Resolved Specific Ion Data Collections

Temperature Range
9.909 eV → 9.909 x 104 eV


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  • Spontaneous Emission: Ge+23(i) → Ge+23(j) + hv
  • Electron Impact Excitation: Ge+23(i) + e → Ge+23(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 265709.0 cm-1
2s1 2p6 2S0.5 1525920.0 cm-1
2s2 2p4 3s1 4P2.5 10497400.0 cm-1
2s2 2p4 3s1 2P1.5 10533100.0 cm-1
2s2 2p4 3s1 4P0.5 10643800.0 cm-1
2s2 2p4 3s1 4P1.5 10738000.0 cm-1
2s2 2p4 3s1 2P0.5 10767200.0 cm-1
2s2 2p4 3p1 4P1.5 10826300.0 cm-1
2s2 2p4 3p1 4P2.5 10839900.0 cm-1
2s2 2p4 3s1 2D2.5 10841300.0 cm-1
2s2 2p4 3s1 2D1.5 10850000.0 cm-1
2s2 2p4 3p1 2P0.5 10893300.0 cm-1
2s2 2p4 3p1 2D2.5 10897400.0 cm-1
2s2 2p4 3p1 4D3.5 10902400.0 cm-1
2s2 2p4 3p1 4D0.5 10983300.0 cm-1
2s2 2p4 3p1 4S1.5 11002400.0 cm-1
2s2 2p4 3p1 4D1.5 11045500.0 cm-1
2s2 2p4 3p1 4P0.5 11057900.0 cm-1
2s2 2p4 3p1 2P1.5 11100100.0 cm-1
2s2 2p4 3p1 4D2.5 11131500.0 cm-1
2s2 2p4 3p1 2S0.5 11155700.0 cm-1
2s2 2p4 3p1 2D1.5 11160400.0 cm-1
2s2 2p4 3s1 2S0.5 11168600.0 cm-1
2s2 2p4 3p1 2F2.5 11174100.0 cm-1
2s2 2p4 3p1 2F3.5 11232900.0 cm-1
2s2 2p4 3p1 2D1.5 11240700.0 cm-1
2s2 2p4 3p1 2D2.5 11265400.0 cm-1
2s2 2p4 3p1 2P1.5 11292700.0 cm-1
2s2 2p4 3d1 4D2.5 11310900.0 cm-1
2s2 2p4 3d1 4D1.5 11313400.0 cm-1
2s2 2p4 3d1 4D3.5 11319300.0 cm-1
2s2 2p4 3d1 2P0.5 11326500.0 cm-1
2s2 2p4 3d1 4F4.5 11347600.0 cm-1
2s2 2p4 3d1 2F3.5 11354200.0 cm-1
2s2 2p4 3p1 2P0.5 11371900.0 cm-1
2s2 2p4 3d1 4P0.5 11385700.0 cm-1
2s2 2p4 3d1 4P1.5 11413400.0 cm-1
2s2 2p4 3d1 2D2.5 11434900.0 cm-1
2s2 2p4 3d1 4F1.5 11481500.0 cm-1
2s2 2p4 3d1 4F2.5 11498800.0 cm-1
2s2 2p4 3d1 4D0.5 11536200.0 cm-1
2s2 2p4 3p1 2P0.5 11564900.0 cm-1
2s2 2p4 3d1 2D1.5 11567000.0 cm-1
2s2 2p4 3p1 2P1.5 11568600.0 cm-1
2s2 2p4 3d1 4F3.5 11573300.0 cm-1
2s2 2p4 3d1 4P2.5 11602000.0 cm-1
2s2 2p4 3d1 2F2.5 11617600.0 cm-1
2s2 2p4 3d1 2P1.5 11617900.0 cm-1
2s2 2p4 3d1 2G3.5 11657700.0 cm-1
2s2 2p4 3d1 2G4.5 11671400.0 cm-1
2s2 2p4 3d1 2D2.5 11695200.0 cm-1
2s2 2p4 3d1 2S0.5 11696200.0 cm-1
2s2 2p4 3d1 2F3.5 11716500.0 cm-1
2s2 2p4 3d1 2P1.5 11722500.0 cm-1
2s2 2p4 3d1 2F2.5 11733400.0 cm-1
2s2 2p4 3d1 2D1.5 11782600.0 cm-1
2s2 2p4 3d1 2P0.5 11799400.0 cm-1
2s1 2p5 3s1 4P2.5 11836800.0 cm-1
2s1 2p5 3s1 2P1.5 11894200.0 cm-1
2s1 2p5 3s1 4P1.5 12000200.0 cm-1
2s1 2p5 3s1 4P0.5 12003200.0 cm-1
2s2 2p4 3d1 2D2.5 12016200.0 cm-1
2s2 2p4 3d1 2D1.5 12045000.0 cm-1
2s1 2p5 3s1 2P0.5 12136700.0 cm-1
2s1 2p5 3p1 4S1.5 12159100.0 cm-1
2s1 2p5 3p1 4D2.5 12188500.0 cm-1
2s1 2p5 3p1 4D3.5 12228600.0 cm-1
