Resolved Specific Ion Data Collections

Temperature Range
13.53 eV → 1.353 x 105 eV


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  • Spontaneous Emission: Ge+27(i) → Ge+27(j) + hv
  • Electron Impact Excitation: Ge+27(i) + e → Ge+27(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 288197.0 cm-1
2s1 2p2 4P0.5 562267.0 cm-1
2s1 2p2 4P1.5 725689.0 cm-1
2s1 2p2 4P2.5 837219.0 cm-1
2s1 2p2 2D1.5 1095420.0 cm-1
2s1 2p2 2P0.5 1189850.0 cm-1
2s1 2p2 2D2.5 1200430.0 cm-1
2s1 2p2 2S0.5 1498610.0 cm-1
2s1 2p2 2P1.5 1514740.0 cm-1
2p3 4S1.5 1792640.0 cm-1
2p3 2D1.5 2020650.0 cm-1
2p3 2D2.5 2102020.0 cm-1
2p3 2P0.5 2275140.0 cm-1
2p3 2P1.5 2472410.0 cm-1
2s2 3s1 2S0.5 13025800.0 cm-1
2s2 3p1 2P0.5 13259000.0 cm-1
2s2 3p1 2P1.5 13338400.0 cm-1
2s1 2p1 3s1 4P0.5 13483300.0 cm-1
2s1 2p1 3s1 4P1.5 13544200.0 cm-1
2s2 3d1 2D1.5 13552500.0 cm-1
2s2 3d1 2D2.5 13578900.0 cm-1
2s1 2p1 3s1 2P0.5 13619600.0 cm-1
2s1 2p1 3p1 4D0.5 13687900.0 cm-1
2s1 2p1 3p1 4D1.5 13743500.0 cm-1
2s1 2p1 3s1 4P2.5 13761400.0 cm-1
2s1 2p1 3p1 2P1.5 13809000.0 cm-1
2s1 2p1 3p1 4P0.5 13832600.0 cm-1
2s1 2p1 3p1 2P0.5 13847700.0 cm-1
2s1 2p1 3s1 2P1.5 13847800.0 cm-1
2s1 2p1 3p1 4D2.5 13853500.0 cm-1
2s1 2p1 3p1 2D1.5 13892200.0 cm-1
2s1 2p1 3d1 4F1.5 13964200.0 cm-1
2s1 2p1 3d1 4F2.5 14005800.0 cm-1
2s1 2p1 3p1 4P1.5 14019400.0 cm-1
2s1 2p1 3p1 4P2.5 14041800.0 cm-1
2s1 2p1 3p1 4D3.5 14054300.0 cm-1
2s1 2p1 3d1 4P2.5 14058500.0 cm-1
2s1 2p1 3d1 4F3.5 14071300.0 cm-1
2s1 2p1 3d1 4D1.5 14078800.0 cm-1
2s1 2p1 3p1 4S1.5 14079100.0 cm-1
2s1 2p1 3d1 4D0.5 14083900.0 cm-1
2s1 2p1 3s1 2P0.5 14118000.0 cm-1
2s1 2p1 3s1 2P1.5 14118600.0 cm-1
2s1 2p1 3p1 2D2.5 14141300.0 cm-1
2s1 2p1 3d1 2D1.5 14149900.0 cm-1
2s1 2p1 3d1 2F2.5 14162400.0 cm-1
2s1 2p1 3p1 2S0.5 14167300.0 cm-1
2s1 2p1 3d1 4F4.5 14256100.0 cm-1
2s1 2p1 3d1 4D3.5 14286300.0 cm-1
2s1 2p1 3d1 4D2.5 14291200.0 cm-1
2s1 2p1 3d1 4P1.5 14301300.0 cm-1
2s1 2p1 3d1 4P0.5 14303600.0 cm-1
2p2 3s1 4P0.5 14329500.0 cm-1
2s1 2p1 3d1 2D2.5 14342500.0 cm-1
2s1 2p1 3p1 2P0.5 14359200.0 cm-1
2s1 2p1 3p1 2D1.5 14360800.0 cm-1
2s1 2p1 3d1 2P1.5 14385000.0 cm-1
2s1 2p1 3p1 2D2.5 14415400.0 cm-1
2s1 2p1 3d1 2F3.5 14424300.0 cm-1
2s1 2p1 3p1 2P1.5 14435200.0 cm-1
2s1 2p1 3d1 2P0.5 14446800.0 cm-1
2s1 2p1 3p1 2S0.5 14486100.0 cm-1
2p2 3p1 4D0.5 14526200.0 cm-1
2p2 3s1 4P1.5 14529300.0 cm-1
2p2 3s1 2P0.5 14593400.0 cm-1
2p2 3s1 4P2.5 14608000.0 cm-1
2p2 3p1 4D1.5 14635800.0 cm-1
2s1 2p1 3d1 2F2.5 14638600.0 cm-1
2s1 2p1 3d1 2F3.5 14641100.0 cm-1
2s1 2p1 3d1 2D1.5 14649200.0 cm-1
2p2 3s1 2D1.5 14658000.0 cm-1
2s1 2p1 3d1 2D2.5 14680700.0 cm-1
