chv6_ic#ca12.dat
Resolved Specific Ion Data Collections
- Ion
- Ca12+
- Temperature Range
- 7.281 eV → 7281 eV
ADF04
- Filename
- chv6_ic#ca12.dat
- Full Path
- adf04/copch#20/chv6_ic#ca12.dat
Download data
- Spontaneous Emission: Ca+12(i) → Ca+12(j) + hv
- Electron Impact Excitation: Ca+12(i) + e → Ca+12(j) + e
| 2s2.2p4 3p2 3P2.0 | 0.0 cm-1 |
| 2s2.2p4 3p1 3P1.0 | 25015.9 cm-1 |
| 2s2.2p4 3p0 3P0.0 | 29487.7 cm-1 |
| 2s2.2p4 1d2 1D2.0 | 91945.0 cm-1 |
| 2s2.2p4 1s0 1S0.0 | 180687.0 cm-1 |
| 2s.2p5 3p2 3P2.0 | 628533.0 cm-1 |
| 2s.2p5 3p1 3P1.0 | 648949.0 cm-1 |
| 2s.2p5 3p0 3P0.0 | 661061.0 cm-1 |
| 2s.2p5 1p1 1P1.0 | 869796.0 cm-1 |
| 2p6 1s0 1S0.0 | 1474920.0 cm-1 |
| 2s2.2p3(4s).3s 5s2 5S2.0 | 3332410.0 cm-1 |
| 2s2.2p3(4s).3s 3s1 3S1.0 | 3373580.0 cm-1 |
| 2s2.2p3(2d).3s 3d1 3D1.0 | 3452100.0 cm-1 |
| 2s2.2p3(2d).3s 3d2 3D2.0 | 3453110.0 cm-1 |
| 2s2.2p3(2d).3s 3d3 3D3.0 | 3459720.0 cm-1 |
| 2s2.2p3(2d).3s 1d2 1D2.0 | 3476610.0 cm-1 |
| 2s2.2p3(4s).3p 5p1 5P1.0 | 3492940.0 cm-1 |
| 2s2.2p3(4s).3p 5p2 5P2.0 | 3494830.0 cm-1 |
| 2s2.2p3(4s).3p 5p3 5P3.0 | 3499020.0 cm-1 |
| 2s2.2p3(2p).3s 3p0 3P0.0 | 3513600.0 cm-1 |
| 2s2.2p3(2p).3s 3p1 3P1.0 | 3516600.0 cm-1 |
| 2s2.2p3(2p).3s 3p2 3P2.0 | 3526320.0 cm-1 |
| 2s2.2p3(4s).3p 3p1 3P1.0 | 3532550.0 cm-1 |
| 2s2.2p3(4s).3p 3p2 3P2.0 | 3535550.0 cm-1 |
| 2s2.2p3(4s).3p 3p0 3P0.0 | 3536790.0 cm-1 |
| 2s2.2p3(2p).3s 1p1 1P1.0 | 3541870.0 cm-1 |
| 2s2.2p3(2d).3p 3d1 3D1.0 | 3592980.0 cm-1 |
| 2s2.2p3(2d).3p 3d2 3D2.0 | 3605070.0 cm-1 |
| 2s2.2p3(2d).3p 3d3 3D3.0 | 3612090.0 cm-1 |
| 2s2.2p3(2d).3p 1p1 1P1.0 | 3612140.0 cm-1 |
| 2s2.2p3(2d).3p 3f2 3F2.0 | 3616360.0 cm-1 |
| 2s2.2p3(2d).3p 3f3 3F3.0 | 3621840.0 cm-1 |
| 2s2.2p3(2d).3p 3f4 3F4.0 | 3627680.0 cm-1 |
| 2s2.2p3(2d).3p 1f3 1F3.0 | 3629170.0 cm-1 |
| 2s2.2p3(2d).3p 3p1 3P1.0 | 3659430.0 cm-1 |
| 2s2.2p3(2d).3p 3p0 3P0.0 | 3665240.0 cm-1 |
| 2s2.2p3(2d).3p 3p2 3P2.0 | 3677040.0 cm-1 |
| 2s2.2p3(2p).3p 1p1 1P1.0 | 3677770.0 cm-1 |
| 2s2.2p3(2p).3p 3d2 3D2.0 | 3682750.0 cm-1 |
| 2s2.2p3(2p).3p 3s1 3S1.0 | 3683480.0 cm-1 |
| 2s2.2p3(2p).3p 3d3 3D3.0 | 3690720.0 cm-1 |
| 2s2.2p3(2d).3p 1d2 1D2.0 | 3691120.0 cm-1 |
| 2s2.2p3(4s).3d 5d0 5D0.0 | 3698190.0 cm-1 |
| 2s2.2p3(4s).3d 5d1 5D1.0 | 3698360.0 cm-1 |
| 2s2.2p3(4s).3d 5d2 5D2.0 | 3698630.0 cm-1 |
| 2s2.2p3(4s).3d 5d3 5D3.0 | 3699000.0 cm-1 |
| 2s2.2p3(4s).3d 5d4 5D4.0 | 3699760.0 cm-1 |
| 2s2.2p3(2p).3p 3d1 3D1.0 | 3699900.0 cm-1 |
| 2s2.2p3(2p).3p 3p2 3P2.0 | 3713780.0 cm-1 |
