flike_mcw06#ni19.dat
Resolved Specific Ion Data Collections
- Ion
- Ni19+
- Temperature Range
- 6.893 eV → 6.893 x 104 eV
ADF04
- Filename
- flike_mcw06#ni19.dat
- Full Path
- adf04/copaw#f/flike_mcw06#ni19.dat
Download data
- Spontaneous Emission: Ni+19(i) → Ni+19(j) + hv
- Electron Impact Excitation: Ni+19(i) + e → Ni+19(j) + e
| 2s2 2p5 2P1.5 | 0.0 cm-1 |
| 2s2 2p5 2P0.5 | 146547.0 cm-1 |
| 2s1 2p6 2S0.5 | 1215330.0 cm-1 |
| 2s2 2p4 3s1 4P2.5 | 7532520.0 cm-1 |
| 2s2 2p4 3s1 2P1.5 | 7563300.0 cm-1 |
| 2s2 2p4 3s1 4P0.5 | 7636000.0 cm-1 |
| 2s2 2p4 3s1 4P1.5 | 7664250.0 cm-1 |
| 2s2 2p4 3s1 2P0.5 | 7692040.0 cm-1 |
| 2s2 2p4 3s1 2D2.5 | 7756080.0 cm-1 |
| 2s2 2p4 3s1 2D1.5 | 7761380.0 cm-1 |
| 2s2 2p4 3p1 4P1.5 | 7804850.0 cm-1 |
| 2s2 2p4 3p1 4P2.5 | 7811810.0 cm-1 |
| 2s2 2p4 3p1 2P0.5 | 7845330.0 cm-1 |
| 2s2 2p4 3p1 2D2.5 | 7850080.0 cm-1 |
| 2s2 2p4 3p1 4D3.5 | 7850870.0 cm-1 |
| 2s2 2p4 3p1 4D0.5 | 7919290.0 cm-1 |
| 2s2 2p4 3p1 4S1.5 | 7920430.0 cm-1 |
| 2s2 2p4 3p1 4P0.5 | 7928980.0 cm-1 |
| 2s2 2p4 3p1 4D1.5 | 7944190.0 cm-1 |
| 2s2 2p4 3p1 2P1.5 | 7969690.0 cm-1 |
| 2s2 2p4 3p1 4D2.5 | 7972170.0 cm-1 |
| 2s2 2p4 3s1 2S0.5 | 7973390.0 cm-1 |
| 2s2 2p4 3p1 2S0.5 | 7994100.0 cm-1 |
| 2s2 2p4 3p1 2D1.5 | 7999340.0 cm-1 |
| 2s2 2p4 3p1 2F2.5 | 8031400.0 cm-1 |
| 2s2 2p4 3p1 2F3.5 | 8061240.0 cm-1 |
| 2s2 2p4 3p1 2D1.5 | 8074230.0 cm-1 |
| 2s2 2p4 3p1 2D2.5 | 8090320.0 cm-1 |
| 2s2 2p4 3p1 2P1.5 | 8137680.0 cm-1 |
| 2s2 2p4 3p1 2P0.5 | 8177500.0 cm-1 |
| 2s2 2p4 3d1 4D2.5 | 8189270.0 cm-1 |
| 2s2 2p4 3d1 4D3.5 | 8192410.0 cm-1 |
| 2s2 2p4 3d1 4D1.5 | 8193690.0 cm-1 |
| 2s2 2p4 3d1 2P0.5 | 8204590.0 cm-1 |
| 2s2 2p4 3d1 4F4.5 | 8218670.0 cm-1 |
| 2s2 2p4 3d1 2F3.5 | 8228580.0 cm-1 |
| 2s2 2p4 3d1 4P0.5 | 8248820.0 cm-1 |
| 2s2 2p4 3d1 4P1.5 | 8268800.0 cm-1 |
| 2s2 2p4 3d1 2F2.5 | 8281420.0 cm-1 |
| 2s2 2p4 3p1 2P1.5 | 8288970.0 cm-1 |
| 2s2 2p4 3p1 2P0.5 | 8300480.0 cm-1 |
| 2s2 2p4 3d1 4F1.5 | 8312720.0 cm-1 |
| 2s2 2p4 3d1 4D0.5 | 8313930.0 cm-1 |
| 2s2 2p4 3d1 4F2.5 | 8318030.0 cm-1 |
| 2s2 2p4 3d1 4F3.5 | 8337320.0 cm-1 |
| 2s2 2p4 3d1 2D1.5 | 8337770.0 cm-1 |
| 2s2 2p4 3d1 4P2.5 | 8360680.0 cm-1 |
| 2s2 2p4 3d1 2P1.5 | 8374830.0 cm-1 |
| 2s2 2p4 3d1 2D2.5 | 8384030.0 cm-1 |
| 2s2 2p4 3d1 2G3.5 | 8416050.0 cm-1 |
| 2s2 2p4 3d1 2G4.5 | 8422510.0 cm-1 |
| 2s2 2p4 3d1 2F2.5 | 8446750.0 cm-1 |