2s1 2p1 3d1 2P0.5 14687900.0 cm-1
2p2 3p1 2S0.5 14708900.0 cm-1
2s1 2p1 3d1 2P1.5 14713800.0 cm-1
2p2 3p1 4P1.5 14747700.0 cm-1
2p2 3p1 4D2.5 14795000.0 cm-1
2p2 3d1 4F1.5 14799500.0 cm-1
2p2 3p1 4P2.5 14814300.0 cm-1
2p2 3p1 4P0.5 14827800.0 cm-1
2p2 3p1 2D1.5 14853700.0 cm-1
2p2 3d1 2F2.5 14856900.0 cm-1
2p2 3p1 4D3.5 14884500.0 cm-1
2p2 3s1 2D2.5 14886200.0 cm-1
2p2 3p1 4S1.5 14915500.0 cm-1
2p2 3s1 2P1.5 14921100.0 cm-1
2p2 3p1 2P1.5 14935600.0 cm-1
2p2 3p1 2F2.5 14961200.0 cm-1
2p2 3d1 2P1.5 14993900.0 cm-1
2p2 3d1 4F2.5 15002900.0 cm-1
2p2 3d1 4D0.5 15005100.0 cm-1
2p2 3d1 4F3.5 15010800.0 cm-1
2p2 3p1 2P0.5 15021600.0 cm-1
2p2 3d1 4D3.5 15056500.0 cm-1
2p2 3d1 4P2.5 15066500.0 cm-1
2p2 3d1 4D1.5 15066800.0 cm-1
2p2 3d1 4F4.5 15081500.0 cm-1
2p2 3d1 4D2.5 15128900.0 cm-1
2p2 3s1 2S0.5 15139400.0 cm-1
2p2 3p1 2D1.5 15139700.0 cm-1
2p2 3d1 4P1.5 15145700.0 cm-1
2p2 3p1 2D2.5 15148000.0 cm-1
2p2 3p1 2F3.5 15162700.0 cm-1
2p2 3d1 4P0.5 15165200.0 cm-1
2p2 3p1 2D2.5 15166900.0 cm-1
2p2 3p1 2P0.5 15182000.0 cm-1
2p2 3d1 2G3.5 15183800.0 cm-1
2p2 3d1 2P0.5 15196200.0 cm-1
2p2 3d1 2D2.5 15201800.0 cm-1
2p2 3d1 2D1.5 15208600.0 cm-1
2p2 3p1 2P1.5 15324800.0 cm-1
2p2 3d1 2F3.5 15344700.0 cm-1
2p2 3d1 2G4.5 15365800.0 cm-1
2p2 3d1 2D1.5 15388100.0 cm-1
2p2 3d1 2D2.5 15392800.0 cm-1
2p2 3p1 2P0.5 15394700.0 cm-1
2p2 3d1 2P0.5 15399800.0 cm-1
2p2 3d1 2F3.5 15426500.0 cm-1
2p2 3p1 2P1.5 15452300.0 cm-1
2p2 3d1 2S0.5 15469900.0 cm-1
2p2 3d1 2P1.5 15493200.0 cm-1
2p2 3d1 2F2.5 15501400.0 cm-1
2p2 3d1 2D2.5 15665200.0 cm-1
2p2 3d1 2D1.5 15671000.0 cm-1
2s2 4s1 2S0.5 17643600.0 cm-1
2s2 4p1 2P0.5 17740500.0 cm-1
2s2 4p1 2P1.5 17773000.0 cm-1
2s2 4d1 2D1.5 17852400.0 cm-1
2s2 4d1 2D2.5 17863100.0 cm-1
2s2 4f1 2F2.5 17910200.0 cm-1
2s2 4f1 2F3.5 17915400.0 cm-1
2s1 2p1 4s1 4P0.5 18091400.0 cm-1
2s1 2p1 4s1 4P1.5 18148500.0 cm-1
2s1 2p1 4s1 2P0.5 18173000.0 cm-1
2s1 2p1 4p1 4D0.5 18177300.0 cm-1
2s1 2p1 4p1 4D1.5 18219100.0 cm-1
2s1 2p1 4p1 4S1.5 18236800.0 cm-1
2s1 2p1 4p1 4P0.5 18262300.0 cm-1
2s1 2p1 4p1 4D2.5 18278100.0 cm-1
2s1 2p1 4p1 2P0.5 18280400.0 cm-1
2s1 2p1 4d1 4F1.5 18286100.0 cm-1
2s1 2p1 4p1 2D1.5 18290600.0 cm-1
2s1 2p1 4d1 4P2.5 18306300.0 cm-1
2s1 2p1 4d1 4F2.5 18344200.0 cm-1
2s1 2p1 4f1 4G2.5 18348300.0 cm-1
2s1 2p1 4f1 4D3.5 18354100.0 cm-1
2s1 2p1 4d1 4D1.5 18357900.0 cm-1
2s1 2p1 4d1 4D0.5 18362000.0 cm-1
2s1 2p1 4d1 4F3.5 18362700.0 cm-1
2s1 2p1 4s1 4P2.5 18371400.0 cm-1
2s1 2p1 4d1 2D1.5 18381500.0 cm-1
2s1 2p1 4d1 2F2.5 18389300.0 cm-1
2s1 2p1 4s1 2P1.5 18399900.0 cm-1
2s1 2p1 4f1 4F1.5 18406900.0 cm-1
