Resolved Specific Ion Data Collections

Temperature Range
12.58 eV → 1.258 x 105 eV


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  • Spontaneous Emission: Ga+26(i) → Ga+26(j) + hv
  • Electron Impact Excitation: Ga+26(i) + e → Ga+26(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 251089.0 cm-1
2s1 2p2 4P0.5 532968.0 cm-1
2s1 2p2 4P1.5 671004.0 cm-1
2s1 2p2 4P2.5 772647.0 cm-1
2s1 2p2 2D1.5 1026490.0 cm-1
2s1 2p2 2D2.5 1110430.0 cm-1
2s1 2p2 2P0.5 1126240.0 cm-1
2s1 2p2 2S0.5 1394910.0 cm-1
2s1 2p2 2P1.5 1411170.0 cm-1
2p3 4S1.5 1693010.0 cm-1
2p3 2D1.5 1898720.0 cm-1
2p3 2D2.5 1972060.0 cm-1
2p3 2P0.5 2140310.0 cm-1
2p3 2P1.5 2305640.0 cm-1
2s2 3s1 2S0.5 12125900.0 cm-1
2s2 3p1 2P0.5 12350200.0 cm-1
2s2 3p1 2P1.5 12419600.0 cm-1
2s1 2p1 3s1 4P0.5 12566600.0 cm-1
2s1 2p1 3s1 4P1.5 12621900.0 cm-1
2s2 3d1 2D1.5 12625900.0 cm-1
2s2 3d1 2D2.5 12648800.0 cm-1
2s1 2p1 3s1 2P0.5 12696300.0 cm-1
2s1 2p1 3p1 4D0.5 12763600.0 cm-1
2s1 2p1 3s1 4P2.5 12808400.0 cm-1
2s1 2p1 3p1 4D1.5 12813900.0 cm-1
2s1 2p1 3p1 2P1.5 12873000.0 cm-1
2s1 2p1 3s1 2P1.5 12892800.0 cm-1
2s1 2p1 3p1 4P0.5 12898700.0 cm-1
2s1 2p1 3p1 2P0.5 12906800.0 cm-1
2s1 2p1 3p1 4D2.5 12911300.0 cm-1
2s1 2p1 3p1 2D1.5 12950700.0 cm-1
2s1 2p1 3d1 4F1.5 13021600.0 cm-1
2s1 2p1 3p1 4P1.5 13056900.0 cm-1
2s1 2p1 3d1 4F2.5 13058900.0 cm-1
2s1 2p1 3p1 4P2.5 13078800.0 cm-1
2s1 2p1 3p1 4D3.5 13082900.0 cm-1
2s1 2p1 3p1 4S1.5 13107600.0 cm-1
2s1 2p1 3d1 4P2.5 13109900.0 cm-1
2s1 2p1 3d1 4F3.5 13117700.0 cm-1
2s1 2p1 3d1 4D1.5 13128300.0 cm-1
2s1 2p1 3d1 4D0.5 13133300.0 cm-1
2s1 2p1 3s1 2P0.5 13156500.0 cm-1
2s1 2p1 3s1 2P1.5 13158400.0 cm-1
2s1 2p1 3p1 2D2.5 13167400.0 cm-1
2s1 2p1 3d1 2D1.5 13192300.0 cm-1
2s1 2p1 3p1 2S0.5 13194500.0 cm-1
2s1 2p1 3d1 2F2.5 13207300.0 cm-1
2s1 2p1 3d1 4F4.5 13274900.0 cm-1
2s1 2p1 3d1 4D3.5 13305700.0 cm-1
2s1 2p1 3d1 4D2.5 13311800.0 cm-1
2s1 2p1 3d1 4P1.5 13320900.0 cm-1
2s1 2p1 3d1 4P0.5 13323200.0 cm-1
2s1 2p1 3d1 2D2.5 13359600.0 cm-1
2s1 2p1 3p1 2P0.5 13371200.0 cm-1
2s1 2p1 3p1 2D1.5 13389700.0 cm-1
2p2 3s1 4P0.5 13394800.0 cm-1
2s1 2p1 3d1 2P1.5 13402300.0 cm-1
2s1 2p1 3p1 2D2.5 13436500.0 cm-1
2s1 2p1 3d1 2F3.5 13438500.0 cm-1
2s1 2p1 3p1 2P1.5 13454100.0 cm-1
2s1 2p1 3d1 2P0.5 13459500.0 cm-1
2s1 2p1 3p1 2S0.5 13504500.0 cm-1
2p2 3s1 4P1.5 13548100.0 cm-1
2p2 3p1 4D0.5 13567000.0 cm-1
2p2 3s1 2P0.5 13612600.0 cm-1
2p2 3s1 4P2.5 13621900.0 cm-1
2s1 2p1 3d1 2F2.5 13649800.0 cm-1
2s1 2p1 3d1 2F3.5 13651000.0 cm-1
2s1 2p1 3d1 2D1.5 13658200.0 cm-1
2p2 3p1 4D1.5 13664800.0 cm-1
2p2 3s1 2D1.5 13673100.0 cm-1
2s1 2p1 3d1 2D2.5 13688000.0 cm-1
