Resolved Specific Ion Data Collections

Temperature Range
11.63 eV → 1.163 x 105 eV


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  • Spontaneous Emission: Se+25(i) → Se+25(j) + hv
  • Electron Impact Excitation: Se+25(i) + e → Se+25(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 347266.0 cm-1
2s1 2p6 2S0.5 1705080.0 cm-1
2s2 2p4 3s1 4P2.5 12160900.0 cm-1
2s2 2p4 3s1 2P1.5 12198800.0 cm-1
2s2 2p4 3s1 4P0.5 12326600.0 cm-1
2s2 2p4 3s1 4P1.5 12477600.0 cm-1
2s2 2p4 3s1 2P0.5 12508300.0 cm-1
2s2 2p4 3p1 4P1.5 12518400.0 cm-1
2s2 2p4 3p1 4P2.5 12534700.0 cm-1
2s2 2p4 3s1 2D2.5 12586500.0 cm-1
2s2 2p4 3s1 2D1.5 12597100.0 cm-1
2s2 2p4 3p1 2P0.5 12603600.0 cm-1
2s2 2p4 3p1 2D2.5 12609200.0 cm-1
2s2 2p4 3p1 4D3.5 12615500.0 cm-1
2s2 2p4 3p1 4D0.5 12696100.0 cm-1
2s2 2p4 3p1 4S1.5 12729900.0 cm-1
2s2 2p4 3p1 4D1.5 12783400.0 cm-1
2s2 2p4 3p1 4P0.5 12825900.0 cm-1
2s2 2p4 3p1 2P1.5 12868300.0 cm-1
2s2 2p4 3p1 4D2.5 12920100.0 cm-1
2s2 2p4 3p1 2S0.5 12945800.0 cm-1
2s2 2p4 3p1 2F2.5 12948400.0 cm-1
2s2 2p4 3p1 2D1.5 12950100.0 cm-1
2s2 2p4 3s1 2S0.5 12991400.0 cm-1
2s2 2p4 3p1 2F3.5 13027800.0 cm-1
2s2 2p4 3p1 2D1.5 13032700.0 cm-1
2s2 2p4 3d1 4D2.5 13059500.0 cm-1
2s2 2p4 3d1 4D1.5 13060600.0 cm-1
2s2 2p4 3p1 2D2.5 13061800.0 cm-1
2s2 2p4 3d1 4D3.5 13071400.0 cm-1
2s2 2p4 3p1 2P1.5 13073500.0 cm-1
2s2 2p4 3d1 2P0.5 13075000.0 cm-1
2s2 2p4 3d1 4F4.5 13101200.0 cm-1
2s2 2p4 3d1 2F3.5 13105100.0 cm-1
2s2 2p4 3d1 4P0.5 13143100.0 cm-1
2s2 2p4 3d1 4P1.5 13174700.0 cm-1
2s2 2p4 3p1 2P0.5 13179600.0 cm-1
2s2 2p4 3d1 2D2.5 13200400.0 cm-1
2s2 2p4 3d1 4F1.5 13252400.0 cm-1
2s2 2p4 3d1 4F2.5 13277800.0 cm-1
2s2 2p4 3d1 4D0.5 13356900.0 cm-1
2s2 2p4 3d1 2D1.5 13391100.0 cm-1
2s2 2p4 3d1 4F3.5 13402200.0 cm-1
2s2 2p4 3p1 2P0.5 13421300.0 cm-1
2s2 2p4 3d1 4P2.5 13431800.0 cm-1
2s2 2p4 3p1 2P1.5 13440100.0 cm-1
2s2 2p4 3d1 2F2.5 13444700.0 cm-1
2s2 2p4 3d1 2P1.5 13450500.0 cm-1
2s2 2p4 3d1 2G3.5 13487500.0 cm-1
2s2 2p4 3d1 2G4.5 13506800.0 cm-1
2s2 2p4 3d1 2S0.5 13529400.0 cm-1
2s2 2p4 3d1 2D2.5 13530600.0 cm-1
2s2 2p4 3d1 2F3.5 13554600.0 cm-1
2s2 2p4 3d1 2P1.5 13556000.0 cm-1
2s2 2p4 3d1 2F2.5 13567400.0 cm-1
2s2 2p4 3d1 2D1.5 13627400.0 cm-1
2s2 2p4 3d1 2P0.5 13648000.0 cm-1
2s1 2p5 3s1 4P2.5 13661200.0 cm-1
2s1 2p5 3s1 2P1.5 13725300.0 cm-1
2s1 2p5 3s1 4P1.5 13854800.0 cm-1
2s1 2p5 3s1 2P0.5 13858100.0 cm-1
2s2 2p4 3d1 2D2.5 13928600.0 cm-1
2s2 2p4 3d1 2D1.5 13957800.0 cm-1
2s1 2p5 3p1 4S1.5 14014000.0 cm-1
2s1 2p5 3s1 4P0.5 14040800.0 cm-1
2s1 2p5 3p1 4D2.5 14043300.0 cm-1
