Resolved Specific Ion Data Collections

Temperature Range
6.893 eV → 6.893 x 104 eV


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  • 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

        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

     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

      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



  • Mike Witthoeft
  • Allan Whiteford
  • Nigel Badnell
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