2s1 2p5 3p1 4D1.5 12248400.0 cm-1
2s1 2p5 3p1 4P2.5 12266700.0 cm-1
2s1 2p5 3p1 4P0.5 12301100.0 cm-1
2s1 2p5 3p1 2P1.5 12321500.0 cm-1
2s1 2p5 3p1 2P0.5 12340100.0 cm-1
2s1 2p5 3p1 2D2.5 12377700.0 cm-1
2s1 2p5 3s1 2P1.5 12381600.0 cm-1
2s1 2p5 3p1 2D1.5 12382900.0 cm-1
2s1 2p5 3s1 2P0.5 12401300.0 cm-1
2s1 2p5 3p1 4D0.5 12416900.0 cm-1
2s1 2p5 3p1 2S0.5 12504500.0 cm-1
2s1 2p5 3p1 4P1.5 12516000.0 cm-1
2s1 2p5 3d1 4P0.5 12612700.0 cm-1
2s1 2p5 3d1 4P1.5 12629800.0 cm-1
2s1 2p5 3d1 4F4.5 12647900.0 cm-1
2s1 2p5 3d1 4D2.5 12654500.0 cm-1
2s1 2p5 3d1 4F3.5 12657300.0 cm-1
2s1 2p5 3d1 4F2.5 12697400.0 cm-1
2s1 2p5 3p1 2D1.5 12707100.0 cm-1
2s1 2p5 3d1 2F3.5 12710800.0 cm-1
2s1 2p5 3d1 4D1.5 12728100.0 cm-1
2s1 2p5 3p1 2P0.5 12763300.0 cm-1
2s1 2p5 3p1 2D2.5 12768500.0 cm-1
2s1 2p5 3d1 4D0.5 12781200.0 cm-1
2s1 2p5 3p1 2P1.5 12785900.0 cm-1
2s1 2p5 3d1 2D2.5 12807400.0 cm-1
2s1 2p5 3d1 2F2.5 12818000.0 cm-1
2s1 2p5 3d1 2D1.5 12818800.0 cm-1
2s1 2p5 3d1 4D3.5 12819200.0 cm-1
2s1 2p5 3p1 2S0.5 12820600.0 cm-1
2s1 2p5 3d1 2P0.5 12832600.0 cm-1
2s1 2p5 3d1 4F1.5 12857000.0 cm-1
2s1 2p5 3d1 4P2.5 12954500.0 cm-1
2s1 2p5 3d1 2P1.5 12989900.0 cm-1
2s1 2p5 3d1 2F2.5 13185500.0 cm-1
2s1 2p5 3d1 2F3.5 13194900.0 cm-1
2s1 2p5 3d1 2P1.5 13219000.0 cm-1
2s1 2p5 3d1 2D2.5 13231800.0 cm-1
2s1 2p5 3d1 2D1.5 13234000.0 cm-1
2s1 2p5 3d1 2P0.5 13241900.0 cm-1
2s2 2p4 4s1 4P2.5 14232300.0 cm-1
2s2 2p4 4s1 2P1.5 14243100.0 cm-1
2s2 2p4 4p1 4P1.5 14369500.0 cm-1
2s2 2p4 4s1 4P0.5 14371400.0 cm-1
2s2 2p4 4p1 4P2.5 14372200.0 cm-1
2s2 2p4 4p1 2D2.5 14394000.0 cm-1
2s2 2p4 4p1 4D3.5 14394600.0 cm-1
2s2 2p4 4p1 2S0.5 14398100.0 cm-1
2s2 2p4 4p1 2P1.5 14437000.0 cm-1
2s2 2p4 4s1 4P1.5 14468200.0 cm-1
2s2 2p4 4s1 2P0.5 14476300.0 cm-1
2s2 2p4 4p1 4D0.5 14507900.0 cm-1
2s2 2p4 4p1 4S1.5 14537000.0 cm-1
2s2 2p4 4d1 4D2.5 14550500.0 cm-1
2s2 2p4 4d1 4D1.5 14551500.0 cm-1
2s2 2p4 4d1 4D3.5 14553000.0 cm-1
2s2 2p4 4d1 4P0.5 14555800.0 cm-1
2s2 2p4 4d1 4F4.5 14561300.0 cm-1
2s2 2p4 4d1 2F3.5 14563600.0 cm-1
2s2 2p4 4s1 2D2.5 14566800.0 cm-1
2s2 2p4 4s1 2D1.5 14570300.0 cm-1
2s2 2p4 4d1 2P0.5 14578400.0 cm-1
2s2 2p4 4d1 2D1.5 14594300.0 cm-1
2s2 2p4 4d1 2D2.5 14599900.0 cm-1
2s2 2p4 4p1 4P0.5 14601600.0 cm-1
2s2 2p4 4p1 4D1.5 14617700.0 cm-1
2s2 2p4 4p1 4D2.5 14627900.0 cm-1
2s2 2p4 4p1 2D1.5 14636300.0 cm-1
2s2 2p4 4p1 2P0.5 14644600.0 cm-1
2s2 2p4 4f1 4F3.5 14651300.0 cm-1
2s2 2p4 4f1 4F2.5 14651700.0 cm-1
2s2 2p4 4f1 4F4.5 14652700.0 cm-1
2s2 2p4 4f1 4D1.5 14654000.0 cm-1
2s2 2p4 4f1 2G4.5 14654700.0 cm-1
2s2 2p4 4f1 4G5.5 14656100.0 cm-1
2s2 2p4 4f1 4D0.5 14656800.0 cm-1