| 2s2 2p4 3d1 2S0.5 | 8448470.0 cm-1 |
| 2s2 2p4 3d1 2F3.5 | 8461590.0 cm-1 |
| 2s2 2p4 3d1 2P1.5 | 8474840.0 cm-1 |
| 2s2 2p4 3d1 2D2.5 | 8482260.0 cm-1 |
| 2s2 2p4 3d1 2D1.5 | 8514200.0 cm-1 |
| 2s2 2p4 3d1 2P0.5 | 8523240.0 cm-1 |
| 2s1 2p5 3s1 4P2.5 | 8595940.0 cm-1 |
| 2s1 2p5 3s1 4P1.5 | 8639450.0 cm-1 |
| 2s2 2p4 3d1 2D2.5 | 8658710.0 cm-1 |
| 2s2 2p4 3d1 2D1.5 | 8680720.0 cm-1 |
| 2s1 2p5 3s1 4P0.5 | 8703730.0 cm-1 |
| 2s1 2p5 3s1 2P1.5 | 8706980.0 cm-1 |
| 2s1 2p5 3s1 2P0.5 | 8780300.0 cm-1 |
| 2s1 2p5 3p1 4S1.5 | 8857810.0 cm-1 |
| 2s1 2p5 3p1 4D2.5 | 8887230.0 cm-1 |
| 2s1 2p5 3p1 4D3.5 | 8902530.0 cm-1 |
| 2s1 2p5 3p1 4D1.5 | 8920520.0 cm-1 |
| 2s1 2p5 3p1 2D2.5 | 8934640.0 cm-1 |
| 2s1 2p5 3p1 4P0.5 | 8955950.0 cm-1 |
| 2s1 2p5 3p1 2P1.5 | 8971670.0 cm-1 |
| 2s1 2p5 3p1 2P0.5 | 8993610.0 cm-1 |
| 2s1 2p5 3p1 4P2.5 | 9000270.0 cm-1 |
| 2s1 2p5 3p1 2D1.5 | 9004610.0 cm-1 |
| 2s1 2p5 3p1 4D0.5 | 9016880.0 cm-1 |
| 2s1 2p5 3s1 2P1.5 | 9018130.0 cm-1 |
| 2s1 2p5 3s1 2P0.5 | 9027610.0 cm-1 |
| 2s1 2p5 3p1 4P1.5 | 9069920.0 cm-1 |
| 2s1 2p5 3p1 2S0.5 | 9095460.0 cm-1 |
| 2s1 2p5 3d1 4P0.5 | 9224050.0 cm-1 |
| 2s1 2p5 3d1 4P1.5 | 9235970.0 cm-1 |
| 2s1 2p5 3d1 4F4.5 | 9247860.0 cm-1 |
| 2s1 2p5 3d1 4P2.5 | 9254830.0 cm-1 |
| 2s1 2p5 3d1 4F3.5 | 9258340.0 cm-1 |
| 2s1 2p5 3d1 4F2.5 | 9285010.0 cm-1 |
| 2s1 2p5 3p1 2D1.5 | 9286760.0 cm-1 |
| 2s1 2p5 3d1 2F3.5 | 9299560.0 cm-1 |
| 2s1 2p5 3d1 4D1.5 | 9306460.0 cm-1 |
| 2s1 2p5 3p1 2D2.5 | 9318680.0 cm-1 |
| 2s1 2p5 3p1 2P0.5 | 9321280.0 cm-1 |
| 2s1 2p5 3p1 2P1.5 | 9334890.0 cm-1 |
| 2s1 2p5 3d1 4D0.5 | 9342350.0 cm-1 |
| 2s1 2p5 3d1 2D2.5 | 9359320.0 cm-1 |
| 2s1 2p5 3d1 4D2.5 | 9362370.0 cm-1 |
| 2s1 2p5 3d1 4D3.5 | 9363280.0 cm-1 |
| 2s1 2p5 3d1 2D1.5 | 9371760.0 cm-1 |
| 2s1 2p5 3p1 2S0.5 | 9375170.0 cm-1 |
| 2s1 2p5 3d1 4F1.5 | 9379490.0 cm-1 |
| 2s1 2p5 3d1 2P0.5 | 9398520.0 cm-1 |
| 2s1 2p5 3d1 2F2.5 | 9433230.0 cm-1 |
| 2s1 2p5 3d1 2P1.5 | 9481130.0 cm-1 |
| 2s1 2p5 3d1 2F2.5 | 9665720.0 cm-1 |
| 2s1 2p5 3d1 2F3.5 | 9669890.0 cm-1 |
| 2s1 2p5 3d1 2P1.5 | 9691820.0 cm-1 |
| 2s1 2p5 3d1 2D2.5 | 9700070.0 cm-1 |
| 2s1 2p5 3d1 2D1.5 | 9701440.0 cm-1 |
| 2s1 2p5 3d1 2P0.5 | 9705840.0 cm-1 |
| 2s2 2p4 4s1 4P2.5 | 10198400.0 cm-1 |
| 2s2 2p4 4s1 2P1.5 | 10208000.0 cm-1 |
| 2s2 2p4 4s1 4P0.5 | 10299000.0 cm-1 |
| 2s2 2p4 4p1 4P1.5 | 10311700.0 cm-1 |
