Resolved Specific Ion Data Collections

Temperature Range
9.134 eV → 9.134 x 104 eV


Full Path
Download data
  • Spontaneous Emission: Ga+22(i) → Ga+22(j) + hv
  • Electron Impact Excitation: Ga+22(i) + e → Ga+22(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 230816.0 cm-1
2s1 2p6 2S0.5 1442740.0 cm-1
2s2 2p4 3s1 4P2.5 9710900.0 cm-1
2s2 2p4 3s1 2P1.5 9745440.0 cm-1
2s2 2p4 3s1 4P0.5 9847160.0 cm-1
2s2 2p4 3s1 4P1.5 9919230.0 cm-1
2s2 2p4 3s1 2P0.5 9947860.0 cm-1
2s2 2p4 3s1 2D2.5 10019700.0 cm-1
2s2 2p4 3p1 4P1.5 10025600.0 cm-1
2s2 2p4 3s1 2D1.5 10027600.0 cm-1
2s2 2p4 3p1 4P2.5 10037700.0 cm-1
2s2 2p4 3p1 2P0.5 10084800.0 cm-1
2s2 2p4 3p1 2D2.5 10088700.0 cm-1
2s2 2p4 3p1 4D3.5 10092800.0 cm-1
2s2 2p4 3p1 4D0.5 10172200.0 cm-1
2s2 2p4 3p1 4S1.5 10185400.0 cm-1
2s2 2p4 3p1 4D1.5 10223200.0 cm-1
2s2 2p4 3p1 4P0.5 10225100.0 cm-1
2s2 2p4 3p1 2P1.5 10267300.0 cm-1
2s2 2p4 3p1 4D2.5 10289900.0 cm-1
2s2 2p4 3p1 2S0.5 10313500.0 cm-1
2s2 2p4 3s1 2S0.5 10314200.0 cm-1
2s2 2p4 3p1 2D1.5 10318300.0 cm-1
2s2 2p4 3p1 2F2.5 10338100.0 cm-1
2s2 2p4 3p1 2F3.5 10388300.0 cm-1
2s2 2p4 3p1 2D1.5 10397400.0 cm-1
2s2 2p4 3p1 2D2.5 10419900.0 cm-1
2s2 2p4 3p1 2P1.5 10453700.0 cm-1
2s2 2p4 3d1 4D2.5 10483600.0 cm-1
2s2 2p4 3d1 4D1.5 10486800.0 cm-1
2s2 2p4 3d1 4D3.5 10490500.0 cm-1
2s2 2p4 3d1 2P0.5 10499300.0 cm-1
2s2 2p4 3d1 4F4.5 10518200.0 cm-1
2s2 2p4 3p1 2P0.5 10521100.0 cm-1
2s2 2p4 3d1 2F3.5 10526000.0 cm-1
2s2 2p4 3d1 4P0.5 10554400.0 cm-1
2s2 2p4 3d1 4P1.5 10580100.0 cm-1
2s2 2p4 3d1 2D2.5 10599500.0 cm-1
2s2 2p4 3d1 4F1.5 10642700.0 cm-1
2s2 2p4 3d1 4F2.5 10656500.0 cm-1
2s2 2p4 3d1 4D0.5 10678700.0 cm-1
2s2 2p4 3p1 2P1.5 10691700.0 cm-1
2s2 2p4 3p1 2P0.5 10693600.0 cm-1
2s2 2p4 3d1 2D1.5 10707800.0 cm-1
2s2 2p4 3d1 4F3.5 10712200.0 cm-1
2s2 2p4 3d1 4P2.5 10739800.0 cm-1
2s2 2p4 3d1 2P1.5 10754800.0 cm-1
2s2 2p4 3d1 2F2.5 10757500.0 cm-1
2s2 2p4 3d1 2G3.5 10795500.0 cm-1
2s2 2p4 3d1 2G4.5 10807000.0 cm-1
2s2 2p4 3d1 2D2.5 10830900.0 cm-1
2s2 2p4 3d1 2S0.5 10832500.0 cm-1
2s2 2p4 3d1 2F3.5 10850600.0 cm-1
2s2 2p4 3d1 2P1.5 10858800.0 cm-1
2s2 2p4 3d1 2F2.5 10869000.0 cm-1
2s2 2p4 3d1 2D1.5 10913500.0 cm-1
2s2 2p4 3d1 2P0.5 10928300.0 cm-1
2s1 2p5 3s1 4P2.5 10976000.0 cm-1
2s1 2p5 3s1 4P1.5 11030000.0 cm-1
2s2 2p4 3d1 2D2.5 11119400.0 cm-1
2s1 2p5 3s1 2P1.5 11125100.0 cm-1
2s1 2p5 3s1 4P0.5 11127300.0 cm-1
2s2 2p4 3d1 2D1.5 11147200.0 cm-1
2s1 2p5 3s1 2P0.5 11242000.0 cm-1
2s1 2p5 3p1 4S1.5 11283100.0 cm-1
2s1 2p5 3p1 4D2.5 11312500.0 cm-1
2s1 2p5 3p1 4D3.5 11345100.0 cm-1
