chv6_ic#mg6.dat
Resolved Specific Ion Data Collections
- Ion
- Mg6+
- Temperature Range
- 2.111 eV → 2111 eV
ADF04
- Filename
- chv6_ic#mg6.dat
- Full Path
- adf04/copch#12/chv6_ic#mg6.dat
Download data
- Spontaneous Emission: Mg+6(i) → Mg+6(j) + hv
- Electron Impact Excitation: Mg+6(i) + e → Mg+6(j) + e
| 2s2.2p2 3p0 3P0.0 | 0.0 cm-1 |
| 2s2.2p2 3p1 3P1.0 | 1123.0 cm-1 |
| 2s2.2p2 3p2 3P2.0 | 2953.0 cm-1 |
| 2s2.2p2 1d2 1D2.0 | 43502.0 cm-1 |
| 2s2.2p2 1s0 1S0.0 | 81506.0 cm-1 |
| 2s.2p3 5s2 5S2.0 | 106244.0 cm-1 |
| 2s.2p3 3d2 3D2.0 | 233763.0 cm-1 |
| 2s.2p3 3d1 3D1.0 | 233777.0 cm-1 |
| 2s.2p3 3d3 3D3.0 | 233843.0 cm-1 |
| 2s.2p3 3p0 3P0.0 | 275221.0 cm-1 |
| 2s.2p3 3p1 3P1.0 | 275251.0 cm-1 |
| 2s.2p3 3p2 3P2.0 | 275302.0 cm-1 |
| 2s.2p3 1d2 1D2.0 | 368657.0 cm-1 |
| 2s.2p3 3s1 3S1.0 | 376345.0 cm-1 |
| 2s.2p3 1p1 1P1.0 | 410197.0 cm-1 |
| 2p4 3p2 3P2.0 | 554688.0 cm-1 |
| 2p4 3p1 3P1.0 | 556759.0 cm-1 |
| 2p4 3p0 3P0.0 | 557700.0 cm-1 |
| 2p4 1d2 1D2.0 | 596878.0 cm-1 |
| 2p4 1s0 1S0.0 | 682221.0 cm-1 |
| 2s2.2p3s 3p0 3P0.0 | 1066140.0 cm-1 |
| 2s2.2p3s 3p1 3P1.0 | 1067010.0 cm-1 |
| 2s2.2p3s 3p2 3P2.0 | 1069250.0 cm-1 |
| 2s2.2p3s 1p1 1P1.0 | 1080140.0 cm-1 |
| 2s2.2p3p 1p1 1P1.0 | 1122560.0 cm-1 |
| 2s2.2p3p 3d1 3D1.0 | 1126860.0 cm-1 |
| 2s2.2p3p 3d2 3D2.0 | 1127770.0 cm-1 |
| 2s2.2p3p 3d3 3D3.0 | 1129730.0 cm-1 |
| 2s2.2p3p 3s1 3S1.0 | 1136690.0 cm-1 |
| 2s2.2p3p 3p0 3P0.0 | 1149170.0 cm-1 |
| 2s2.2p3p 3p1 3P1.0 | 1149980.0 cm-1 |
| 2s2.2p3p 3p2 3P2.0 | 1151100.0 cm-1 |
| 2s2.2p3p 1d2 1D2.0 | 1164570.0 cm-1 |
| 2s2.2p3p 1s0 1S0.0 | 1185990.0 cm-1 |
| 2s2.2p3d 3f2 3F2.0 | 1195550.0 cm-1 |
| 2s2.2p3d 3f3 3F3.0 | 1197020.0 cm-1 |
| 2s2.2p3d 1d2 1D2.0 | 1198360.0 cm-1 |
| 2s2.2p3d 3f4 3F4.0 | 1198600.0 cm-1 |
| 2s2.2p3d 3d1 3D1.0 | 1210410.0 cm-1 |
| 2s2.2p3d 3d2 3D2.0 | 1210760.0 cm-1 |
| 2s2.2p3d 3d3 3D3.0 | 1211700.0 cm-1 |
| 2s2.2p3d 3p2 3P2.0 | 1214610.0 cm-1 |
| 2s2.2p3d 3p1 3P1.0 | 1215250.0 cm-1 |
| 2s2.2p3d 3p0 3P0.0 | 1215570.0 cm-1 |
| 2s2.2p3d 1p1 1P1.0 | 1233650.0 cm-1 |
| 2s2.2p3d 1f3 1F3.0 | 1234090.0 cm-1 |
Contributors
- CHIANTI
- Kanti Aggarwal
- Martin O'Mullane
---------------------------------------------------------------------------- Data generated from CHIANTI version 6.0 http://www.chianti.rl.ac.uk/ CHIANTI references ------------------ Energy levels : %energy levels (level 2): Kelly, D.M., & Lacy, J.H., 1995, ApJ, 454, L161 %energy levels (level 3): Kelly, D.M., & Lacy, J.H., 1995, ApJ, 454, L161 %energy levels (level 3): Feuchtgruber, H., Lutz, D.A., Beintema, E.A. et al., 1997, ApJ, 487, 962 %energy levels (level 4): Young, P.R., Dupree, A.K., Espey, B.R., & Kenyon, S.J., 2006, ApJ, 650, 1091 %energy levels: Martin, W. C., Sugar, J., Musgrove, A., and Dalton, G. R., 1995, NIST Database for Atomic Spectroscopy, Version 