2s1 2p1 4f1 4G3.5 18408300.0 cm-1
2s1 2p1 4f1 4D2.5 18410400.0 cm-1
2s1 2p1 4f1 4G4.5 18412500.0 cm-1
2s1 2p1 4f1 2D2.5 18417500.0 cm-1
2s1 2p1 4f1 2G3.5 18420100.0 cm-1
2s1 2p1 4p1 4P1.5 18474000.0 cm-1
2s1 2p1 4p1 4P2.5 18479200.0 cm-1
2s1 2p1 4p1 4D3.5 18491700.0 cm-1
2s1 2p1 4p1 2P1.5 18503000.0 cm-1
2s1 2p1 4p1 2D2.5 18522200.0 cm-1
2s1 2p1 4p1 2S0.5 18534600.0 cm-1
2s1 2p1 4d1 4F4.5 18572200.0 cm-1
2s1 2p1 4d1 4D3.5 18578600.0 cm-1
2s1 2p1 4d1 4D2.5 18580000.0 cm-1
2s1 2p1 4d1 4P1.5 18584100.0 cm-1
2s1 2p1 4d1 4P0.5 18585400.0 cm-1
2s1 2p1 4d1 2D2.5 18600100.0 cm-1
2s1 2p1 4d1 2P1.5 18612600.0 cm-1
2s1 2p1 4d1 2F3.5 18623800.0 cm-1
2s1 2p1 4f1 4F3.5 18632100.0 cm-1
2s1 2p1 4d1 2P0.5 18633000.0 cm-1
2s1 2p1 4f1 4F4.5 18634300.0 cm-1
2s1 2p1 4f1 4F2.5 18634500.0 cm-1
2s1 2p1 4f1 4D1.5 18639600.0 cm-1
2s1 2p1 4f1 2F3.5 18640300.0 cm-1
2s1 2p1 4f1 4G5.5 18641000.0 cm-1
2s1 2p1 4f1 4D0.5 18643600.0 cm-1
2s1 2p1 4f1 2G4.5 18645300.0 cm-1
2s1 2p1 4f1 2F2.5 18646400.0 cm-1
2s1 2p1 4f1 2D1.5 18654400.0 cm-1
2s1 2p1 4s1 2P0.5 18714600.0 cm-1
2s1 2p1 4s1 2P1.5 18717800.0 cm-1
2s1 2p1 4p1 2D1.5 18810400.0 cm-1
2s1 2p1 4p1 2P0.5 18810900.0 cm-1
2s1 2p1 4p1 2D2.5 18835400.0 cm-1
2s1 2p1 4p1 2P1.5 18844500.0 cm-1
2s1 2p1 4p1 2S0.5 18851300.0 cm-1
2s1 2p1 4d1 2D1.5 18918200.0 cm-1
2s1 2p1 4d1 2F2.5 18920400.0 cm-1
2s1 2p1 4d1 2F3.5 18923500.0 cm-1
2s1 2p1 4d1 2D2.5 18931400.0 cm-1
2s1 2p1 4d1 2P0.5 18934000.0 cm-1
2s1 2p1 4d1 2P1.5 18944900.0 cm-1
2s1 2p1 4f1 2F2.5 18963300.0 cm-1
2s1 2p1 4f1 2F3.5 18968400.0 cm-1
2s1 2p1 4f1 2G3.5 18975900.0 cm-1
2s1 2p1 4f1 2G4.5 18980400.0 cm-1
2s1 2p1 4f1 2D1.5 18983000.0 cm-1
2s1 2p1 4f1 2D2.5 18987800.0 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 = 1.37687
         2S = 1.25275
         2P = 1.17616
         3S = 1.57485
         3P = 1.37703
         3D = 1.48933
         4S = 1.50708
         4P = 1.38854
         4D = 1.53885
         4F = 1.60483

 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 2504.7329 Rydbergs (34079.395837 eV)

 A fine energy mesh of 0.000001 Z**2 Rydbergs (0.009918774 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.918774 eV) was used
 from the last threshold up to 0.842947 Z**2 Rydbergs (8361 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.918774 eV) was used
 from first threshold up to 0.842947 Z**2 Rydbergs (8361 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:        06/07/12

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

 Date:  Wed May 29 10:40:07 2013


  • Guiyun Liang
  • Nigel Badnell
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