| 2s2.2p3 4s3/2 4S1.5 | 0.0 cm-1 |
| 2s2.2p3 2d3/2 2D1.5 | 110948.0 cm-1 |
| 2s2.2p3 2d5/2 2D2.5 | 118992.0 cm-1 |
| 2s2.2p3 2p1/2 2P0.5 | 176969.0 cm-1 |
| 2s2.2p3 2p3/2 2P1.5 | 188288.0 cm-1 |
| 2s.2p4 4p5/2 4P2.5 | 521094.0 cm-1 |
| 2s.2p4 4p3/2 4P1.5 | 541642.0 cm-1 |
| 2s.2p4 4p1/2 4P0.5 | 551083.0 cm-1 |
| 2s.2p4 2d3/2 2D1.5 | 724962.0 cm-1 |
| 2s.2p4 2d5/2 2D2.5 | 727026.0 cm-1 |
| 2s.2p4 2s1/2 2S0.5 | 840461.0 cm-1 |
| 2s.2p4 2p3/2 2P1.5 | 876284.0 cm-1 |
| 2s.2p4 2p1/2 2P0.5 | 904253.0 cm-1 |
| 2p5 2p3/2 2P1.5 | 1375290.0 cm-1 |
| 2p5 2p1/2 2P0.5 | 1408390.0 cm-1 |
| 2s2.2p2(3p).3s 4p1/2 4P0.5 | 3763830.0 cm-1 |
| 2s2.2p2(3p).3s 4p3/2 4P1.5 | 3778920.0 cm-1 |
| 2s2.2p2(3p).3s 4p5/2 4P2.5 | 3796350.0 cm-1 |
| 2s2.2p2(3p).3s 2p1/2 2P0.5 | 3806610.0 cm-1 |
| 2s2.2p2(3p).3s 2p3/2 2P1.5 | 3826670.0 cm-1 |
| 2s2.2p2(1d).3s 2d5/2 2D2.5 | 3880760.0 cm-1 |
| 2s2.2p2(1d).3s 2d3/2 2D1.5 | 3882500.0 cm-1 |
| 2s2.2p2(3p).3p 2s1/2 2S0.5 | 3904050.0 cm-1 |
| 2s2.2p2(3p).3p 4d1/2 4D0.5 | 3915430.0 cm-1 |
| 2s2.2p2(3p).3p 4d3/2 4D1.5 | 3918610.0 cm-1 |
| 2s2.2p2(3p).3p 4d5/2 4D2.5 | 3932490.0 cm-1 |
| 2s2.2p2(3p).3p 4p3/2 4P1.5 | 3939000.0 cm-1 |
| 2s2.2p2(3p).3p 4p1/2 4P0.5 | 3940220.0 cm-1 |
| 2s2.2p2(3p).3p 4d7/2 4D3.5 | 3948800.0 cm-1 |
| 2s2.2p2(3p).3p 4p5/2 4P2.5 | 3949720.0 cm-1 |
| 2s2.2p2(3p).3p 2d3/2 2D1.5 | 3957740.0 cm-1 |
| 2s2.2p2(1s).3s 2s1/2 2S0.5 | 3964450.0 cm-1 |
| 2s2.2p2(3p).3p 4s3/2 4S1.5 | 3974310.0 cm-1 |
| 2s2.2p2(3p).3p 2d5/2 2D2.5 | 3981240.0 cm-1 |
| 2s2.2p2(3p).3p 2p3/2 2P1.5 | 3990440.0 cm-1 |
| 2s2.2p2(3p).3p 2p1/2 2P0.5 | 3992940.0 cm-1 |
| 2s.2p3(5s).3s 6s5/2 6S2.5 | 4028730.0 cm-1 |
| 2s2.2p2(1d).3p 2f5/2 2F2.5 | 4033330.0 cm-1 |
| 2s2.2p2(1d).3p 2f7/2 2F3.5 | 4039270.0 cm-1 |
| 2s2.2p2(1d).3p 2d3/2 2D1.5 | 4064380.0 cm-1 |
| 2s2.2p2(1d).3p 2d5/2 2D2.5 | 4068250.0 cm-1 |
| 2s2.2p2(1d).3p 2p1/2 2P0.5 | 4082940.0 cm-1 |
| 2s2.2p2(3p).3d 4f3/2 4F1.5 | 4090490.0 cm-1 |
| 2s2.2p2(3p).3d 4f5/2 4F2.5 | 4097600.0 cm-1 |
| 2s2.2p2(1d).3p 2p3/2 2P1.5 | 4100270.0 cm-1 |
| 2s2.2p2(3p).3d 4f7/2 4F3.5 | 4108850.0 cm-1 |
| 2s2.2p2(3p).3d 4d3/2 4D1.5 | 4117770.0 cm-1 |
| 2s.2p3(5s).3s 4s3/2 4S1.5 | 4121680.0 cm-1 |
| 2s2.2p2(3p).3d 4d1/2 4D0.5 | 4121680.0 cm-1 |
| 2s2.2p2(3p).3d 4d5/2 4D2.5 | 4122030.0 cm-1 |
| 2s2.2p2(3p).3d 4f9/2 4F4.5 | 4122810.0 cm-1 |
| 2s2.2p2(3p).3d 2p3/2 2P1.5 | 4128950.0 cm-1 |
| 2s2.2p2(3p).3d 4d7/2 4D3.5 | 4130550.0 cm-1 |
| 2s2.2p2(1s).3p 2p1/2 2P0.5 | 4134470.0 cm-1 |
| 2s2.2p2(1s).3p 2p3/2 2P1.5 | 4135650.0 cm-1 |
| 2s2.2p2(3p).3d 2f5/2 2F2.5 | 4136520.0 cm-1 |
| 2s2.2p2(3p).3d 2p1/2 2P0.5 | 4145940.0 cm-1 |