2s1 2p1 3d1 2P0.5 13698600.0 cm-1
2p2 3p1 2S0.5 13720700.0 cm-1
2s1 2p1 3d1 2P1.5 13721700.0 cm-1
2p2 3p1 4P1.5 13759000.0 cm-1
2p2 3p1 4D2.5 13799900.0 cm-1
2p2 3p1 4P2.5 13817100.0 cm-1
2p2 3d1 4F1.5 13822300.0 cm-1
2p2 3p1 4P0.5 13827400.0 cm-1
2p2 3p1 2D1.5 13852500.0 cm-1
2p2 3s1 2D2.5 13869000.0 cm-1
2p2 3d1 2F2.5 13873300.0 cm-1
2p2 3p1 4D3.5 13880000.0 cm-1
2p2 3s1 2P1.5 13901500.0 cm-1
2p2 3p1 4S1.5 13916200.0 cm-1
2p2 3p1 2P1.5 13932000.0 cm-1
2p2 3p1 2F2.5 13953500.0 cm-1
2p2 3d1 2P1.5 13987800.0 cm-1
2p2 3d1 4F2.5 13996600.0 cm-1
2p2 3d1 4D0.5 13998600.0 cm-1
2p2 3d1 4F3.5 14001200.0 cm-1
2p2 3p1 2P0.5 14009400.0 cm-1
2p2 3d1 4D3.5 14046100.0 cm-1
2p2 3d1 4D1.5 14054700.0 cm-1
2p2 3d1 4P2.5 14055000.0 cm-1
2p2 3d1 4F4.5 14066900.0 cm-1
2p2 3p1 2D2.5 14112100.0 cm-1
2p2 3p1 2D1.5 14113900.0 cm-1
2p2 3d1 4D2.5 14114500.0 cm-1
2p2 3s1 2S0.5 14118500.0 cm-1
2p2 3p1 2F3.5 14127500.0 cm-1
2p2 3d1 4P1.5 14131100.0 cm-1
2p2 3p1 2D2.5 14139800.0 cm-1
2p2 3d1 4P0.5 14147400.0 cm-1
2p2 3p1 2P0.5 14151300.0 cm-1
2p2 3d1 2G3.5 14165700.0 cm-1
2p2 3d1 2P0.5 14172500.0 cm-1
2p2 3d1 2D2.5 14187300.0 cm-1
2p2 3d1 2D1.5 14192600.0 cm-1
2p2 3p1 2P1.5 14283000.0 cm-1
2p2 3d1 2F3.5 14298900.0 cm-1
2p2 3d1 2G4.5 14320300.0 cm-1
2p2 3d1 2D1.5 14343900.0 cm-1
2p2 3d1 2D2.5 14348700.0 cm-1
2p2 3d1 2P0.5 14358400.0 cm-1
2p2 3p1 2P0.5 14360600.0 cm-1
2p2 3d1 2F3.5 14381500.0 cm-1
2p2 3p1 2P1.5 14409400.0 cm-1
2p2 3d1 2S0.5 14423400.0 cm-1
2p2 3d1 2P1.5 14443100.0 cm-1
2p2 3d1 2F2.5 14449400.0 cm-1
2p2 3d1 2D2.5 14611700.0 cm-1
2p2 3d1 2D1.5 14618600.0 cm-1
2s2 4s1 2S0.5 16426600.0 cm-1
2s2 4p1 2P0.5 16519700.0 cm-1
2s2 4p1 2P1.5 16548100.0 cm-1
2s2 4d1 2D1.5 16624500.0 cm-1
2s2 4d1 2D2.5 16633800.0 cm-1
2s2 4f1 2F2.5 16679100.0 cm-1
2s2 4f1 2F3.5 16683500.0 cm-1
2s1 2p1 4s1 4P0.5 16858400.0 cm-1
2s1 2p1 4s1 4P1.5 16910300.0 cm-1
2s1 2p1 4s1 2P0.5 16933900.0 cm-1
2s1 2p1 4p1 4D0.5 16941100.0 cm-1
2s1 2p1 4p1 4D1.5 16978300.0 cm-1
2s1 2p1 4p1 4S1.5 16995400.0 cm-1
2s1 2p1 4p1 4P0.5 17019400.0 cm-1
2s1 2p1 4p1 4D2.5 17031700.0 cm-1
2s1 2p1 4p1 2P0.5 17034100.0 cm-1
2s1 2p1 4d1 4F1.5 17042800.0 cm-1
2s1 2p1 4p1 2D1.5 17044400.0 cm-1
2s1 2p1 4d1 4F2.5 17061000.0 cm-1
2s1 2p1 4d1 4P2.5 17093400.0 cm-1
2s1 2p1 4f1 4G2.5 17101900.0 cm-1
2s1 2p1 4s1 4P2.5 17105300.0 cm-1
2s1 2p1 4f1 4D3.5 17107000.0 cm-1
2s1 2p1 4d1 4D1.5 17108600.0 cm-1
2s1 2p1 4d1 4F3.5 17112000.0 cm-1
2s1 2p1 4d1 4D0.5 17112600.0 cm-1
2s1 2p1 4s1 2P1.5 17129700.0 cm-1
2s1 2p1 4d1 2D1.5 17130700.0 cm-1
2s1 2p1 4d1 2F2.5 17137900.0 cm-1
2s1 2p1 4f1 4F1.5 17154800.0 cm-1
