lilike_lgy10#s13.dat
Resolved Specific Ion Data Collections
- Ion
- S13+
- Temperature Range
- 3.378 eV → 3.378 x 104 eV
ADF04
- Filename
- lilike_lgy10#s13.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#s13.dat
Download data
- Spontaneous Emission: S+13(i) → S+13(j) + hv
- Electron Impact Excitation: S+13(i) + e → S+13(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 225178.0 cm-1 |
| 2p1 2P1.5 | 240081.0 cm-1 |
| 3s1 2S0.5 | 3220240.0 cm-1 |
| 3p1 2P0.5 | 3282310.0 cm-1 |
| 3p1 2P1.5 | 3286680.0 cm-1 |
| 3d1 2D1.5 | 3309960.0 cm-1 |
| 3d1 2D2.5 | 3311340.0 cm-1 |
| 4s1 2S0.5 | 4319880.0 cm-1 |
| 4p1 2P0.5 | 4345390.0 cm-1 |
| 4p1 2P1.5 | 4347220.0 cm-1 |
| 4d1 2D1.5 | 4356880.0 cm-1 |
| 4d1 2D2.5 | 4357470.0 cm-1 |
| 4f1 2F2.5 | 4357940.0 cm-1 |
| 4f1 2F3.5 | 4358240.0 cm-1 |
| 5s1 2S0.5 | 4822780.0 cm-1 |
| 5p1 2P0.5 | 4835670.0 cm-1 |
| 5p1 2P1.5 | 4836590.0 cm-1 |
| 5d1 2D1.5 | 4841500.0 cm-1 |
| 5d1 2D2.5 | 4841800.0 cm-1 |
| 5f1 2F2.5 | 4842070.0 cm-1 |
| 5f1 2F3.5 | 4842220.0 cm-1 |
| 5g1 2G3.5 | 4842220.0 cm-1 |
| 5g1 2G4.5 | 4842310.0 cm-1 |
| 1s1 2s2 2S0.5 | 19453500.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 19510600.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 19515600.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 19524600.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 19686600.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 19693600.0 cm-1 |
| 1s1 2p2 4P0.5 | 19751900.0 cm-1 |
| 1s1 2p2 4P1.5 | 19757300.0 cm-1 |
| 1s1 2p2 4P2.5 | 19765600.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 19773000.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 19776600.0 cm-1 |
| 1s1 2p2 2D1.5 | 19872800.0 cm-1 |
| 1s1 2p2 2D2.5 | 19874500.0 cm-1 |
| 1s1 2p2 2P0.5 | 19899600.0 cm-1 |
| 1s1 2p2 2P1.5 | 19911600.0 cm-1 |
| 1s1 2p2 2S0.5 | 20034900.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 22776000.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 22835000.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 22855500.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 22856400.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 22859100.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 22862100.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 22862400.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 22903100.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 22903600.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 22904500.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 22905600.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 22928300.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 22935200.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 22935200.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 22950700.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 22955200.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 22963800.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 22980800.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 22984200.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 22989600.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 22993000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 22999000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 23006000.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 23006200.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 23006600.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 23020700.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 23024200.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 23032100.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 23035800.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 23036300.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 23039500.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 23040000.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 23043700.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 23044200.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 23046000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 23048100.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 23050300.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 23052100.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 23052800.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 23059600.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 23070200.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 23075200.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 23075500.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 23076800.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 23077800.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 23078000.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 23082100.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 23086000.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 23092000.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 23094100.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 23095300.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 23097000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 23099300.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 23123700.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 23130100.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 23131900.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 23132400.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 23132900.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 23137300.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 23167100.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 23168500.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 23174500.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 23182400.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 23185400.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 23204600.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 23207600.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 23934900.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 23954100.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 23963400.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 23963800.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 23964700.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 23972200.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 23972600.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 23983400.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 23983500.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 23983800.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 23984100.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 23993500.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 23993600.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 23998600.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 23998700.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 23998800.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 23999000.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 24002000.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 24002100.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 24073000.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 24082100.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 24086100.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 24093500.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 24095500.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 24096500.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 24100400.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 24103200.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 24105800.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 24107600.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 24110300.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 24111800.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 24114800.