| 2s2 2p4 4p1 4P2.5 | 10312700.0 cm-1 |
| 2s2 2p4 4s1 4P1.5 | 10324300.0 cm-1 |
| 2s2 2p4 4p1 4D3.5 | 10325300.0 cm-1 |
| 2s2 2p4 4p1 2D2.5 | 10325700.0 cm-1 |
| 2s2 2p4 4p1 2S0.5 | 10329800.0 cm-1 |
| 2s2 2p4 4s1 2P0.5 | 10331800.0 cm-1 |
| 2s2 2p4 4p1 2P1.5 | 10359000.0 cm-1 |
| 2s2 2p4 4p1 4D0.5 | 10411700.0 cm-1 |
| 2s2 2p4 4s1 2D2.5 | 10413500.0 cm-1 |
| 2s2 2p4 4s1 2D1.5 | 10415200.0 cm-1 |
| 2s2 2p4 4p1 4D1.5 | 10425700.0 cm-1 |
| 2s2 2p4 4p1 4P0.5 | 10434200.0 cm-1 |
| 2s2 2p4 4p1 4D2.5 | 10448800.0 cm-1 |
| 2s2 2p4 4p1 4S1.5 | 10450400.0 cm-1 |
| 2s2 2p4 4d1 4D2.5 | 10453800.0 cm-1 |
| 2s2 2p4 4d1 4D3.5 | 10454400.0 cm-1 |
| 2s2 2p4 4d1 4D1.5 | 10455600.0 cm-1 |
| 2s2 2p4 4p1 2D1.5 | 10456500.0 cm-1 |
| 2s2 2p4 4d1 4P0.5 | 10459500.0 cm-1 |
| 2s2 2p4 4d1 4F4.5 | 10461700.0 cm-1 |
| 2s2 2p4 4p1 2P0.5 | 10464200.0 cm-1 |
| 2s2 2p4 4d1 2F3.5 | 10465500.0 cm-1 |
| 2s2 2p4 4d1 2P0.5 | 10476300.0 cm-1 |
| 2s2 2p4 4d1 2D1.5 | 10488200.0 cm-1 |
| 2s2 2p4 4d1 2F2.5 | 10491500.0 cm-1 |
| 2s2 2p4 4p1 2F2.5 | 10525200.0 cm-1 |
| 2s2 2p4 4f1 4F3.5 | 10533000.0 cm-1 |
| 2s2 2p4 4f1 4F4.5 | 10533700.0 cm-1 |
| 2s2 2p4 4f1 4F2.5 | 10533800.0 cm-1 |
| 2s2 2p4 4f1 4D1.5 | 10535900.0 cm-1 |
| 2s2 2p4 4f1 2G4.5 | 10535900.0 cm-1 |
| 2s2 2p4 4f1 4G5.5 | 10536500.0 cm-1 |
| 2s2 2p4 4f1 2F3.5 | 10536700.0 cm-1 |
| 2s2 2p4 4p1 2F3.5 | 10537200.0 cm-1 |
| 2s2 2p4 4f1 4D0.5 | 10538600.0 cm-1 |
| 2s2 2p4 4f1 2F2.5 | 10539300.0 cm-1 |
| 2s2 2p4 4p1 2P1.5 | 10540100.0 cm-1 |
| 2s2 2p4 4f1 2D1.5 | 10541100.0 cm-1 |
| 2s2 2p4 4p1 2D1.5 | 10545900.0 cm-1 |
| 2s2 2p4 4p1 2D2.5 | 10546300.0 cm-1 |
| 2s2 2p4 4d1 4F1.5 | 10558100.0 cm-1 |
| 2s2 2p4 4d1 4F2.5 | 10563000.0 cm-1 |
| 2s2 2p4 4p1 2P0.5 | 10571600.0 cm-1 |
| 2s2 2p4 4d1 4D0.5 | 10577900.0 cm-1 |
| 2s2 2p4 4d1 4F3.5 | 10583900.0 cm-1 |
| 2s2 2p4 4d1 4P1.5 | 10586500.0 cm-1 |
| 2s2 2p4 4d1 4P2.5 | 10592400.0 cm-1 |
| 2s2 2p4 4d1 2D2.5 | 10600400.0 cm-1 |
| 2s2 2p4 4d1 2P1.5 | 10606500.0 cm-1 |
| 2s2 2p4 4s1 2S0.5 | 10629600.0 cm-1 |
| 2s2 2p4 4f1 4G2.5 | 10632800.0 cm-1 |
| 2s2 2p4 4f1 2G3.5 | 10634600.0 cm-1 |
| 2s2 2p4 4f1 4F1.5 | 10657200.0 cm-1 |
| 2s2 2p4 4f1 4G3.5 | 10658700.0 cm-1 |
| 2s2 2p4 4f1 4G4.5 | 10659100.0 cm-1 |
| 2s2 2p4 4f1 4D2.5 | 10659600.0 cm-1 |
| 2s2 2p4 4f1 2D2.5 | 10662900.0 cm-1 |
| 2s2 2p4 4f1 4D3.5 | 10663500.0 cm-1 |
| 2s2 2p4 4d1 2G3.5 | 10668200.0 cm-1 |