2s1 2p5 3p1 4D3.5 14101600.0 cm-1
2s1 2p5 3p1 4D1.5 14122100.0 cm-1
2s1 2p5 3p1 4P2.5 14142700.0 cm-1
2s1 2p5 3p1 4P0.5 14182800.0 cm-1
2s1 2p5 3p1 2P1.5 14203800.0 cm-1
2s1 2p5 3p1 2S0.5 14219900.0 cm-1
2s1 2p5 3p1 2D2.5 14279100.0 cm-1
2s1 2p5 3p1 2D1.5 14285100.0 cm-1
2s1 2p5 3s1 2P1.5 14285500.0 cm-1
2s1 2p5 3s1 2P0.5 14312600.0 cm-1
2s1 2p5 3p1 4D0.5 14333900.0 cm-1
2s1 2p5 3p1 2P0.5 14432200.0 cm-1
2s1 2p5 3p1 4P1.5 14470500.0 cm-1
2s1 2p5 3d1 4P0.5 14517300.0 cm-1
2s1 2p5 3d1 4P1.5 14537100.0 cm-1
2s1 2p5 3d1 4F4.5 14559800.0 cm-1
2s1 2p5 3d1 4D2.5 14564700.0 cm-1
2s1 2p5 3d1 4F3.5 14567200.0 cm-1
2s1 2p5 3d1 4F2.5 14614900.0 cm-1
2s1 2p5 3d1 2F3.5 14628000.0 cm-1
2s1 2p5 3p1 2D1.5 14640200.0 cm-1
2s1 2p5 3d1 2D1.5 14650300.0 cm-1
2s1 2p5 3p1 2P0.5 14712000.0 cm-1
2s1 2p5 3d1 4D0.5 14713600.0 cm-1
2s1 2p5 3p1 2D2.5 14722200.0 cm-1
2s1 2p5 3p1 2P1.5 14739800.0 cm-1
2s1 2p5 3d1 2D2.5 14744000.0 cm-1
2s1 2p5 3d1 4D1.5 14755300.0 cm-1
2s1 2p5 3d1 2P0.5 14760900.0 cm-1
2s1 2p5 3d1 2F2.5 14761200.0 cm-1
2s1 2p5 3d1 4D3.5 14761700.0 cm-1
2s1 2p5 3p1 2S0.5 14767600.0 cm-1
2s1 2p5 3d1 4F1.5 14812600.0 cm-1
2s1 2p5 3d1 4P2.5 14948500.0 cm-1
2s1 2p5 3d1 2P1.5 14972900.0 cm-1
2s1 2p5 3d1 2F2.5 15174100.0 cm-1
2s1 2p5 3d1 2F3.5 15188100.0 cm-1
2s1 2p5 3d1 2P1.5 15212900.0 cm-1
2s1 2p5 3d1 2D2.5 15228200.0 cm-1
2s1 2p5 3d1 2D1.5 15230000.0 cm-1
2s1 2p5 3d1 2P0.5 15239100.0 cm-1
2s2 2p4 4s1 4P2.5 16499700.0 cm-1
2s2 2p4 4s1 2P1.5 16511100.0 cm-1
2s2 2p4 4p1 4P1.5 16649000.0 cm-1
2s2 2p4 4p1 4P2.5 16652400.0 cm-1
2s2 2p4 4s1 4P0.5 16656700.0 cm-1
2s2 2p4 4p1 2D2.5 16681200.0 cm-1
2s2 2p4 4p1 4D3.5 16682100.0 cm-1
2s2 2p4 4p1 2S0.5 16685100.0 cm-1
2s2 2p4 4p1 2P1.5 16728500.0 cm-1
2s2 2p4 4p1 4D0.5 16805300.0 cm-1
2s2 2p4 4s1 4P1.5 16812100.0 cm-1
2s2 2p4 4s1 2P0.5 16820600.0 cm-1
2s2 2p4 4p1 4S1.5 16843400.0 cm-1
2s2 2p4 4d1 4D2.5 16851900.0 cm-1
2s2 2p4 4d1 4D1.5 16852400.0 cm-1
2s2 2p4 4d1 4D3.5 16855600.0 cm-1
2s2 2p4 4d1 4P0.5 16856900.0 cm-1
2s2 2p4 4d1 4F4.5 16864700.0 cm-1
2s2 2p4 4d1 2F3.5 16865900.0 cm-1
2s2 2p4 4d1 2P0.5 16883000.0 cm-1
2s2 2p4 4d1 2D1.5 16900700.0 cm-1
2s2 2p4 4d1 2D2.5 16902300.0 cm-1
2s2 2p4 4s1 2D1.5 16920300.0 cm-1
2s2 2p4 4s1 2D2.5 16920700.0 cm-1
2s2 2p4 4p1 4P0.5 16957600.0 cm-1
2s2 2p4 4f1 4F3.5 16964100.0 cm-1
2s2 2p4 4f1 4F2.5 16964400.0 cm-1
2s2 2p4 4f1 4F4.5 16965800.0 cm-1
2s2 2p4 4f1 4D1.5 16966400.0 cm-1
2s2 2p4 4f1 2G4.5 16968100.0 cm-1
2s2 2p4 4f1 4D0.5 16969400.0 cm-1
2s2 2p4 4f1 4G5.5 16969900.0 cm-1
2s2 2p4 4f1 2F3.5 16971500.0 cm-1