2s2 2p4 4f1 2F3.5 14657300.0 cm-1
2s2 2p4 4f1 2F2.5 14659800.0 cm-1
2s2 2p4 4f1 2D1.5 14661000.0 cm-1
2s2 2p4 4d1 4F1.5 14693900.0 cm-1
2s2 2p4 4p1 2F2.5 14703800.0 cm-1
2s2 2p4 4d1 4F2.5 14705500.0 cm-1
2s2 2p4 4p1 2P1.5 14724800.0 cm-1
2s2 2p4 4p1 2F3.5 14726400.0 cm-1
2s2 2p4 4p1 2D1.5 14731000.0 cm-1
2s2 2p4 4p1 2D2.5 14737000.0 cm-1
2s2 2p4 4p1 2P0.5 14768000.0 cm-1
2s2 2p4 4d1 4D0.5 14782400.0 cm-1
2s2 2p4 4f1 4G2.5 14788600.0 cm-1
2s2 2p4 4f1 2G3.5 14792100.0 cm-1
2s2 2p4 4d1 4F3.5 14793200.0 cm-1
2s2 2p4 4d1 4P1.5 14793300.0 cm-1
2s2 2p4 4d1 4P2.5 14803100.0 cm-1
2s2 2p4 4d1 2F2.5 14807000.0 cm-1
2s2 2p4 4d1 2P1.5 14818300.0 cm-1
2s2 2p4 4f1 4F1.5 14884600.0 cm-1
2s2 2p4 4d1 2G3.5 14885000.0 cm-1
2s2 2p4 4f1 4G3.5 14887000.0 cm-1
2s2 2p4 4s1 2S0.5 14888400.0 cm-1
2s2 2p4 4f1 4G4.5 14888500.0 cm-1
2s2 2p4 4f1 4D2.5 14888600.0 cm-1
2s2 2p4 4d1 2G4.5 14890800.0 cm-1
2s2 2p4 4f1 2D2.5 14892600.0 cm-1
2s2 2p4 4f1 4D3.5 14894100.0 cm-1
2s2 2p4 4d1 2D2.5 14899400.0 cm-1
2s2 2p4 4d1 2P1.5 14901400.0 cm-1
2s2 2p4 4d1 2S0.5 14902800.0 cm-1
2s2 2p4 4d1 2F2.5 14905500.0 cm-1
2s2 2p4 4d1 2F3.5 14905700.0 cm-1
2s2 2p4 4d1 2D1.5 14924500.0 cm-1
2s2 2p4 4d1 2P0.5 14934100.0 cm-1
2s2 2p4 4f1 2P0.5 14980200.0 cm-1
2s2 2p4 4f1 2H4.5 14981000.0 cm-1
2s2 2p4 4f1 2P1.5 14982500.0 cm-1
2s2 2p4 4f1 2H5.5 14983900.0 cm-1
2s2 2p4 4f1 2D2.5 14987400.0 cm-1
2s2 2p4 4f1 2D1.5 14988000.0 cm-1
2s2 2p4 4f1 2G3.5 14990600.0 cm-1
2s2 2p4 4f1 2F2.5 14991900.0 cm-1
2s2 2p4 4f1 2F3.5 14993000.0 cm-1
2s2 2p4 4f1 2G4.5 14993700.0 cm-1
2s2 2p4 4p1 2P0.5 15043400.0 cm-1
2s2 2p4 4p1 2P1.5 15055500.0 cm-1
2s2 2p4 4d1 2D2.5 15222500.0 cm-1
2s2 2p4 4d1 2D1.5 15229200.0 cm-1
2s2 2p4 4f1 2F2.5 15311600.0 cm-1
2s2 2p4 4f1 2F3.5 15314100.0 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 = 1.4072
         2S = 1.2125
         2P = 1.1481
         3S = 1.1368
         3P = 1.0869
         3D = 1.1224
         4S = 1.1534
         4P = 1.0999
         4D = 1.1246
         4F = 1.1357

 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, giving a smallest maximum
 basis-orbital energy of 1120.4843 Rydbergs (15245.309386 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.03598787 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 0.901137 Z**2 Rydbergs (6486 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 0.901137 Z**2 Rydbergs (6486 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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  • Allan Whiteford
  • Nigel Badnell
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