lilike_lgy10#ar15.dat
Resolved Specific Ion Data Collections
- Ion
- Ar15+
- Temperature Range
- 4.412 eV → 4.412 x 104 eV
ADF04
- Filename
- lilike_lgy10#ar15.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#ar15.dat
Download data
- Spontaneous Emission: Ar+15(i) → Ar+15(j) + hv
- Electron Impact Excitation: Ar+15(i) + e → Ar+15(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 257751.0 cm-1 |
| 2p1 2P1.5 | 283061.0 cm-1 |
| 3s1 2S0.5 | 4176520.0 cm-1 |
| 3p1 2P0.5 | 4247710.0 cm-1 |
| 3p1 2P1.5 | 4255120.0 cm-1 |
| 3d1 2D1.5 | 4282320.0 cm-1 |
| 3d1 2D2.5 | 4284680.0 cm-1 |
| 4s1 2S0.5 | 5606430.0 cm-1 |
| 4p1 2P0.5 | 5635710.0 cm-1 |
| 4p1 2P1.5 | 5638800.0 cm-1 |
| 4d1 2D1.5 | 5650090.0 cm-1 |
| 4d1 2D2.5 | 5651080.0 cm-1 |
| 4f1 2F2.5 | 5651660.0 cm-1 |
| 4f1 2F3.5 | 5652160.0 cm-1 |
| 5s1 2S0.5 | 6261140.0 cm-1 |
| 5p1 2P0.5 | 6275930.0 cm-1 |
| 5p1 2P1.5 | 6277500.0 cm-1 |
| 5d1 2D1.5 | 6283230.0 cm-1 |
| 5d1 2D2.5 | 6283740.0 cm-1 |
| 5f1 2F2.5 | 6284060.0 cm-1 |
| 5f1 2F3.5 | 6284310.0 cm-1 |
| 5g1 2G3.5 | 6284320.0 cm-1 |
| 5g1 2G4.5 | 6284470.0 cm-1 |
| 1s1 2s2 2S0.5 | 24874300.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 24938700.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 24947000.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 24962300.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 25142900.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 25154900.0 cm-1 |
| 1s1 2p2 4P0.5 | 25218400.0 cm-1 |
| 1s1 2p2 4P1.5 | 25227900.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 25241400.0 cm-1 |
| 1s1 2p2 4P2.5 | 25241600.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 25247300.0 cm-1 |
| 1s1 2p2 2D1.5 | 25361300.0 cm-1 |
| 1s1 2p2 2D2.5 | 25365300.0 cm-1 |
| 1s1 2p2 2P0.5 | 25390100.0 cm-1 |
| 1s1 2p2 2P1.5 | 25411400.0 cm-1 |
| 1s1 2p2 2S0.5 | 25546100.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 29164600.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 29232200.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 29255200.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 29256500.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 29261300.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 29265500.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 29265800.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 29312000.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 29312900.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 29314200.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 29316100.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 29339400.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 29349400.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 29349400.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 29363000.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 29370400.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 29385300.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 29399900.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 29405900.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 29407700.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 29413300.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 29423600.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 29431900.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 29433400.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 29436900.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 29443400.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 29454100.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 29462700.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 29462800.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 29463900.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 29469100.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 29471000.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 29475900.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 29476800.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 29477200.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 29480700.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 29486300.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 29486900.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 29488100.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 29491000.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 29509000.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 29511000.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 29511100.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 29513100.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 29514800.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 29515100.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 29522800.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 29523700.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 29533800.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 29536500.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 29538100.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 29539800.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 29541700.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 29567700.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 29577000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 29577800.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 29578400.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 29579000.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 29586000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 29620200.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 29622400.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 29626500.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 29637400.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 29642300.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 29661600.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 29666500.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 30661400.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 30683600.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 30694100.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 30694900.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 30696500.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 30705000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 30705600.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 30718100.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 30718300.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 30718700.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 30719200.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 30729800.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 30730000.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 30735900.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 30736000.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 30736200.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 30736500.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 30739800.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 30739900.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 30820200.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 30828700.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 30835100.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 30844000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 30848900.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 30849700.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 30851600.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 30854200.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 30856900.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 30861300.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 30862400.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 30866000.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 30869700.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 30872700.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 30872800.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 30873800.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 30874600.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 30874800.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 30875500.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 30877100.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 30883000.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 30883200.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 30883400.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 30883400.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 30885100.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 30887300.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 30888300.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 30889200.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 30890000.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 30890200.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 30890700.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 30891100.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 30894600.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 30895400.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 30895600.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 30896000.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 30896500.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 30897000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 30897900.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 30901600.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 30902100.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 30903500.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 30906000.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 30908900.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 30909200.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 30910300.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 30912400.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 30914000.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 30914100.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 30916400.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 30916900.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 30917000.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 30917300.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 30918800.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 30919900.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 30920200.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 30920700.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 30922100.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 30924400.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 30924500.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 30960700.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 30960900.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 30985100.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 30985200.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 30986400.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 30988200.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 31000300.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 31004900.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 31005800.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 31007400.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 31009500.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 31012200.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 31012700.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 31017900.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 31019800.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 31019800.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 31019900.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 31024600.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 31025300.0 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 = 1.28136 2S = 1.04052 2P = 0.93965 3S = 1.02761 3P = 0.93258 3D = 0.86682 4S = 1.02632 4P = 0.93219 4D = 0.86863 4F = 1.01227 5S = 1.02802 5P = 0.93350 5D = 0.87282 5F = 0.85031 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 883.0170 Rydbergs (12014.329302 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.0122454 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used from the last threshold up to 3.067274 Z**2 Rydbergs (9390 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used from first threshold up to 3.067274 Z**2 Rydbergs (9390 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 = 1.28617 2S = 1.04253 2P = 0.94219 3S = 1.03003 3P = 0.93419 3D = 0.87071 4S = 1.03023 4P = 0.93503 4D = 0.87574 4F = 0.98643 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. 40 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 (0.0306135 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used from the last threshold up to 2.999940 Z**2 Rydbergs (9183.86502 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used from first threshold up to 2.999940 Z**2 Rydbergs (9183.86502 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 2.34219 3 2.57527 4 38.0548 5 38.6966 6 38.7658 7 39.0129 8 39.0347 9 51.0833 10 51.3477 11 51.3766 12 51.4777 13 51.487 16 57.041 17 57.180 18 57.195 19 57.247 20 57.251 25 226.30 26 226.90 27 226.96 28 227.12 31 229.45 32 229.55 33 229.61 34 229.67 35 229.67 36 230.72 37 230.73 Produced by: Guiyun Liang Date: 24/11/10 ------------------------------------------------------------------------