| 2s2 2p4 4d1 2G4.5 | 10671100.0 cm-1 |
| 2s2 2p4 4d1 2D2.5 | 10679400.0 cm-1 |
| 2s2 2p4 4d1 2S0.5 | 10681000.0 cm-1 |
| 2s2 2p4 4d1 2P1.5 | 10682800.0 cm-1 |
| 2s2 2p4 4d1 2F3.5 | 10684100.0 cm-1 |
| 2s2 2p4 4d1 2F2.5 | 10686100.0 cm-1 |
| 2s2 2p4 4d1 2D1.5 | 10699100.0 cm-1 |
| 2s2 2p4 4d1 2P0.5 | 10704300.0 cm-1 |
| 2s2 2p4 4f1 2H4.5 | 10742900.0 cm-1 |
| 2s2 2p4 4f1 2P0.5 | 10742900.0 cm-1 |
| 2s2 2p4 4f1 2P1.5 | 10744300.0 cm-1 |
| 2s2 2p4 4f1 2H5.5 | 10744400.0 cm-1 |
| 2s2 2p4 4f1 2D2.5 | 10748400.0 cm-1 |
| 2s2 2p4 4f1 2D1.5 | 10748600.0 cm-1 |
| 2s2 2p4 4f1 2G3.5 | 10751300.0 cm-1 |
| 2s2 2p4 4f1 2F2.5 | 10752000.0 cm-1 |
| 2s2 2p4 4f1 2F3.5 | 10752400.0 cm-1 |
| 2s2 2p4 4f1 2G4.5 | 10752900.0 cm-1 |
| 2s2 2p4 4p1 2P0.5 | 10753100.0 cm-1 |
| 2s2 2p4 4p1 2P1.5 | 10757200.0 cm-1 |
| 2s2 2p4 4d1 2D2.5 | 10893800.0 cm-1 |
| 2s2 2p4 4d1 2D1.5 | 10899700.0 cm-1 |
| 2s2 2p4 4f1 2F2.5 | 10964100.0 cm-1 |
| 2s2 2p4 4f1 2F3.5 | 10965300.0 cm-1 |
Contributors
- Mike Witthoeft
- Allan Whiteford
- Nigel Badnell
------------------------------------------------------------------------ Result of ICFT R-matrix calculation +++++++++++++++++++++++++++++++++++ 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 = 1.4118 2S = 1.2094 2P = 1.1461 3S = 1.1330 3P = 1.0831 3D = 1.1175 4S = 1.1493 4P = 1.0955 4D = 1.1195 4F = 1.1283 An exchange calculation was performed up to J=12 A non-exchange calculation was then performed up to J=40 Followed by a top-up calculation to J -> infinity. 30 continuum basis orbitals were used. A fine energy mesh of 0.000005 Z**2 Rydbergs (0.02455883 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.001000 Z**2 Rydbergs (4.911766 eV) was used from the last threshold up to 0.943652 Z**2 Rydbergs (4635 eV) in the excitation calculation. A coarse energy mesh of 0.001000 Z**2 Rydbergs (4.911766 eV) was used from first threshold up to 0.943652 Z**2 Rydbergs (4635 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 See: M C Witthoeft, A D Whiteford and N R Badnell J Phys B 40 2969-2993 (2007) DOI: 10.1088/0953-4075/40/15/001 Produced by: Mike Witthoeft Date: 18/07/06 Update: Allan Whiteford, 14/03/08 Added Journal reference Removed incomplete comment about basis orbitals Added parent specification ------------------------------------------------------------------------