2s1 2p5 3p1 4D1.5 11364500.0 cm-1
2s1 2p5 3p1 4P2.5 11381700.0 cm-1
2s1 2p5 3p1 4P0.5 11413000.0 cm-1
2s1 2p5 3p1 2P1.5 11432500.0 cm-1
2s1 2p5 3p1 2P0.5 11452300.0 cm-1
2s1 2p5 3p1 2D2.5 11480500.0 cm-1
2s1 2p5 3p1 2D1.5 11485400.0 cm-1
2s1 2p5 3s1 2P1.5 11486100.0 cm-1
2s1 2p5 3s1 2P0.5 11502700.0 cm-1
2s1 2p5 3p1 4D0.5 11512800.0 cm-1
2s1 2p5 3p1 2S0.5 11597300.0 cm-1
2s1 2p5 3p1 4P1.5 11597500.0 cm-1
2s1 2p5 3d1 4P0.5 11713500.0 cm-1
2s1 2p5 3d1 4P1.5 11729200.0 cm-1
2s1 2p5 3d1 4F4.5 11745500.0 cm-1
2s1 2p5 3d1 4P2.5 11752500.0 cm-1
2s1 2p5 3d1 4F3.5 11755500.0 cm-1
2s1 2p5 3d1 4F2.5 11792100.0 cm-1
2s1 2p5 3p1 2D1.5 11797200.0 cm-1
2s1 2p5 3d1 2F3.5 11805600.0 cm-1
2s1 2p5 3d1 4D1.5 11820300.0 cm-1
2s1 2p5 3p1 2P0.5 11846900.0 cm-1
2s1 2p5 3p1 2D2.5 11849900.0 cm-1
2s1 2p5 3p1 2P1.5 11867100.0 cm-1
2s1 2p5 3d1 4D0.5 11868700.0 cm-1
2s1 2p5 3d1 2D2.5 11892500.0 cm-1
2s1 2p5 3d1 2F2.5 11900800.0 cm-1
2s1 2p5 3d1 4D3.5 11901900.0 cm-1
2s1 2p5 3p1 2S0.5 11904200.0 cm-1
2s1 2p5 3d1 2D1.5 11904300.0 cm-1
2s1 2p5 3d1 2P0.5 11921800.0 cm-1
2s1 2p5 3d1 4F1.5 11933500.0 cm-1
2s1 2p5 3d1 4D2.5 12016800.0 cm-1
2s1 2p5 3d1 2P1.5 12056600.0 cm-1
2s1 2p5 3d1 2F2.5 12249400.0 cm-1
2s1 2p5 3d1 2F3.5 12257100.0 cm-1
2s1 2p5 3d1 2P1.5 12280800.0 cm-1
2s1 2p5 3d1 2D2.5 12292400.0 cm-1
2s1 2p5 3d1 2D1.5 12294500.0 cm-1
2s1 2p5 3d1 2P0.5 12301600.0 cm-1
2s2 2p4 4s1 4P2.5 13161300.0 cm-1
2s2 2p4 4s1 2P1.5 13171800.0 cm-1
2s2 2p4 4s1 4P0.5 13291200.0 cm-1
2s2 2p4 4p1 4P1.5 13292500.0 cm-1
2s2 2p4 4p1 4P2.5 13294900.0 cm-1
2s2 2p4 4p1 2D2.5 13313800.0 cm-1
2s2 2p4 4p1 4D3.5 13314200.0 cm-1
2s2 2p4 4p1 2S0.5 13318000.0 cm-1
2s2 2p4 4p1 2P1.5 13354500.0 cm-1
2s2 2p4 4s1 4P1.5 13364700.0 cm-1
2s2 2p4 4s1 2P0.5 13372600.0 cm-1
2s2 2p4 4p1 4D0.5 13421700.0 cm-1
2s2 2p4 4p1 4S1.5 13446700.0 cm-1
2s2 2p4 4s1 2D2.5 13460800.0 cm-1
2s2 2p4 4s1 2D1.5 13463500.0 cm-1
2s2 2p4 4d1 4D2.5 13463600.0 cm-1
2s2 2p4 4d1 4P1.5 13464900.0 cm-1
2s2 2p4 4d1 4D3.5 13465200.0 cm-1
2s2 2p4 4d1 4P0.5 13468600.0 cm-1
2s2 2p4 4d1 4F4.5 13473200.0 cm-1
2s2 2p4 4d1 2F3.5 13475900.0 cm-1
2s2 2p4 4d1 2P0.5 13489700.0 cm-1
2s2 2p4 4p1 4P0.5 13492100.0 cm-1
2s2 2p4 4d1 2D1.5 13504600.0 cm-1
2s2 2p4 4p1 4D1.5 13508100.0 cm-1
2s2 2p4 4d1 2D2.5 13509400.0 cm-1
2s2 2p4 4p1 4D2.5 13515100.0 cm-1
2s2 2p4 4p1 2D1.5 13523200.0 cm-1
2s2 2p4 4p1 2P0.5 13531400.0 cm-1
2s2 2p4 4f1 4F3.5 13558500.0 cm-1
2s2 2p4 4f1 4F2.5 13559000.0 cm-1
2s2 2p4 4f1 4F4.5 13559700.0 cm-1
2s2 2p4 4f1 4D1.5 13561200.0 cm-1
2s2 2p4 4f1 2G4.5 13561700.0 cm-1