1.0, NIST Standar %Theoretical energy levels: Bhatia, A.K., Doschek, G.A., 1995, ADNDT, 60, 145 %comment: the Kelly & Lacy and Feuchtgruber measurements are combined to give the level 3 energy % produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % P.R. Young - 3-Dec-2007 A-values levels : %filename: mg_7.wgfa %energy levels (level 2): Kelly, D.M., & Lacy, J.H., 1995, ApJ, 454, L161 %energy levels (level 3): Kelly, D.M., & Lacy, J.H., 1995, ApJ, 454, L161 %energy levels (level 3): Feuchtgruber, H., Lutz, D.A., Beintema, E.A. et al., 1997, ApJ, 487, 962 %energy levels (level 4): Young, P.R., Dupree, A.K., Espey, B.R., & Kenyon, S.J., 2006, ApJ, 650, 1091 %energy levels: Martin, W. C., Sugar, J., Musgrove, A., and Dalton, G. R., 1995, NIST Database for Atomic Spectroscopy, Version 1.0, NIST Standar %Theoretical energy levels: Bhatia, A.K.,Doschek, G.A., ADNDT, 60, 145, 1995 %oscillator strengths: Bhatia, A.K., Doschek, G.A.,1995, ADNDT, 60, 145 %A-values (2-4 and 3-4 transitions): Storey PJ, Zeippen CJ, MNRAS 312, 813, 2000 %A-values (other ground transitions): Galavis, M.E., Mendoza, C., Zeippen, C.J., 1997, A&AS, 123, 159 %comment: the Kelly & Lacy and Feuchtgruber measurements are combined to give the level 3 energy % produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % P.R. Young - 3-Dec-2006 Collision strengths : %filename: mg_7.splups %oscillator strengths: Bhatia, A.K., Doschek, G.A., 1995, ADNDT, 60, 145 %upsilons (ground configuration, levels 1 to 5): Lennon, D.J., Burke, V.M., 1994, A&AS, 103, 273 %upsilons (ground configuration, levels 1 to 5): Aggarwal, K, 1984, Sol. Phys., 94, 75 %upsilons (ground configuration, levels 1 to 5): Aggarwal, K, 1984, ApJS, 56, 303 %collision strengths (all other transitions): Bhatia, A.K., Doschek, G.A., 1995, ADNDT, 60, 145 %comment: The Lennon & Burke upsilons are tabulated between logT=3.0-5.0, and the T_max of Mg VII is 5.7. The Aggarwal data go up to logT=7.7. I've thus used all of the Lennon & Burke data and appended the Aggarwal data for temperatures logT=5.2-7.6. It was necessary to scale the Aggarwal by the ratio of the Lennon & Burke data to the Aggarwal data at logT=5.0 to ensure a smooth join between the two data-sets. The scale factor varied from 0.82 (4-5) to 1.19 (1-5). The fits to the ground configuration upsilons are accurate to 1.2% over the temperature range logT=3.8-6.2. % produced as part of the Arcetri/Cambridge/NRL 'CHIANTI' atomic data base collaboration % % P.R. Young and E.Landi - 3-Dec-2007 Added to ADAS by ---------------- Author : Martin O'Mullane Date : 28/10/10 ---------------------------------------------------------------------------- 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 -------------------------------------------------------------------------------