P3/2
 12  1s2.4d 2D3/2
 13  1s2.4d 2D5/2
 14  1s2.4f 2F5/2
 15  1s2.4f 2F7/2
     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
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  0  0   5.19e-03
  0  0   5.67e-03
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  2 10   4.74e-02
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