2s2 2p4 4f1 4G5.5 13562900.0 cm-1
2s2 2p4 4f1 2F3.5 13563900.0 cm-1
2s2 2p4 4f1 4D0.5 13564000.0 cm-1
2s2 2p4 4f1 2F2.5 13566300.0 cm-1
2s2 2p4 4f1 2D1.5 13567700.0 cm-1
2s2 2p4 4p1 2F2.5 13591600.0 cm-1
2s2 2p4 4d1 4F1.5 13597300.0 cm-1
2s2 2p4 4d1 4F2.5 13607200.0 cm-1
2s2 2p4 4p1 2F3.5 13610900.0 cm-1
2s2 2p4 4p1 2P1.5 13611300.0 cm-1
2s2 2p4 4p1 2D1.5 13616400.0 cm-1
2s2 2p4 4p1 2D2.5 13621300.0 cm-1
2s2 2p4 4p1 2P0.5 13650800.0 cm-1
2s2 2p4 4d1 4D0.5 13663200.0 cm-1
2s2 2p4 4d1 4F3.5 13672600.0 cm-1
2s2 2p4 4d1 4D1.5 13673500.0 cm-1
2s2 2p4 4d1 4P2.5 13682300.0 cm-1
2s2 2p4 4f1 4G2.5 13686700.0 cm-1
2s2 2p4 4d1 2F2.5 13687000.0 cm-1
2s2 2p4 4f1 2G3.5 13689700.0 cm-1
2s2 2p4 4d1 2P1.5 13697000.0 cm-1
2s2 2p4 4s1 2S0.5 13752700.0 cm-1
2s2 2p4 4f1 4F1.5 13759500.0 cm-1
2s2 2p4 4f1 4G3.5 13761700.0 cm-1
2s2 2p4 4d1 2G3.5 13762700.0 cm-1
2s2 2p4 4f1 4G4.5 13762800.0 cm-1
2s2 2p4 4f1 4D2.5 13763000.0 cm-1
2s2 2p4 4f1 2D2.5 13766900.0 cm-1
2s2 2p4 4d1 2G4.5 13767600.0 cm-1
2s2 2p4 4f1 4D3.5 13768100.0 cm-1
2s2 2p4 4d1 2D2.5 13776100.0 cm-1
2s2 2p4 4d1 2S0.5 13777700.0 cm-1
2s2 2p4 4d1 2P1.5 13778600.0 cm-1
2s2 2p4 4d1 2F3.5 13782100.0 cm-1
2s2 2p4 4d1 2F2.5 13782600.0 cm-1
2s2 2p4 4d1 2D1.5 13799900.0 cm-1
2s2 2p4 4d1 2P0.5 13808100.0 cm-1
2s2 2p4 4f1 2P0.5 13852600.0 cm-1
2s2 2p4 4f1 2H4.5 13853200.0 cm-1
2s2 2p4 4f1 2P1.5 13854600.0 cm-1
2s2 2p4 4f1 2H5.5 13855700.0 cm-1
2s2 2p4 4f1 2D2.5 13859300.0 cm-1
2s2 2p4 4f1 2D1.5 13859800.0 cm-1
2s2 2p4 4f1 2G3.5 13862500.0 cm-1
2s2 2p4 4f1 2F2.5 13863600.0 cm-1
2s2 2p4 4f1 2F3.5 13864500.0 cm-1
2s2 2p4 4f1 2G4.5 13865200.0 cm-1
2s2 2p4 4p1 2P0.5 13898000.0 cm-1
2s2 2p4 4p1 2P1.5 13907500.0 cm-1
2s2 2p4 4d1 2D2.5 14066800.0 cm-1
2s2 2p4 4d1 2D1.5 14073500.0 cm-1
2s2 2p4 4f1 2F2.5 14151200.0 cm-1
2s2 2p4 4f1 2F3.5 14153300.0 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 = 1.4082
         2S = 1.2118
         2P = 1.1476
         3S = 1.1359
         3P = 1.0860
         3D = 1.1213
         4S = 1.1525
         4P = 1.0989
         4D = 1.1235
         4F = 1.1340

 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 (0.03292652 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (6.585304 eV) was used
 from the last threshold up to 0.908386 Z**2 Rydbergs (5982 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (6.585304 eV) was used
 from first threshold up to 0.908386 Z**2 Rydbergs (5982 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
  • Processes
  • States
  • Comments
  • Origins

Data Classes