Resolved Specific Ion Data Collections

Temperature Range
9.909 eV → 9.909 x 104 eV


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  • Spontaneous Emission: Ni+23(i) → Ni+23(j) + hv
  • Electron Impact Excitation: Ni+23(i) + e → Ni+23(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 161108.0 cm-1
2s1 2p2 4P0.5 449094.0 cm-1
2s1 2p2 4P1.5 529658.0 cm-1
2s1 2p2 4P2.5 602797.0 cm-1
2s1 2p2 2D1.5 842645.0 cm-1
2s1 2p2 2D2.5 882634.0 cm-1
2s1 2p2 2P0.5 955538.0 cm-1
2s1 2p2 2S0.5 1126630.0 cm-1
2s1 2p2 2P1.5 1143280.0 cm-1
2p3 4S1.5 1416650.0 cm-1
2p3 2D1.5 1578650.0 cm-1
2p3 2D2.5 1627210.0 cm-1
2p3 2P0.5 1780420.0 cm-1
2p3 2P1.5 1871910.0 cm-1
2s2 3s1 2S0.5 9627520.0 cm-1
2s2 3p1 2P0.5 9825310.0 cm-1
2s2 3p1 2P1.5 9870140.0 cm-1
2s1 2p1 3s1 4P0.5 10018400.0 cm-1
2s2 3d1 2D1.5 10053400.0 cm-1
2s1 2p1 3s1 4P1.5 10058100.0 cm-1
2s2 3d1 2D2.5 10067900.0 cm-1
2s1 2p1 3s1 2P0.5 10129100.0 cm-1
2s1 2p1 3s1 4P2.5 10172400.0 cm-1
2s1 2p1 3p1 4D0.5 10193000.0 cm-1
2s1 2p1 3p1 4D1.5 10228700.0 cm-1
2s1 2p1 3s1 2P1.5 10250500.0 cm-1
2s1 2p1 3p1 2P1.5 10272300.0 cm-1
2s1 2p1 3p1 2P0.5 10289200.0 cm-1
2s1 2p1 3p1 4D2.5 10294000.0 cm-1
2s1 2p1 3p1 4P0.5 10304100.0 cm-1
2s1 2p1 3p1 2D1.5 10334400.0 cm-1
2s1 2p1 3p1 4P1.5 10393300.0 cm-1
2s1 2p1 3p1 4D3.5 10397800.0 cm-1
2s1 2p1 3d1 4F1.5 10402500.0 cm-1
2s1 2p1 3p1 4P2.5 10413000.0 cm-1
2s1 2p1 3p1 4S1.5 10422900.0 cm-1
2s1 2p1 3d1 4F2.5 10428500.0 cm-1
2s1 2p1 3d1 4F3.5 10469500.0 cm-1
2s1 2p1 3d1 4P2.5 10474600.0 cm-1
2s1 2p1 3p1 2D2.5 10474800.0 cm-1
2s1 2p1 3d1 4D1.5 10487300.0 cm-1
2s1 2p1 3d1 4D0.5 10491200.0 cm-1
2s1 2p1 3s1 2P0.5 10494600.0 cm-1
2s1 2p1 3s1 2P1.5 10497000.0 cm-1
2s1 2p1 3p1 2S0.5 10504700.0 cm-1
2s1 2p1 3d1 2D1.5 10533400.0 cm-1
2s1 2p1 3d1 2D2.5 10550800.0 cm-1
2s1 2p1 3d1 4F4.5 10562700.0 cm-1
2s1 2p1 3d1 4D3.5 10594000.0 cm-1
2s1 2p1 3d1 4D2.5 10603100.0 cm-1
2s1 2p1 3d1 4P1.5 10609300.0 cm-1
2s1 2p1 3d1 4P0.5 10611300.0 cm-1
2s1 2p1 3d1 2F2.5 10644500.0 cm-1
2s1 2p1 3d1 2P1.5 10685400.0 cm-1
2s1 2p1 3p1 2P0.5 10690200.0 cm-1
2s1 2p1 3p1 2D1.5 10698800.0 cm-1
2s1 2p1 3d1 2F3.5 10711600.0 cm-1
2s1 2p1 3p1 2D2.5 10727300.0 cm-1
2s1 2p1 3d1 2P0.5 10728600.0 cm-1
2p2 3s1 4P0.5 10732600.0 cm-1
2s1 2p1 3p1 2P1.5 10738900.0 cm-1
2s1 2p1 3p1 2S0.5 10788200.0 cm-1
2p2 3s1 4P1.5 10828900.0 cm-1
2p2 3s1 4P2.5 10887000.0 cm-1
2p2 3p1 4D0.5 10893800.0 cm-1
2p2 3s1 2P0.5 10894500.0 cm-1
2s1 2p1 3d1 2F3.5 10910600.0 cm-1
2s1 2p1 3d1 2F2.5 10911600.0 cm-1
2s1 2p1 3d1 2D1.5 10922000.0 cm-1
2s1 2p1 3d1 2D2.5 10940500.0 cm-1
2p2 3s1 2P1.5 10942400.0 cm-1
2p2 3p1 4D1.5 10953700.0 cm-1
2s1 2p1 3d1 2P0.5 10958700.0 cm-1
2s1 2p1 3d1 2P1.5 10976100.0 cm-1
2p2 3p1 2S0.5 10980600.0 cm-1