| 2s2.2p3(2p).3p 3p1 3P1.0 | 3716370.0 cm-1 |
| 2s2.2p3(2p).3p 3p0 3P0.0 | 3716860.0 cm-1 |
| 2s2.2p3(4s).3d 3d2 3D2.0 | 3741730.0 cm-1 |
| 2s2.2p3(4s).3d 3d1 3D1.0 | 3744680.0 cm-1 |
| 2s2.2p3(4s).3d 3d3 3D3.0 | 3745840.0 cm-1 |
| 2s2.2p3(2p).3p 1d2 1D2.0 | 3750850.0 cm-1 |
| 2s2.2p3(2d).3d 3f2 3F2.0 | 3802460.0 cm-1 |
| 2s2.2p3(2d).3d 3f3 3F3.0 | 3808180.0 cm-1 |
| 2s2.2p3(2p).3p 1s0 1S0.0 | 3811460.0 cm-1 |
| 2s2.2p3(2d).3d 1s0 1S0.0 | 3811660.0 cm-1 |
| 2s2.2p3(2d).3d 3f4 3F4.0 | 3814740.0 cm-1 |
| 2s2.2p3(2d).3d 3g3 3G3.0 | 3820570.0 cm-1 |
| 2s2.2p3(2d).3d 3g4 3G4.0 | 3823850.0 cm-1 |
| 2s2.2p3(2d).3d 3g5 3G5.0 | 3828150.0 cm-1 |
| 2s2.2p3(2d).3d 3d1 3D1.0 | 3829220.0 cm-1 |
| 2s2.2p3(2d).3d 1g4 1G4.0 | 3830980.0 cm-1 |
| 2s2.2p3(2d).3d 3d2 3D2.0 | 3842450.0 cm-1 |
| 2s2.2p3(2d).3d 1p1 1P1.0 | 3845730.0 cm-1 |
| 2s2.2p3(2d).3d 3d3 3D3.0 | 3847900.0 cm-1 |
| 2s2.2p3(2p).3d 1d2 1D2.0 | 3852480.0 cm-1 |
| 2s2.2p3(2d).3d 3p2 3P2.0 | 3855690.0 cm-1 |
| 2s2.2p3(2d).3d 3p0 3P0.0 | 3858300.0 cm-1 |
| 2s2.2p3(2d).3d 3p1 3P1.0 | 3860120.0 cm-1 |
| 2s2.2p3(2d).3d 3s1 3S1.0 | 3866070.0 cm-1 |
| 2s2.2p3(2p).3d 3f3 3F3.0 | 3883660.0 cm-1 |
| 2s2.2p3(2p).3d 3f2 3F2.0 | 3887220.0 cm-1 |
| 2s2.2p3(2d).3d 1f3 1F3.0 | 3889920.0 cm-1 |
| 2s2.2p3(2p).3d 3f4 3F4.0 | 3890950.0 cm-1 |
| 2s2.2p3(2p).3d 3p0 3P0.0 | 3892280.0 cm-1 |
| 2s2.2p3(2p).3d 3p1 3P1.0 | 3896350.0 cm-1 |
| 2s2.2p3(2p).3d 3p2 3P2.0 | 3897020.0 cm-1 |
| 2s2.2p3(2p).3d 3d2 3D2.0 | 3908230.0 cm-1 |
| 2s2.2p3(2p).3d 3d1 3D1.0 | 3914200.0 cm-1 |
| 2s2.2p3(2p).3d 3d3 3D3.0 | 3915250.0 cm-1 |
| 2s2.2p3(2d).3d 1d2 1D2.0 | 3931720.0 cm-1 |
| 2s2.2p3(2p).3d 1f3 1F3.0 | 3935280.0 cm-1 |
| 2s2.2p3(2p).3d 1p1 1P1.0 | 3972700.0 cm-1 |
A+12 20 13 5845430.2 ---------------------------------------------------------------------------- Data generated from CHIANTI version 6.0 http://www.chianti.rl.ac.uk/ CHIANTI references ------------------ Energy levels : %Observed energy levels (1 - 10): Edlen, 1983, Ph. Scr., 28, 51 %Observed energy levels (4,5): Feldman, Curdt, Landi, Wilhelm, 2000, ApJ, 544, 508 %Observed energy levels (11): from the spectrum of Acton et al 1985, ApJ, 291, 865 %Observed energy levels (12 - 16,25 - 26): Doschek et al 1973, J.Opt.Soc.Am, 63, 1463 %Observed energy levels (2s2.2p3.3d configuration): Fawcett & Hayes, 1975, MNRAS, 170, 185 %theoretical energy levels: Landi, E., Bhatia, A.K., 2005, A&A, 444, 305 %comment: theoretical energy levels come from the 