Resolved Specific Ion Data Collections

Temperature Range
10.77 eV → 1.077 x 105 eV


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  • Spontaneous Emission: As+24(i) → As+24(j) + hv
  • Electron Impact Excitation: As+24(i) + e → As+24(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 304432.0 cm-1
2s1 2p6 2S0.5 1613260.0 cm-1
2s2 2p4 3s1 4P2.5 11314000.0 cm-1
2s2 2p4 3s1 2P1.5 11350900.0 cm-1
2s2 2p4 3s1 4P0.5 11470300.0 cm-1
2s2 2p4 3s1 4P1.5 11590700.0 cm-1
2s2 2p4 3s1 2P0.5 11620600.0 cm-1
2s2 2p4 3p1 4P1.5 11657200.0 cm-1
2s2 2p4 3p1 4P2.5 11672200.0 cm-1
2s2 2p4 3s1 2D2.5 11696800.0 cm-1
2s2 2p4 3s1 2D1.5 11706500.0 cm-1
2s2 2p4 3p1 2P0.5 11732900.0 cm-1
2s2 2p4 3p1 2D2.5 11737600.0 cm-1
2s2 2p4 3p1 4D3.5 11743300.0 cm-1
2s2 2p4 3p1 4D0.5 11824600.0 cm-1
2s2 2p4 3p1 4S1.5 11850600.0 cm-1
2s2 2p4 3p1 4D1.5 11898900.0 cm-1
2s2 2p4 3p1 4P0.5 11924700.0 cm-1
2s2 2p4 3p1 2P1.5 11967000.0 cm-1
2s2 2p4 3p1 4D2.5 12008100.0 cm-1
2s2 2p4 3p1 2S0.5 12033000.0 cm-1
2s2 2p4 3p1 2D1.5 12037500.0 cm-1
2s2 2p4 3p1 2F2.5 12044100.0 cm-1
2s2 2p4 3s1 2S0.5 12060800.0 cm-1
2s2 2p4 3p1 2F3.5 12112600.0 cm-1
2s2 2p4 3p1 2D1.5 12119000.0 cm-1
2s2 2p4 3p1 2D2.5 12145900.0 cm-1
2s2 2p4 3p1 2P1.5 12165800.0 cm-1
2s2 2p4 3d1 4D2.5 12169500.0 cm-1
2s2 2p4 3d1 4D1.5 12171300.0 cm-1
2s2 2p4 3d1 4D3.5 12179500.0 cm-1
2s2 2p4 3d1 2P0.5 12185000.0 cm-1
2s2 2p4 3d1 4F4.5 12208600.0 cm-1
2s2 2p4 3d1 2F3.5 12213900.0 cm-1
2s2 2p4 3d1 4P0.5 12248600.0 cm-1
2s2 2p4 3p1 2P0.5 12257900.0 cm-1
2s2 2p4 3d1 4P1.5 12278200.0 cm-1
2s2 2p4 3d1 2D2.5 12301800.0 cm-1
2s2 2p4 3d1 4F1.5 12351400.0 cm-1
2s2 2p4 3d1 4F2.5 12372600.0 cm-1
2s2 2p4 3d1 4D0.5 12428800.0 cm-1
2s2 2p4 3d1 2D1.5 12461300.0 cm-1
2s2 2p4 3d1 4F3.5 12469900.0 cm-1
2s2 2p4 3p1 2P0.5 12473900.0 cm-1
2s2 2p4 3p1 2P1.5 12484500.0 cm-1
2s2 2p4 3d1 4P2.5 12499300.0 cm-1
2s2 2p4 3d1 2F2.5 12513100.0 cm-1
2s2 2p4 3d1 2P1.5 12516300.0 cm-1
2s2 2p4 3d1 2G3.5 12554900.0 cm-1
2s2 2p4 3d1 2G4.5 12571200.0 cm-1
2s2 2p4 3d1 2D2.5 12595000.0 cm-1
2s2 2p4 3d1 2S0.5 12595100.0 cm-1
2s2 2p4 3d1 2F3.5 12617700.0 cm-1
2s2 2p4 3d1 2P1.5 12621500.0 cm-1
2s2 2p4 3d1 2F2.5 12632700.0 cm-1
2s2 2p4 3d1 2D1.5 12687100.0 cm-1
2s2 2p4 3d1 2P0.5 12705900.0 cm-1
2s1 2p5 3s1 4P2.5 12731800.0 cm-1
2s1 2p5 3s1 2P1.5 12792500.0 cm-1
2s1 2p5 3s1 4P1.5 12910000.0 cm-1
2s1 2p5 3s1 4P0.5 12913400.0 cm-1
2s2 2p4 3d1 2D2.5 12952400.0 cm-1
2s2 2p4 3d1 2D1.5 12981700.0 cm-1
2s1 2p5 3p1 4S1.5 13069300.0 cm-1
2s1 2p5 3s1 2P0.5 13069500.0 cm-1
2s1 2p5 3p1 4D2.5 13098700.0 cm-1