2p2 3p1 4P1.5 11017900.0 cm-1
2p2 3p1 4D2.5 11037900.0 cm-1
2p2 3p1 4P0.5 11057000.0 cm-1
2p2 3p1 4P2.5 11057700.0 cm-1
2p2 3s1 2D2.5 11063400.0 cm-1
2p2 3p1 2D1.5 11079700.0 cm-1
2p2 3s1 2D1.5 11087400.0 cm-1
2p2 3p1 4D3.5 11096800.0 cm-1
2p2 3d1 4F1.5 11101400.0 cm-1
2p2 3d1 4F2.5 11135300.0 cm-1
2p2 3p1 4S1.5 11141400.0 cm-1
2p2 3p1 2P1.5 11153100.0 cm-1
2p2 3p1 2D2.5 11160400.0 cm-1
2p2 3p1 2P0.5 11200200.0 cm-1
2p2 3d1 2P1.5 11201300.0 cm-1
2p2 3d1 4F3.5 11205400.0 cm-1
2p2 3d1 4D2.5 11209400.0 cm-1
2p2 3d1 4D0.5 11210000.0 cm-1
2p2 3d1 4D3.5 11246200.0 cm-1
2p2 3d1 4D1.5 11251200.0 cm-1
2p2 3d1 2F2.5 11253200.0 cm-1
2p2 3d1 4F4.5 11255600.0 cm-1
2p2 3p1 2F2.5 11257700.0 cm-1
2p2 3p1 2F3.5 11274200.0 cm-1
2p2 3p1 2D1.5 11283800.0 cm-1
2p2 3s1 2S0.5 11295000.0 cm-1
2p2 3d1 4P2.5 11302800.0 cm-1
2p2 3p1 2D2.5 11304600.0 cm-1
2p2 3p1 2P0.5 11314800.0 cm-1
2p2 3d1 4P1.5 11318100.0 cm-1
2p2 3d1 4P0.5 11328000.0 cm-1
2p2 3d1 2P0.5 11335900.0 cm-1
2p2 3d1 2G3.5 11341700.0 cm-1
2p2 3d1 2D2.5 11375100.0 cm-1
2p2 3d1 2D1.5 11377600.0 cm-1
2p2 3p1 2P1.5 11409000.0 cm-1
2p2 3d1 2F3.5 11417900.0 cm-1
2p2 3d1 2G4.5 11438500.0 cm-1
2p2 3d1 2D1.5 11463900.0 cm-1
2p2 3d1 2D2.5 11469700.0 cm-1
2p2 3d1 2P0.5 11488600.0 cm-1
2p2 3d1 2F3.5 11498400.0 cm-1
2p2 3p1 2P0.5 11503600.0 cm-1
2p2 3p1 2P1.5 11531700.0 cm-1
2p2 3d1 2S0.5 11537100.0 cm-1
2p2 3d1 2P1.5 11546800.0 cm-1
2p2 3d1 2F2.5 11546900.0 cm-1
2p2 3d1 2D2.5 11704300.0 cm-1
2p2 3d1 2D1.5 11712800.0 cm-1
2s2 4s1 2S0.5 13047400.0 cm-1
2s2 4p1 2P0.5 13129200.0 cm-1
2s2 4p1 2P1.5 13147600.0 cm-1
2s2 4d1 2D1.5 13215200.0 cm-1
2s2 4d1 2D2.5 13221100.0 cm-1
2s2 4f1 2F2.5 13260700.0 cm-1
2s2 4f1 2F3.5 13263600.0 cm-1
2s1 2p1 4s1 4P0.5 13432000.0 cm-1
2s1 2p1 4s1 4P1.5 13469100.0 cm-1
2s1 2p1 4s1 2P0.5 13490400.0 cm-1
2s1 2p1 4p1 4D0.5 13504900.0 cm-1
2s1 2p1 4p1 4D1.5 13530700.0 cm-1
2s1 2p1 4p1 4S1.5 13544900.0 cm-1
2s1 2p1 4p1 4P0.5 13564300.0 cm-1
2s1 2p1 4p1 4D2.5 13568500.0 cm-1
2s1 2p1 4p1 2P0.5 13571200.0 cm-1
2s1 2p1 4p1 2D1.5 13581600.0 cm-1
2s1 2p1 4s1 4P2.5 13585600.0 cm-1
2s1 2p1 4d1 4F1.5 13587500.0 cm-1
2s1 2p1 4d1 4F2.5 13602400.0 cm-1
2s1 2p1 4s1 2P1.5 13612400.0 cm-1
2s1 2p1 4d1 4P2.5 13628100.0 cm-1
2s1 2p1 4d1 4F3.5 13636800.0 cm-1
2s1 2p1 4d1 4D1.5 13636800.0 cm-1
2s1 2p1 4f1 4G2.5 13638100.0 cm-1
2s1 2p1 4d1 4D0.5 13640200.0 cm-1
2s1 2p1 4f1 4D3.5 13641500.0 cm-1
2s1 2p1 4d1 2D1.5 13654700.0 cm-1
2s1 2p1 4d1 2F2.5 13662000.0 cm-1
2s1 2p1 4p1 4P1.5 13674300.0 cm-1
2s1 2p1 4f1 4F1.5 13675700.0 cm-1
2s1 2p1 4f1 4G3.5 13677200.0 cm-1
2s1 2p1 4f1 2F2.5 13677800.0 cm-1
2s1 2p1 4p1 4P2.5 13678700.0 cm-1
2s1 2p1 4f1 4G4.5 13678900.0 cm-1
2s1 2p1 4p1 4D3.5 13680000.0 cm-1