24-configuration calculation in Landi & Bhatia (2005) %produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % E. Landi - Mar 2005 A-values levels : %filename: ca_13.wgfa %Observed energy levels (1-10): Edlen, 1983, Ph. Scr., 28, 51 %Observed energy levels (4,5): Feldman, Curdt, Landi, Wilhelm, 2000, ApJ, 544, 508 %Observed energy levels (11): from the spectrum of Acton et al 1985, ApJ, 291, 865 %Observed energy levels (12-16,25-26): Doschek et al 1973, J.Opt.Soc.Am, 63, 1463 %Observed energy levels (2s2.2p3.3d configuration): Fawcett & Hayes, 1975, MNRAS, 170, 185 %theoretical energy levels: Landi, E., Bhatia, A.K., 2005, A&A, 444, 305 %A values and oscillator strengths: Landi, E., Bhatia, A.K., 2005, A&A, 444, 305 %comment: theoretical energies and radiative data come from the 24-configuration calculation in Landi & Bhatia (2005) %produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % E. Landi - Apr 2005 Collision strengths : %filename: ca_13.splups %Collision strengths: Landi & Bhatia 2005, A&A, 444, 305 %Oscillator strengths: Landi & Bhatia 2005, A&A, 444, 305 %comment: oscillator strengths have been taken from the 6-configuration model of Landi & Bhatia (2005) for consistency with the collisional calculation %produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % E. Landi - Mar 2005 Added to ADAS by ---------------- Author : Martin O'Mullane Date : 28/10/10 ---------------------------------------------------------------------------- Unphysical A values. Set A=1.0E-30 for following transitions : 20 21 A = 4.47E-01 24 25 A = 6.68E-08 43 45 A = 4.39E-11 43 49 A = 1.96E-10 44 45 A = 1.04E-03 44 49 A = 1.12E+01 46 47 A = 1.17E-02 46 49 A = 3.06E+01 46 48 A = 3.38E-14 40 49 A = 5.56E+01 60 65 A = 6.56E-01 61 65 A = 2.79E+00 62 65 A = 5.42E-03 63 65 A = 8.67E-02 70 72 A = 8.37E-01 71 72 A = 9.56E-02 ------------------------------------------------------------------------------- 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 Original level order : 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 21 23 25 20 22 24 26 27 28 29 31 30 32 33 34 36 35 37 39 38 45 47 49 40 41 42 43 44 48 46 50 51 52 53 54 55 56 57 65 58 59 60 61 62 64 63 66 67 68 72 69 70 71 73 74 75 76 77 78 79 80 81 83 82 84 85 86 ------------------------------------------------------------------------------- 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 -------------------------------------------------------------------------------