2s1 2p5 3p1 4D3.5 13147300.0 cm-1
2s1 2p5 3p1 4D1.5 13167500.0 cm-1
2s1 2p5 3p1 4P2.5 13186900.0 cm-1
2s1 2p5 3p1 4P0.5 13224300.0 cm-1
2s1 2p5 3p1 2P1.5 13245300.0 cm-1
2s1 2p5 3p1 2P0.5 13262500.0 cm-1
2s1 2p5 3p1 2D2.5 13310500.0 cm-1
2s1 2p5 3s1 2P1.5 13314500.0 cm-1
2s1 2p5 3p1 2D1.5 13316100.0 cm-1
2s1 2p5 3s1 2P0.5 13337700.0 cm-1
2s1 2p5 3p1 4D0.5 13357200.0 cm-1
2s1 2p5 3p1 2S0.5 13449300.0 cm-1
2s1 2p5 3p1 4P1.5 13473400.0 cm-1
2s1 2p5 3d1 4P0.5 13547200.0 cm-1
2s1 2p5 3d1 4P1.5 13565600.0 cm-1
2s1 2p5 3d1 4F4.5 13585900.0 cm-1
2s1 2p5 3d1 4D2.5 13591800.0 cm-1
2s1 2p5 3d1 4F3.5 13594500.0 cm-1
2s1 2p5 3d1 4F2.5 13638300.0 cm-1
2s1 2p5 3d1 2F3.5 13651400.0 cm-1
2s1 2p5 3p1 2D1.5 13654500.0 cm-1
2s1 2p5 3d1 4D1.5 13671300.0 cm-1
2s1 2p5 3p1 2P0.5 13718100.0 cm-1
2s1 2p5 3p1 2D2.5 13725700.0 cm-1
2s1 2p5 3d1 4D0.5 13729400.0 cm-1
2s1 2p5 3p1 2P1.5 13743200.0 cm-1
2s1 2p5 3d1 2D2.5 13757800.0 cm-1
2s1 2p5 3d1 2D1.5 13769000.0 cm-1
2s1 2p5 3d1 2F2.5 13771400.0 cm-1
2s1 2p5 3d1 4D3.5 13772400.0 cm-1
2s1 2p5 3p1 2S0.5 13774800.0 cm-1
2s1 2p5 3d1 2P0.5 13778900.0 cm-1
2s1 2p5 3d1 4F1.5 13816700.0 cm-1
2s1 2p5 3d1 4P2.5 13931500.0 cm-1
2s1 2p5 3d1 2P1.5 13961700.0 cm-1
2s1 2p5 3d1 2F2.5 14160200.0 cm-1
2s1 2p5 3d1 2F3.5 14171700.0 cm-1
2s1 2p5 3d1 2P1.5 14196100.0 cm-1
2s1 2p5 3d1 2D2.5 14210200.0 cm-1
2s1 2p5 3d1 2D1.5 14212300.0 cm-1
2s1 2p5 3d1 2P0.5 14220800.0 cm-1
2s2 2p4 4s1 4P2.5 15345100.0 cm-1
2s2 2p4 4s1 2P1.5 15356200.0 cm-1
2s2 2p4 4p1 4P1.5 15488300.0 cm-1
2s2 2p4 4p1 4D2.5 15491400.0 cm-1
2s2 2p4 4s1 4P0.5 15493200.0 cm-1
2s2 2p4 4p1 2D2.5 15516500.0 cm-1
2s2 2p4 4p1 4D3.5 15517200.0 cm-1
2s2 2p4 4p1 2S0.5 15520500.0 cm-1
2s2 2p4 4p1 2P1.5 15561600.0 cm-1
2s2 2p4 4s1 4P1.5 15617200.0 cm-1
2s2 2p4 4s1 2P0.5 15625500.0 cm-1
2s2 2p4 4p1 4D0.5 15635800.0 cm-1
2s2 2p4 4p1 4S1.5 15669200.0 cm-1
2s2 2p4 4d1 4D2.5 15680000.0 cm-1
2s2 2p4 4d1 4D1.5 15680800.0 cm-1
2s2 2p4 4d1 4D3.5 15683200.0 cm-1
2s2 2p4 4d1 4P0.5 15685200.0 cm-1
2s2 2p4 4d1 4F4.5 15691800.0 cm-1
2s2 2p4 4d1 2F3.5 15693500.0 cm-1
2s2 2p4 4d1 2P0.5 15709500.0 cm-1
2s2 2p4 4s1 2D2.5 15716500.0 cm-1
2s2 2p4 4s1 2D1.5 15721700.0 cm-1
2s2 2p4 4d1 2D1.5 15726900.0 cm-1
2s2 2p4 4d1 2D2.5 15734200.0 cm-1
2s2 2p4 4p1 4P0.5 15756600.0 cm-1
2s2 2p4 4p1 4D1.5 15772900.0 cm-1
2s2 2p4 4p1 4P2.5 15786200.0 cm-1
2s2 2p4 4f1 4F3.5 15786400.0 cm-1
2s2 2p4 4f1 4F2.5 15787400.0 cm-1
2s2 2p4 4f1 4F4.5 15788100.0 cm-1
2s2 2p4 4f1 4D1.5 15789100.0 cm-1
2s2 2p4 4f1 2G4.5 15790100.0 cm-1
2s2 2p4 4f1 4G5.5 15791800.0 cm-1