| 2s2.2p2(3p).3d 4p5/2 4P2.5 | 4151590.0 cm-1 |
| 2s2.2p2(3p).3d 4p3/2 4P1.5 | 4157710.0 cm-1 |
| 2s2.2p2(3p).3d 2f7/2 2F3.5 | 4160510.0 cm-1 |
| 2s2.2p2(3p).3d 4p1/2 4P0.5 | 4160870.0 cm-1 |
| 2s2.2p2(3p).3d 2d3/2 2D1.5 | 4195720.0 cm-1 |
| 2s2.2p2(3p).3d 2d5/2 2D2.5 | 4199250.0 cm-1 |
| 2s2.2p2(1d).3d 2f7/2 2F3.5 | 4214470.0 cm-1 |
| 2s2.2p2(1d).3d 2g9/2 2G4.5 | 4218530.0 cm-1 |
| 2s2.2p2(1d).3d 2d3/2 2D1.5 | 4231700.0 cm-1 |
| 2s2.2p2(1d).3d 2d5/2 2D2.5 | 4234870.0 cm-1 |
| 2s2.2p2(1d).3d 2g7/2 2G3.5 | 4243720.0 cm-1 |
| 2s2.2p2(1d).3d 2p1/2 2P0.5 | 4251420.0 cm-1 |
| 2s2.2p2(1d).3d 2f5/2 2F2.5 | 4252530.0 cm-1 |
| 2s2.2p2(1d).3d 2p3/2 2P1.5 | 4260680.0 cm-1 |
| 2s2.2p2(1d).3d 2s1/2 2S0.5 | 4267570.0 cm-1 |
| 2s.2p3(3d).3s 4d3/2 4D1.5 | 4273230.0 cm-1 |
| 2s.2p3(3d).3s 4d5/2 4D2.5 | 4273630.0 cm-1 |
| 2s.2p3(3d).3s 4d1/2 4D0.5 | 4273840.0 cm-1 |
| 2s.2p3(3d).3s 4d7/2 4D3.5 | 4277570.0 cm-1 |
| 2s2.2p2(1s).3d 2d5/2 2D2.5 | 4315350.0 cm-1 |
| 2s2.2p2(1s).3d 2d3/2 2D1.5 | 4320930.0 cm-1 |
| 2s.2p3(3d).3s 2d3/2 2D1.5 | 4326260.0 cm-1 |
| 2s.2p3(3d).3s 2d5/2 2D2.5 | 4327960.0 cm-1 |
| 2s.2p3(3p).3s 4p1/2 4P0.5 | 4356320.0 cm-1 |
| 2s.2p3(3p).3s 4p3/2 4P1.5 | 4358500.0 cm-1 |
| 2s.2p3(3p).3s 4p5/2 4P2.5 | 4362780.0 cm-1 |
| 2s.2p3(3p).3s 2p1/2 2P0.5 | 4407080.0 cm-1 |
| 2s.2p3(3p).3s 2p3/2 2P1.5 | 4409880.0 cm-1 |
| 2s.2p3(3s).3s 4s3/2 4S1.5 | 4513820.0 cm-1 |
| 2s.2p3(1d).3s 2d5/2 2D2.5 | 4528300.0 cm-1 |
| 2s.2p3(1d).3s 2d3/2 2D1.5 | 4529000.0 cm-1 |
| 2s.2p3(3s).3s 2s1/2 2S0.5 | 4540330.0 cm-1 |
| 2s.2p3(1p).3s 2p3/2 2P1.5 | 4610320.0 cm-1 |
| 2s.2p3(1p).3s 2p1/2 2P0.5 | 4611470.0 cm-1 |
A+13 20 14 6517328.0 ---------------------------------------------------------------------------- Data generated from CHIANTI version 6.0 http://www.chianti.rl.ac.uk/ CHIANTI references ------------------ Energy levels : %Observed energy levels (1-6): Feldman et al, 2000, ApJ, 544, 508 %Observed energy levels (6-15): Edlen, 1984, Phys.Scripta, 30, 135 %Observed energy levels (3d: 52,56,57,58,62,63,67,68,70,74): J.R. Fuhr, D.E. Kelleher, W.C. Martin, A. Musgrove, J. Sugar, W.L. Wiese, G.R. Dalton, R.A. Dragoset, P.J. Mohr, K. Olsen, J. Reader, E.B. Saloman, C.J. Sansonetti, G. Wiersma, "NIST Atomic Spectra Database" Ver. 2.0, March 1999, NIST Physical Reference Data %Observed energy levels (3s: 17,18,20): Kaufman, V., Sugar, J., Cooper, D., 1982, Phys. Scr., 26, 163 %Theoretical energy levels: Bhatia & Landi 2005, ADNDT, 90, 177 %comment: theoretical energy levels come from the 24-configuration calculation in Bhatia & Landi (2005) % produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % Enrico Landi - April 