chv6_ic#fe13.dat
Resolved Specific Ion Data Collections
- Ion
- Fe13+
- Temperature Range
- 8.444 eV → 8444 eV
ADF04
- Filename
- chv6_ic#fe13.dat
- Full Path
- adf04/copch#26/chv6_ic#fe13.dat
Download data
- Spontaneous Emission: Fe+13(i) → Fe+13(j) + hv
- Electron Impact Excitation: Fe+13(i) + e → Fe+13(j) + e
| 3s2.3p 2p1/2 2P0.5 | 0.0 cm-1 |
| 3s2.3p 2p3/2 2P1.5 | 18490.7 cm-1 |
| 3s.3p2 4p1/2 4P0.5 | 222469.0 cm-1 |
| 3s.3p2 4p3/2 4P1.5 | 229974.0 cm-1 |
| 3s.3p2 4p5/2 4P2.5 | 239478.0 cm-1 |
| 3s.3p2 2d3/2 2D1.5 | 299672.0 cm-1 |
| 3s.3p2 2d5/2 2D2.5 | 301765.0 cm-1 |
| 3s.3p2 2s1/2 2S0.5 | 368998.0 cm-1 |
| 3s.3p2 2p1/2 2P0.5 | 393266.0 cm-1 |
| 3s.3p2 2p3/2 2P1.5 | 401322.0 cm-1 |
| 3s2.3d 2d3/2 2D1.5 | 481390.0 cm-1 |
| 3s2.3d 2d5/2 2D2.5 | 483818.0 cm-1 |
| 3p3 2d3/2 2D1.5 | 576628.0 cm-1 |
| 3p3 2d5/2 2D2.5 | 580267.0 cm-1 |
| 3p3 4s3/2 4S1.5 | 589990.0 cm-1 |
| 3s.3p(3p).3d 4f3/2 4F1.5 | 644908.0 cm-1 |
| 3p3 2p1/2 2P0.5 | 645651.0 cm-1 |
| 3p3 2p3/2 2P1.5 | 648556.0 cm-1 |
| 3s.3p(3p).3d 4f5/2 4F2.5 | 648910.0 cm-1 |
| 3s.3p(3p).3d 4f7/2 4F3.5 | 654680.0 cm-1 |
| 3s.3p(3p).3d 4f9/2 4F4.5 | 662678.0 cm-1 |
| 3s.3p(3p).3d 4p5/2 4P2.5 | 695226.0 cm-1 |
| 3s.3p(3p).3d 4d3/2 4D1.5 | 697508.0 cm-1 |
| 3s.3p(3p).3d 4d1/2 4D0.5 | 699097.0 cm-1 |
| 3s.3p(3p).3d 4p1/2 4P0.5 | 707362.0 cm-1 |
| 3s.3p(3p).3d 4p3/2 4P1.5 | 708179.0 cm-1 |
| 3s.3p(3p).3d 4d7/2 4D3.5 | 708483.0 cm-1 |
| 3s.3p(3p).3d 4d5/2 4D2.5 | 708637.0 cm-1 |
| 3s.3p(3p).3d 2d3/2 2D1.5 | 723440.0 cm-1 |
| 3s.3p(3p).3d 2d5/2 2D2.5 | 724028.0 cm-1 |
| 3s.3p(3p).3d 2f5/2 2F2.5 | 755311.0 cm-1 |
| 3s.3p(3p).3d 2f7/2 2F3.5 | 769622.0 cm-1 |
| 3s.3p(3p).3d 2p3/2 2P1.5 | 819697.0 cm-1 |
| 3s.3p(3p).3d 2p1/2 2P0.5 | 827768.0 cm-1 |
| 3s.3p(1p).3d 2f7/2 2F3.5 | 831095.0 cm-1 |
| 3s.3p(1p).3d 2f5/2 2F2.5 | 833814.0 cm-1 |
| 3s.3p(1p).3d 2p1/2 2P0.5 | 854964.0 cm-1 |
| 3s.3p(1p).3d 2d3/2 2D1.5 | 856128.0 cm-1 |
| 3s.3p(1p).3d 2p3/2 2P1.5 | 859131.0 cm-1 |
| 3s.3p(1p).3d 2d5/2 2D2.5 | 859267.0 cm-1 |
Contributors
- CHIANTI
- K P Dere
- Martin O'Mullane
---------------------------------------------------------------------------- Data generated from CHIANTI version 6.0 http://www.chianti.rl.ac.uk/ CHIANTI references ------------------ Energy levels : %observed energy levels: Churilov S.S., Levashov V.E., 1993, Physica Scripta 48, 425 %observed energy levels: Redfors A., Litzen U., 1989, J.Opt.Soc.Am.B 6, #8, 1447 %theoretical energy levels: Storey P.J., Mason H.E., Young P.R., 2000, A&ASS 141, 285 %comment Only level 16 does not have an observed energy. I have placed in the third energy column a recommended value for the energy value of this level, based on the theoretical and observed splittings of the 4F levels. It is this energy value which is used to compute the wavelengths of transitions involving level 16 given in the .wgfa file. %produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % P.R.Young Feb 99 A-values levels : %filename: fe_14.wgfa %observed energy levels: Churilov S.S., Levashov V.E., 1993, Physica Scripta 48, 425 %observed energy levels: Redfors A., Litzen U., 1989, J.Opt.Soc.Am.B 6, #8, 