lilike_lgy10#al10.dat
Resolved Specific Ion Data Collections
- Ion
- Al10+
- Temperature Range
- 2.085 eV → 2.085 x 104 eV
ADF04
- Filename
- lilike_lgy10#al10.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#al10.dat
Download data
- Spontaneous Emission: Al+10(i) → Al+10(j) + hv
- Electron Impact Excitation: Al+10(i) + e → Al+10(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 176869.0 cm-1 |
| 2p1 2P1.5 | 182602.0 cm-1 |
| 3s1 2S0.5 | 2020250.0 cm-1 |
| 3p1 2P0.5 | 2068790.0 cm-1 |
| 3p1 2P1.5 | 2070480.0 cm-1 |
| 3d1 2D1.5 | 2087960.0 cm-1 |
| 3d1 2D2.5 | 2088490.0 cm-1 |
| 4s1 2S0.5 | 2706180.0 cm-1 |
| 4p1 2P0.5 | 2726100.0 cm-1 |
| 4p1 2P1.5 | 2726800.0 cm-1 |
| 4d1 2D1.5 | 2734070.0 cm-1 |
| 4d1 2D2.5 | 2734300.0 cm-1 |
| 4f1 2F2.5 | 2734630.0 cm-1 |
| 4f1 2F3.5 | 2734740.0 cm-1 |
| 5s1 2S0.5 | 3019050.0 cm-1 |
| 5p1 2P0.5 | 3029100.0 cm-1 |
| 5p1 2P1.5 | 3029460.0 cm-1 |
| 5d1 2D1.5 | 3033160.0 cm-1 |
| 5d1 2D2.5 | 3033270.0 cm-1 |
| 5f1 2F2.5 | 3033460.0 cm-1 |
| 5f1 2F3.5 | 3033520.0 cm-1 |
| 5g1 2G3.5 | 3033520.0 cm-1 |
| 5g1 2G4.5 | 3033560.0 cm-1 |
| 1s1 2s2 2S0.5 | 12579600.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 12626100.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 12628100.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 12631600.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 12761400.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 12764000.0 cm-1 |
| 1s1 2p2 4P0.5 | 12814300.0 cm-1 |
| 1s1 2p2 4P1.5 | 12816300.0 cm-1 |
| 1s1 2p2 4P2.5 | 12819600.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 12831800.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 12833200.0 cm-1 |
| 1s1 2p2 2D1.5 | 12905100.0 cm-1 |
| 1s1 2p2 2D2.5 | 12905500.0 cm-1 |
| 1s1 2p2 2P0.5 | 12926900.0 cm-1 |
| 1s1 2p2 2P1.5 | 12931300.0 cm-1 |
| 1s1 2p2 2S0.5 | 13034900.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 14684500.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 14731100.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 14747800.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 14748100.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 14749100.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 14750600.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 14750700.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 14783100.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 14783300.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 14783600.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 14784100.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 14803600.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 14807800.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 14807800.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 14824800.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 14826600.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 14829900.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 14844900.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 14846100.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 14854700.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 14856000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 14858200.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 14861100.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 14862500.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 14862700.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 14877200.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 14878800.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 14883300.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 14889300.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 14890200.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 14890600.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 14891600.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 14892300.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 14893200.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 14893900.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 14894600.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 14894800.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 14898500.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 14899000.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 14907300.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 14911400.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 14917700.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 14918300.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 14919000.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 14919100.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 14919600.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 14920900.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 14926400.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 14929500.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 14930600.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 14930700.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 14931200.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 14935800.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 14955500.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 14957900.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 14961500.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 14961600.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 14961700.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 14963500.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 14986400.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 14987000.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 14994600.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 14998700.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 14999800.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 15017300.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 15018500.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 15418100.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 15433000.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 15440400.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 15440600.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 15440900.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 15446800.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 15446900.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 15455200.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 15455200.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 15455300.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 15455400.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 15462900.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 15463000.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 15466800.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 15466800.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 15466900.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 15466900.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 15469600.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 15469600.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 15525700.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 15536100.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 15537800.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 15541200.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 15542100.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 15543100.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 15550500.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 15551600.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 15553300.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 15553400.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 15556100.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 15556500.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 15556800.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 15556800.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 15560100.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 15560200.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 15560600.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 15560800.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 15562800.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 15563100.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 15564500.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 15565700.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 15567300.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 15568300.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 15568500.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 15569200.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 15569700.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 15570200.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 15570300.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 15572400.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 15573000.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 15573200.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 15573800.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 15575400.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 15575400.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 15575800.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 15576000.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 15576100.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 15576400.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 15576900.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 15578200.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 15579100.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 15579500.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 15579600.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 15580300.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 15581800.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 15582400.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 15583000.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 15583200.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 15584500.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 15584700.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 15585400.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 15585500.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 15585600.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 15586500.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 15587100.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 15587400.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 15587400.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 15588900.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 15589500.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 15615900.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 15615900.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 15632200.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 15632400.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 15632400.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 15633100.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 15642400.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 15644200.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 15644400.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 15646200.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 15646700.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 15648600.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 15648700.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 15653700.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 15653700.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 15653800.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 15654300.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 15657500.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 15657700.0 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 = 1.27978 2S = 1.03249 2P = 0.92744 3S = 1.02000 3P = 0.92086 3D = 0.85314 4S = 1.01892 4P = 0.92074 4D = 0.85522 4F = 0.97734 5S = 1.02000 5P = 0.92235 5D = 0.85853 5F = 0.83986 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. 63 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 465.0428 Rydbergs (6327.372337 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.0054424 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (13.606 eV) was used from the last threshold up to 3.462443 Z**2 Rydbergs (4711 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (13.606 eV) was used from first threshold up to 3.462443 Z**2 Rydbergs (4711 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: 14/10/10 ------------------------------------------------------------------------ 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 = 1.28409 2S = 1.03471 2P = 0.93056 3S = 1.02338 3P = 0.92275 3D = 0.85706 4S = 1.02271 4P = 0.92366 4D = 0.86230 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 0.000010 Z**2 Rydbergs (0.013606 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (13.606 eV) was used from the last threshold up to 3.462443 Z**2 Rydbergs (4711 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (13.606 eV) was used from first threshold up to 3.462443 Z**2 Rydbergs (4711 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 1.60400 3 1.65676 4 18.4117 5 18.8520 6 18.8680 7 19.028 8 19.0321 9 24.656 10 24.8422 11 24.8494 12 24.9150 13 24.9181 14 24.9220 15 24.923 16 27.518 17 27.609 18 27.609 19 27.6420 20 27.6430 21 27.645 22 27.6457 25 114.450 26 114.8672 27 114.8814 28 114.9169 29 116.101 30 116.130 31 116.5737 32 116.5974 33 116.6239 34 116.681 35 116.695 36 117.368 37 117.358 38 117.569 39 117.619 40 118.491 46 134.155 47 134.155 53 134.743 54 134.743 58 135.133 59 135.133 64 135.146 65 135.146 75 135.560 80 135.563 81 135.602 82 135.659 83 135.669 93 135.843 96 136.089 97 136.085 99 136.110 Produced by: Guiyun Liang Date: 25/11/10 ------------------------------------------------------------------------