lilike_lgy10#o5.dat
Resolved Specific Ion Data Collections
- Ion
- O5+
- Temperature Range
- 0.620 eV → 6204 eV
ADF04
- Filename
- lilike_lgy10#o5.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#o5.dat
Download data
- Spontaneous Emission: O+5(i) → O+5(j) + hv
- Electron Impact Excitation: O+5(i) + e → O+5(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 97154.0 cm-1 |
| 2p1 2P1.5 | 97673.0 cm-1 |
| 3s1 2S0.5 | 639381.0 cm-1 |
| 3p1 2P0.5 | 665635.0 cm-1 |
| 3p1 2P1.5 | 665788.0 cm-1 |
| 3d1 2D1.5 | 673882.0 cm-1 |
| 3d1 2D2.5 | 673928.0 cm-1 |
| 4s1 2S0.5 | 851905.0 cm-1 |
| 4p1 2P0.5 | 862601.0 cm-1 |
| 4p1 2P1.5 | 862665.0 cm-1 |
| 4d1 2D1.5 | 866053.0 cm-1 |
| 4d1 2D2.5 | 866072.0 cm-1 |
| 4f1 2F2.5 | 866196.0 cm-1 |
| 4f1 2F3.5 | 866206.0 cm-1 |
| 5s1 2S0.5 | 947872.0 cm-1 |
| 5p1 2P0.5 | 953250.0 cm-1 |
| 5p1 2P1.5 | 953283.0 cm-1 |
| 5d1 2D1.5 | 955009.0 cm-1 |
| 5d1 2D2.5 | 955019.0 cm-1 |
| 5f1 2F2.5 | 955090.0 cm-1 |
| 5f1 2F3.5 | 955095.0 cm-1 |
| 5g1 2G3.5 | 955096.0 cm-1 |
| 5g1 2G4.5 | 955099.0 cm-1 |
| 1s1 2s2 2S0.5 | 4453770.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 4483480.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 4483670.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 4483980.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 4553340.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 4553580.0 cm-1 |
| 1s1 2p2 4P0.5 | 4590630.0 cm-1 |
| 1s1 2p2 4P1.5 | 4590820.0 cm-1 |
| 1s1 2p2 4P2.5 | 4591130.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 4599450.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 4599580.0 cm-1 |
| 1s1 2p2 2D1.5 | 4636500.0 cm-1 |
| 1s1 2p2 2D2.5 | 4636520.0 cm-1 |
| 1s1 2p2 2P0.5 | 4646280.0 cm-1 |
| 1s1 2p2 2P1.5 | 4646660.0 cm-1 |
| 1s1 2p2 2S0.5 | 4712820.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 5147680.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 5174020.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 5183570.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 5183600.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 5184480.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 5184520.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 5184580.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 5201650.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 5201670.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 5201690.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 5201730.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 5211960.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 5214830.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 5214830.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 5233070.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 5233230.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 5233520.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 5235700.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 5235800.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 5247250.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 5247370.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 5247560.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 5247810.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 5248780.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 5248820.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 5257890.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 5259860.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 5260150.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 5260220.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 5260290.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 5265490.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 5265600.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 5265750.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 5265950.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 5269410.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 5269460.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 5269710.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 5269810.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 5269980.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 5274480.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 5274880.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 5277840.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 5277930.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 5281070.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 5281110.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 5281170.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 5281260.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 5283730.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 5284130.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 5286670.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 5286780.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 5286840.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 5287750.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 5300680.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 5300910.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 5302100.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 5302130.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 5302170.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 5302340.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 5312920.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 5312990.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 5319340.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 5319440.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 5320300.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 5331280.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 5331380.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 5388440.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 5396680.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 5400610.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 5400620.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 5400650.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 5403770.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 5403780.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 5407420.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 5407420.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 5407430.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 5407440.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 5411630.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 5411640.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 5413550.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 5413550.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 5413550.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 5413560.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 5415620.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 5415620.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 5445340.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 5455110.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 5455150.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 5459850.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 5460020.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 5460300.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 5463270.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 5463290.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 5467430.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 5467660.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 5467760.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 5467770.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 5467920.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 5468140.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 5468440.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 5468460.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 5469240.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 5469360.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 5471230.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 5472230.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 5472350.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 5472480.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 5474390.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 5474490.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 5474640.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 5474830.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 5474990.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 5475060.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 5476300.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 5476600.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 5477840.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 5477860.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 5477920.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 5478000.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 5478940.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 5479010.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 5479210.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 5479230.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 5479270.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 5479320.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 5479910.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 5480030.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 5480100.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 5481230.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 5481330.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 5481460.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 5481620.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 5482680.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 5482940.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 5482970.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 5483290.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 5483800.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 5483920.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 5484010.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 5484070.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 5484090.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 5485210.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 5485390.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 5485650.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 5485860.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 5496900.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 5496900.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 5505890.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 5505890.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 5506050.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 5506110.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 5511420.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 5511460.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 5511480.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 5512830.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 5512880.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 5513580.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 5513590.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 5516320.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 5516330.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 5517050.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 5517100.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 5518820.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 5518840.0 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 = 1.27592 2S = 1.01330 2P = 0.89766 3S = 1.00231 3P = 0.89263 3D = 0.81962 4S = 1.00090 4P = 0.89264 4D = 0.82155 4F = 0.88781 5S = 1.00267 5P = 0.89410 5D = 0.82480 5F = 0.79836 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. 70 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 171.6572 Rydbergs (2335.567863 eV) A fine energy mesh of 0.000030 Z**2 Rydbergs (0.0102045 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (3.4015 eV) was used from the last threshold up to 4.060591 Z**2 Rydbergs (1381.21 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (3.4015 eV) was used from first threshold up to 4.060591 Z**2 Rydbergs (1381.21 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: 22/12/10 ------------------------------------------------------------------------ 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 = 1.27895 2S = 1.01594 2P = 0.90207 3S = 1.00463 3P = 0.89456 3D = 0.82496 4S = 1.00474 4P = 0.89563 4D = 0.83075 4F = 0.99000 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 0.000050 Z**2 Rydbergs (0.0170075 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (3.4015 eV) was used from the last threshold up to 4.060591 Z**2 Rydbergs (1381.21 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (3.4015 eV) was used from first threshold up to 4.060591 Z**2 Rydbergs (1381.21 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 0.878234 3 0.883086 4 5.832472 5 6.070070 6 6.071497 7 6.147642 8 6.148107 9 7.770338 10 7.867276 11 7.867859 12 7.899593 13 7.899788 14 7.901393 15 7.901478 16 8.645099 17 8.694217 18 8.694217 19 8.710355 20 8.710437 21 8.711531 22 8.711531 23 8.711622 24 8.711622 26 40.736371 29 41.383371 31 41.690468 34 41.715072 36 42.077756 38 42.219914 40 42.719288 41 46.738249 55 47.427076 90 47.935836 114 49.086675 158 49.668611 166 49.677723 Produced by: Guiyun Liang Date: 03/08/10 ------------------------------------------------------------------------