2004 A-values levels : %filename: ca_14.wgfa %Observed energy levels (1-6): Feldman et al, 2000, ApJ, 544, 508 %Observed energy levels (6-15): Edlen, 1984, Phys.Scripta, 30, 135 %Observed energy levels (3d: 52,56,57,58,62,63,67,68,70,74): J.R. Fuhr, D.E. Kelleher, W.C. Martin, A. Musgrove, J. Sugar, W.L. Wiese, G.R. Dalton, R.A. Dragoset, P.J. Mohr, K. Olsen, J. Reader, E.B. Saloman, C.J. Sansonetti, G. Wiersma, "NIST Atomic Spectra Database" Ver. 2.0, March 1999, NIST Physical Reference Data %Observed energy levels (3s: 17,18,20): Kaufman, V., Sugar, J., Cooper, D., 1982, Phys. Scr., 26, 163 %Theoretical energy levels: 24-conf. model from Bhatia & Landi 2005, ADNDT, 444, 90, 177 %A values and oscillator strengths: Bhatia & Landi 2005, ADNDT, 444, 90, 177 %comment: theoretical energy levels and all radiative data come from the 24-configuration calculation in Bhatia & Landi (2005) % produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % Enrico Landi - April 2004 Collision strengths : %filename: ca_14.splups %Collision strengths: Landi & Bhatia, 2005, ADNDT, 90, 177 %Oscillator strengths: Landi & Bhatia, 2005, ADNDT, 90, 177 %comment: oscillator strengths have been taken from the 6-configuration model of Bhatia & Landi (2005) for consistency with the collisional calculation % produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % E. Landi - Apr 2004 Added to ADAS by ---------------- Author : Martin O'Mullane Date : 28/10/10 ---------------------------------------------------------------------------- Unphysical A values. Set A=1.0E-30 for following transitions : 33 36 A = 2.54E+00 34 36 A = 1.47E-03 35 36 A = 2.62E-01 56 60 A = 1.64E+02 56 61 A = 7.34E-04 57 61 A = 1.45E+00 58 60 A = 1.40E+00 58 61 A = 3.52E-04 59 60 A = 1.06E-08 59 61 A = 1.38E+00 73 74 A = 2.26E-03 73 76 A = 5.00E-09 71 76 A = 9.28E-10 79 81 A = 2.29E+01 79 83 A = 8.45E+00 80 81 A = 1.09E-05 80 83 A = 1.16E+02 82 83 A = 1.24E+00 77 83 A = 3.84E+03 ------------------------------------------------------------------------------- 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 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 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 24 23 25 26 27 28 29 30 31 36 32 33 34 35 37 38 39 40 41 42 43 44 45 46 48 47 49 51 50 52 53 60 61 54 55 56 57 58 59 62 63 64 65 66 67 68 69 70 74 76 71 72 73 75 81 83 77 78 79 80 82 84 85 86 87 88 89 90 91 ------------------------------------------------------------------------------- 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 -------------------------------------------------------------------------------