1447 %theoretical energy levels: Storey P.J., Mason H.E., Young P.R., 2000, A&ASS 141, 285 %A-values: Storey P.J., Mason H.E., Young P.R., 2000, A&ASS 141, 285 %A-value (2-5): Traebert, E., Heckmann, P.H., Hutton , R., & Martinson, I. 1988, J. Opt. Soc. Am. B, 5, 2173 %comment: This set of radiative data were calculated using the FeXIV model described on p.679 of Storey, Mason & Saraph (1996, A&A 309, 677) and labelled by them as the "extended basis". In Storey, Mason & Young, this basis is referred to as "basis 3". The wavelengths for transitions involving level 16 were derived using the "best guess" energy for level 16 given in the 3rd energy column of the .elvlc file. %comment: added transition experimental A-value 2-5 from Traebert et al 1988 (E. Landi, Sept. 20, 2006). % produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % Peter Young - Feb 1999 Collision strengths : filename: fe_14.splups %effective collision strengths: Storey P.J., Mason H.E., Young P.R., 2000, A&ASS 141, 285 %comment: effective collision strengths were given in the temperature range 5.5 < Log T < 7.2 %effective collision strengths (1-2 transition): Storey PJ, Mason HE, Saraph HE, 1996, A&A 309, 677 %comment: effective collision strengths for the 1-2 transition were given for temperatures lower than Log T = 7.0 %comment: Although data for the 1-2 transition was calculated by Storey, Mason & Young (1999), that presented in Storey, Mason & Saraph (1996) is considered more accurate. Only transitions involving levels 1, 2 and 21 are tabulated here. These are the only levels with significant population. Inclusion of all of the other Fe XIV transitions has negligible effects on the level balance of the ion. For the gf values, I have used those calculated in the "basis 1" model of the ion, which is the one used for the collisional calculation. Note that the gf values in the .wgfa file are from the more accurate "basis 3" model. %Produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % Peter Young Feb 1999 Added to ADAS by ---------------- Author : Martin O'Mullane Date : 28/10/10 ---------------------------------------------------------------------------- Level list : 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 Original level order : 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 26 28 25 27 29 30 31 32 33 34 35 36 37 38 39 40 ------------------------------------------------------------------------------- Filtered adf04 file to - sort energy levels - remove non physical A values from energy level reversals - remove energies above ionisation potential - remove duplicate transitions Code : ADAS utility program, filter04 Date : 28-10-2010 Producer : Martin O'Mullane ------------------------------------------------------------------------------- Regenerated to use the standard ADAS temperature set. Add the transitions in the CHIANTI source which have a transition probability but no accompanying effective collision strength and set these upsilons to zero. Update : Martin O'Mullane Date : 28-10-2010 -------------------------------------------------------------------------------