2s1 2p1 4f1 2D2.5 13684400.0 cm-1
2s1 2p1 4f1 2G3.5 13686000.0 cm-1
2s1 2p1 4p1 2P1.5 13690100.0 cm-1
2s1 2p1 4p1 2D2.5 13707500.0 cm-1
2s1 2p1 4p1 2S0.5 13719100.0 cm-1
2s1 2p1 4d1 4F4.5 13745400.0 cm-1
2s1 2p1 4d1 4D3.5 13752800.0 cm-1
2s1 2p1 4d1 4D2.5 13755400.0 cm-1
2s1 2p1 4d1 4P1.5 13758700.0 cm-1
2s1 2p1 4d1 4P0.5 13759900.0 cm-1
2s1 2p1 4d1 2D2.5 13770200.0 cm-1
2s1 2p1 4d1 2P1.5 13781800.0 cm-1
2s1 2p1 4d1 2F3.5 13792000.0 cm-1
2s1 2p1 4f1 4F3.5 13796400.0 cm-1
2s1 2p1 4f1 4F4.5 13797300.0 cm-1
2s1 2p1 4d1 2P0.5 13798600.0 cm-1
2s1 2p1 4f1 4F2.5 13798600.0 cm-1
2s1 2p1 4f1 2F3.5 13802000.0 cm-1
2s1 2p1 4f1 4G5.5 13802400.0 cm-1
2s1 2p1 4f1 4D1.5 13803000.0 cm-1
2s1 2p1 4f1 4D0.5 13806200.0 cm-1
2s1 2p1 4f1 2G4.5 13806900.0 cm-1
2s1 2p1 4f1 4D2.5 13807200.0 cm-1
2s1 2p1 4f1 2D1.5 13813900.0 cm-1
2s1 2p1 4s1 2P0.5 13899100.0 cm-1
2s1 2p1 4s1 2P1.5 13901200.0 cm-1
2s1 2p1 4p1 2D1.5 13979300.0 cm-1
2s1 2p1 4p1 2P0.5 13980600.0 cm-1
2s1 2p1 4p1 2D2.5 13992600.0 cm-1
2s1 2p1 4p1 2P1.5 13999200.0 cm-1
2s1 2p1 4p1 2S0.5 14008500.0 cm-1
2s1 2p1 4d1 2D1.5 14062500.0 cm-1
2s1 2p1 4d1 2F2.5 14063600.0 cm-1
2s1 2p1 4d1 2F3.5 14064600.0 cm-1
2s1 2p1 4d1 2D2.5 14070000.0 cm-1
2s1 2p1 4d1 2P0.5 14077400.0 cm-1
2s1 2p1 4d1 2P1.5 14083300.0 cm-1
2s1 2p1 4f1 2F2.5 14097400.0 cm-1
2s1 2p1 4f1 2F3.5 14100200.0 cm-1
2s1 2p1 4f1 2G3.5 14108500.0 cm-1
2s1 2p1 4f1 2G4.5 14111100.0 cm-1
2s1 2p1 4f1 2D1.5 14115200.0 cm-1
2s1 2p1 4f1 2D2.5 14117800.0 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 = 1.37839
         2S = 1.25204
         2P = 1.17552
         3S = 1.57908
         3P = 1.37485
         3D = 1.48746
         4S = 1.50382
         4P = 1.38573
         4D = 1.53800
         4F = 1.58859

 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.

 40 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 1866.1474 Rydbergs (25390.801524 eV)

 A fine energy mesh of 0.000002 Z**2 Rydbergs (0.014395148 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (7.197574 eV) was used
 from the last threshold up to 0.862374 Z**2 Rydbergs (6207 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (7.197574 eV) was used
 from first threshold up to 0.862374 Z**2 Rydbergs (6207 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

      G Y Liang, N R Badnell and G Zhao
      A&A 547, A87 (2012)
      DOI: 10.1051/0004-6361/201220277

 Produced by: Guiyun Liang
 Date:        09/04/12

 Those data points with same collision strength in OMEGAU at higher energies
 are deleted. The adf04 file is generated based upon this correction.

 Date:  Tue May 28 23:01:42 2013


  • Guiyun Liang
  • Nigel Badnell
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