2s2 2p4 4f1 4D0.5 15791800.0 cm-1
2s2 2p4 4f1 2F3.5 15793100.0 cm-1
2s2 2p4 4p1 2D1.5 15795300.0 cm-1
2s2 2p4 4f1 2F2.5 15795600.0 cm-1
2s2 2p4 4f1 2D1.5 15796900.0 cm-1
2s2 2p4 4p1 2P0.5 15804100.0 cm-1
2s2 2p4 4d1 4F1.5 15832500.0 cm-1
2s2 2p4 4d1 4P2.5 15845900.0 cm-1
2s2 2p4 4p1 2F2.5 15861600.0 cm-1
2s2 2p4 4p1 2P1.5 15883700.0 cm-1
2s2 2p4 4p1 2F3.5 15887800.0 cm-1
2s2 2p4 4p1 2D1.5 15891900.0 cm-1
2s2 2p4 4p1 2D2.5 15898800.0 cm-1
2s2 2p4 4p1 2P0.5 15931200.0 cm-1
2s2 2p4 4f1 4G2.5 15932600.0 cm-1
2s2 2p4 4f1 2G3.5 15936700.0 cm-1
2s2 2p4 4d1 4D0.5 15947600.0 cm-1
2s2 2p4 4d1 4P1.5 15959100.0 cm-1
2s2 2p4 4d1 4F3.5 15959800.0 cm-1
2s2 2p4 4d1 4F2.5 15969800.0 cm-1
2s2 2p4 4d1 2F2.5 15973300.0 cm-1
2s2 2p4 4d1 2P1.5 15985700.0 cm-1
2s2 2p4 4d1 2G3.5 16053300.0 cm-1
2s2 2p4 4f1 4F1.5 16055800.0 cm-1
2s2 2p4 4f1 4G3.5 16058500.0 cm-1
2s2 2p4 4d1 2G4.5 16060200.0 cm-1
2s2 2p4 4f1 4D2.5 16060200.0 cm-1
2s2 2p4 4f1 4G4.5 16060400.0 cm-1
2s2 2p4 4f1 2D2.5 16064500.0 cm-1
2s2 2p4 4d1 2S0.5 16064600.0 cm-1
2s2 2p4 4f1 4D3.5 16066300.0 cm-1
2s2 2p4 4d1 2D2.5 16068900.0 cm-1
2s2 2p4 4d1 2P1.5 16070300.0 cm-1
2s2 2p4 4d1 2F2.5 16074500.0 cm-1
2s2 2p4 4d1 2F3.5 16075500.0 cm-1
2s2 2p4 4s1 2S0.5 16081900.0 cm-1
2s2 2p4 4d1 2D1.5 16095100.0 cm-1
2s2 2p4 4d1 2P0.5 16107200.0 cm-1
2s2 2p4 4f1 2P0.5 16154000.0 cm-1
2s2 2p4 4f1 2H4.5 16154900.0 cm-1
2s2 2p4 4f1 2P1.5 16156500.0 cm-1
2s2 2p4 4f1 2H5.5 16158300.0 cm-1
2s2 2p4 4f1 2D2.5 16161700.0 cm-1
2s2 2p4 4f1 2D1.5 16162400.0 cm-1
2s2 2p4 4f1 2G3.5 16164800.0 cm-1
2s2 2p4 4f1 2F2.5 16166300.0 cm-1
2s2 2p4 4f1 2F3.5 16167600.0 cm-1
2s2 2p4 4f1 2G4.5 16168400.0 cm-1
2s2 2p4 4p1 2P0.5 16238300.0 cm-1
2s2 2p4 4p1 2P1.5 16253400.0 cm-1
2s2 2p4 4d1 2D2.5 16428400.0 cm-1
2s2 2p4 4d1 2D1.5 16434800.0 cm-1
2s2 2p4 4f1 2F2.5 16522100.0 cm-1
2s2 2p4 4f1 2F3.5 16525100.0 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 = 1.4063
         2S = 1.2131
         2P = 1.1485
         3S = 1.1375
         3P = 1.0876
         3D = 1.1234
         4S = 1.1543
         4P = 1.1008
         4D = 1.1256
         4F = 1.1373

 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 (0.03918528 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (7.837056 eV) was used
 from the last threshold up to 0.894596 Z**2 Rydbergs (7011 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (7.837056 eV) was used
 from first threshold up to 0.894596 Z**2 Rydbergs (7011 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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