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 24115300.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 24115400.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 24118000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 24118800.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 24119300.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 24119600.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 24122300.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 24123100.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 24123200.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 24126300.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 24127200.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 24127700.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 24128200.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 24131300.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 24131800.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 24132800.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 24133200.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 24133300.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 24134100.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 24135100.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 24135200.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 24136000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 24137100.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 24137300.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 24137700.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 24138400.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 24139900.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 24142000.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 24142900.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 24143200.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 24144800.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 24145700.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 24145900.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 24148600.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 24149000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 24149500.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 24151000.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 24151200.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 24152000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 24153200.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 24153300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 24153600.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 24154400.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 24154900.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 24155700.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 24157800.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 24158100.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 24191400.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 24191500.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 24212500.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 24212600.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 24213100.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 24214400.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 24225500.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 24228800.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 24229400.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 24231100.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 24232400.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 24234900.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 24235200.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 24240600.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 24241500.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 24241500.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 24241800.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 24245900.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 24246300.0 cm-1 |
Contributors
- Guiyun Liang
- Nigel Badnell
------------------------------------------------------------------------ Result of ICFT R-matrix calculation for outer shell excitation +++++++++++++++++++++++++++++++++++ Calculation automated by offline ADAS code ADAS8#3 Summary Information +++++++++++++++++++ * Ionisation energy taken from ADAS adf00 files * Energy levels calculated by AUTOSTRUCTURE * Radiative rates calculated by AUTOSTRUCTURE * Effective collision strengths calculated by ICFT R-matrix calculation using target structure from AUTOSTRUCTURE. Calculation details +++++++++++++++++++ The following scaling parameters on bound orbitals were used: 1S = 1.28087 2S = 1.03777 2P = 0.93576 3S = 1.02526 3P = 0.92883 3D = 0.86236 4S = 1.02391 4P = 0.92845 4D = 0.86423 4F = 1.00598 5S = 1.02566 5P = 0.93011 5D = 0.86814 5F = 0.84759 5G = 1.00000 An exchange calculation was performed up to J=10 A non-exchange calculation was then performed up to J=40 Followed by a top-up calculation to J -> infinity. 60 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 675.9065 Rydbergs (9196.383839 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.009197656 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (22.99414 eV) was used from the last threshold up to 3.187769 Z**2 Rydbergs (7330 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (22.99414 eV) was used from first threshold up to 3.187769 Z**2 Rydbergs (7330 eV) in the non-exchange calculation. Dipole and Born limits were used from the last calculated energy points up to infinite energy to complete the effective collision strengths Produced by: Guiyun Liang Date: 13/10/10 ------------------------------------------------------------------------ Result of ICFT R-matrix calculation for core-excitation G.Y. Liang, and N.R. Badnell, A&A (2010) +++++++++++++++++++++++++++++++++++ Calculation automated by offline ADAS code ADAS8#3 Summary Information +++++++++++++++++++ * Ionisation energy taken from ADAS adf00 files * Energy levels calculated by AUTOSTRUCTURE * Radiative rates calculated by AUTOSTRUCTURE * Effective collision strengths calculated by ICFT R-matrix calculation using target structure from AUTOSTRUCTURE. Calculation details +++++++++++++++++++ The following scaling parameters on bound orbitals were used: 1S = 1.28554 2S = 1.03966 2P = 0.93847 3S = 1.02802 3P = 0.93062 3D = 0.86620 4S = 1.02783 4P = 0.93142 4D = 0.87127 4F = 0.99405 An exchange calculation was performed up to J=10 A non-exchange calculation was then performed up to J=40 Followed by a top-up calculation to J -> infinity. 45 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 0 Rydbergs (0.000000 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.02299414 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (22.99414 eV) was used from the last threshold up to 3.187769 Z**2 Rydbergs (7330 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (22.99414 eV) was used from first threshold up to 3.187769 Z**2 Rydbergs (7330 eV) in the non-exchange calculation. Dipole and Born limits were used from the last calculated energy points up to infinite energy to complete the effective collision strengths NIST v4 energy (Ryd) 2 2.04457 3 2.18184 4 29.3437 5 29.9080 6 29.9492 7 30.1562 8 30.1691 9 39.3640 10 39.5944 11 39.6115 12 39.7000 13 39.7058 14 39.7096 15 39.7124 16 43.9463 19 44.1155 20 44.1183 21 44.1211 22 44.1225 25 176.986 26 177.518 27 177.556 28 177.646 29 179.120 30 179.191 31 179.714 32 179.774 33 179.841 34 179.855 35 179.891 36 180.779 37 180.786 38 181.014 39 181.146 40 182.201 46 207.976 47 207.986 53 208.644 54 208.640 58 209.112 59 209.150 63 209.264 64 209.273 75 209.736 76 209.736 80 209.769 81 209.868 82 209.914 85 209.932 93 210.148 96 210.461 97 210.461 98 210.466 99 210.516 Produced by: Guiyun Liang Date: 25/11/10 ------------------------------------------------------------------------