2s2 2p4 4f1 2F2.5 16973900.0 cm-1
2s2 2p4 4p1 4D1.5 16974300.0 cm-1
2s2 2p4 4f1 2D1.5 16974900.0 cm-1
2s2 2p4 4p1 4D2.5 16992000.0 cm-1
2s2 2p4 4p1 2D1.5 17000900.0 cm-1
2s2 2p4 4p1 2P0.5 17009700.0 cm-1
2s2 2p4 4d1 4F1.5 17013200.0 cm-1
2s2 2p4 4d1 4P2.5 17028500.0 cm-1
2s2 2p4 4p1 2F2.5 17065300.0 cm-1
2s2 2p4 4p1 2P1.5 17088500.0 cm-1
2s2 2p4 4p1 2F3.5 17095600.0 cm-1
2s2 2p4 4p1 2D1.5 17099300.0 cm-1
2s2 2p4 4p1 2D2.5 17106900.0 cm-1
2s2 2p4 4f1 4G2.5 17118900.0 cm-1
2s2 2p4 4f1 2G3.5 17123600.0 cm-1
2s2 2p4 4p1 2P0.5 17140700.0 cm-1
2s2 2p4 4d1 4D0.5 17159200.0 cm-1
2s2 2p4 4d1 4P1.5 17171300.0 cm-1
2s2 2p4 4d1 4F3.5 17173000.0 cm-1
2s2 2p4 4d1 4F2.5 17182700.0 cm-1
2s2 2p4 4d1 2F2.5 17186300.0 cm-1
2s2 2p4 4d1 2P1.5 17199700.0 cm-1
2s2 2p4 4d1 2G3.5 17267900.0 cm-1
2s2 2p4 4f1 4F1.5 17273500.0 cm-1
2s2 2p4 4d1 2G4.5 17276000.0 cm-1
2s2 2p4 4f1 4G3.5 17276400.0 cm-1
2s2 2p4 4f1 4D2.5 17278400.0 cm-1
2s2 2p4 4f1 4G4.5 17278800.0 cm-1
2s2 2p4 4d1 2S0.5 17281300.0 cm-1
2s2 2p4 4f1 2D2.5 17282900.0 cm-1
2s2 2p4 4d1 2D2.5 17284800.0 cm-1
2s2 2p4 4f1 4D3.5 17285000.0 cm-1
2s2 2p4 4d1 2P1.5 17285600.0 cm-1
2s2 2p4 4d1 2F2.5 17289800.0 cm-1
2s2 2p4 4d1 2F3.5 17291800.0 cm-1
2s2 2p4 4d1 2D1.5 17312100.0 cm-1
2s2 2p4 4d1 2P0.5 17312400.0 cm-1
2s2 2p4 4s1 2S0.5 17331400.0 cm-1
2s2 2p4 4f1 2P0.5 17374300.0 cm-1
2s2 2p4 4f1 2H4.5 17375300.0 cm-1
2s2 2p4 4f1 2P1.5 17377100.0 cm-1
2s2 2p4 4f1 2H5.5 17379300.0 cm-1
2s2 2p4 4f1 2D2.5 17382500.0 cm-1
2s2 2p4 4f1 2D1.5 17383400.0 cm-1
2s2 2p4 4f1 2G3.5 17385500.0 cm-1
2s2 2p4 4f1 2F2.5 17387300.0 cm-1
2s2 2p4 4f1 2F3.5 17388800.0 cm-1
2s2 2p4 4f1 2G4.5 17389700.0 cm-1
2s2 2p4 4p1 2P0.5 17483500.0 cm-1
2s2 2p4 4p1 2P1.5 17501900.0 cm-1
2s2 2p4 4d1 2D2.5 17684900.0 cm-1
2s2 2p4 4d1 2D1.5 17691000.0 cm-1
2s2 2p4 4f1 2F2.5 17783400.0 cm-1
2s2 2p4 4f1 2F3.5 17786800.0 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 = 1.4054
         2S = 1.2137
         2P = 1.1489
         3S = 1.1382
         3P = 1.0884
         3D = 1.1243
         4S = 1.1551
         4P = 1.1016
         4D = 1.1266
         4F = 1.1387

 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 (0.04251875 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (8.50375 eV) was used
 from the last threshold up to 0.887961 Z**2 Rydbergs (7551 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (8.50375 eV) was used
 from first threshold up to 0.887961 Z**2 Rydbergs (7551 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



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