2s1 2p1 4f1 4G3.5 17156300.0 cm-1
2s1 2p1 4f1 4D2.5 17158100.0 cm-1
2s1 2p1 4f1 4G4.5 17159800.0 cm-1
2s1 2p1 4f1 2D2.5 17164900.0 cm-1
2s1 2p1 4f1 2G3.5 17167300.0 cm-1
2s1 2p1 4p1 4P1.5 17200800.0 cm-1
2s1 2p1 4p1 4P2.5 17205700.0 cm-1
2s1 2p1 4p1 4D3.5 17214900.0 cm-1
2s1 2p1 4p1 2P1.5 17225900.0 cm-1
2s1 2p1 4p1 2D2.5 17244600.0 cm-1
2s1 2p1 4p1 2S0.5 17256800.0 cm-1
2s1 2p1 4d1 4F4.5 17291300.0 cm-1
2s1 2p1 4d1 4D3.5 17298100.0 cm-1
2s1 2p1 4d1 4D2.5 17300000.0 cm-1
2s1 2p1 4d1 4P1.5 17303800.0 cm-1
2s1 2p1 4d1 4P0.5 17305100.0 cm-1
2s1 2p1 4d1 2D2.5 17318500.0 cm-1
2s1 2p1 4d1 2P1.5 17330700.0 cm-1
2s1 2p1 4d1 2F3.5 17341900.0 cm-1
2s1 2p1 4f1 4F3.5 17349100.0 cm-1
2s1 2p1 4d1 2P0.5 17350300.0 cm-1
2s1 2p1 4f1 4F4.5 17350900.0 cm-1
2s1 2p1 4f1 4F2.5 17351400.0 cm-1
2s1 2p1 4f1 4D1.5 17356300.0 cm-1
2s1 2p1 4f1 2F3.5 17356500.0 cm-1
2s1 2p1 4f1 4G5.5 17357200.0 cm-1
2s1 2p1 4f1 4D0.5 17360200.0 cm-1
2s1 2p1 4f1 2G4.5 17361500.0 cm-1
2s1 2p1 4f1 2F2.5 17362400.0 cm-1
2s1 2p1 4f1 2D1.5 17370100.0 cm-1
2s1 2p1 4s1 2P0.5 17437700.0 cm-1
2s1 2p1 4s1 2P1.5 17440600.0 cm-1
2s1 2p1 4p1 2D1.5 17529600.0 cm-1
2s1 2p1 4p1 2P0.5 17530300.0 cm-1
2s1 2p1 4p1 2D2.5 17551100.0 cm-1
2s1 2p1 4p1 2P1.5 17559600.0 cm-1
2s1 2p1 4p1 2S0.5 17567600.0 cm-1
2s1 2p1 4d1 2D1.5 17630600.0 cm-1
2s1 2p1 4d1 2F2.5 17632600.0 cm-1
2s1 2p1 4d1 2F3.5 17635000.0 cm-1
2s1 2p1 4d1 2D2.5 17642200.0 cm-1
2s1 2p1 4d1 2P0.5 17646500.0 cm-1
2s1 2p1 4d1 2P1.5 17655800.0 cm-1
2s1 2p1 4f1 2F2.5 17673000.0 cm-1
2s1 2p1 4f1 2F3.5 17677400.0 cm-1
2s1 2p1 4f1 2G3.5 17685200.0 cm-1
2s1 2p1 4f1 2G4.5 17689200.0 cm-1
2s1 2p1 4f1 2D1.5 17692300.0 cm-1
2s1 2p1 4f1 2D2.5 17696400.0 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 = 1.37721
         2S = 1.25259
         2P = 1.17601
         3S = 1.57582
         3P = 1.37649
         3D = 1.48887
         4S = 1.50638
         4P = 1.38789
         4D = 1.53866
         4F = 1.60106

 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 2336.3272 Rydbergs (31788.067883 eV)

 A fine energy mesh of 0.000001 Z**2 Rydbergs (0.009197656 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.197656 eV) was used
 from the last threshold up to 0.845433 Z**2 Rydbergs (7776 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (9.197656 eV) was used
 from first threshold up to 0.845433 Z**2 Rydbergs (7776 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:        05/07/12

 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 10:08:38 2013


  • Guiyun Liang
  • Nigel Badnell
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