Resolved Specific Ion Data Collections

Temperature Range
9.134 eV → 9.134 x 104 eV


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  • Spontaneous Emission: Co+22(i) → Co+22(j) + hv
  • Electron Impact Excitation: Co+22(i) + e → Co+22(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 139290.0 cm-1
2s1 2p2 4P0.5 431562.0 cm-1
2s1 2p2 4P1.5 499270.0 cm-1
2s1 2p2 4P2.5 559760.0 cm-1
2s1 2p2 2D1.5 788520.0 cm-1
2s1 2p2 2D2.5 819149.0 cm-1
2s1 2p2 2P0.5 903309.0 cm-1
2s1 2p2 2S0.5 1050810.0 cm-1
2s1 2p2 2P1.5 1064960.0 cm-1
2p3 4S1.5 1338760.0 cm-1
2p3 2D1.5 1486350.0 cm-1
2p3 2D2.5 1523150.0 cm-1
2p3 2P0.5 1672130.0 cm-1
2p3 2P1.5 1745870.0 cm-1
2s2 3s1 2S0.5 8861000.0 cm-1
2s2 3p1 2P0.5 9050080.0 cm-1
2s2 3p1 2P1.5 9088390.0 cm-1
2s1 2p1 3s1 4P0.5 9235520.0 cm-1
2s2 3d1 2D1.5 9263960.0 cm-1
2s1 2p1 3s1 4P1.5 9270510.0 cm-1
2s2 3d1 2D2.5 9276350.0 cm-1
2s1 2p1 3s1 2P0.5 9340160.0 cm-1
2s1 2p1 3s1 4P2.5 9366460.0 cm-1
2s1 2p1 3p1 4D0.5 9402700.0 cm-1
2s1 2p1 3p1 4D1.5 9434060.0 cm-1
2s1 2p1 3s1 2P1.5 9442370.0 cm-1
2s1 2p1 3p1 2P1.5 9473430.0 cm-1
2s1 2p1 3p1 2P0.5 9486170.0 cm-1
2s1 2p1 3p1 4D2.5 9490600.0 cm-1
2s1 2p1 3p1 4P0.5 9505560.0 cm-1
2s1 2p1 3p1 2D1.5 9530540.0 cm-1
2s1 2p1 3p1 4D3.5 9577390.0 cm-1
2s1 2p1 3p1 4P1.5 9578540.0 cm-1
2s1 2p1 3p1 4P2.5 9597180.0 cm-1
2s1 2p1 3d1 4F1.5 9598050.0 cm-1
2s1 2p1 3p1 4S1.5 9602890.0 cm-1
2s1 2p1 3d1 4F2.5 9620750.0 cm-1
2s1 2p1 3p1 2D2.5 9651830.0 cm-1
2s1 2p1 3d1 4F3.5 9656570.0 cm-1
2s1 2p1 3d1 4P2.5 9665240.0 cm-1
2s1 2p1 3d1 4D1.5 9676070.0 cm-1
2s1 2p1 3s1 2P0.5 9678390.0 cm-1
2s1 2p1 3d1 4D0.5 9680780.0 cm-1
2s1 2p1 3s1 2P1.5 9681890.0 cm-1
2s1 2p1 3p1 2S0.5 9682570.0 cm-1
2s1 2p1 3d1 2D1.5 9716870.0 cm-1
2s1 2p1 3d1 2D2.5 9733670.0 cm-1
2s1 2p1 3d1 4F4.5 9733860.0 cm-1
2s1 2p1 3d1 4D3.5 9765050.0 cm-1
2s1 2p1 3d1 4D2.5 9774900.0 cm-1
2s1 2p1 3d1 4P1.5 9780030.0 cm-1
2s1 2p1 3d1 4P0.5 9782000.0 cm-1
2s1 2p1 3d1 2F2.5 9815480.0 cm-1
2s1 2p1 3d1 2P1.5 9854920.0 cm-1
2s1 2p1 3p1 2P0.5 9866670.0 cm-1
2s1 2p1 3p1 2D1.5 9874220.0 cm-1
2s1 2p1 3d1 2F3.5 9877490.0 cm-1
2s1 2p1 3d1 2P0.5 9893420.0 cm-1
2s1 2p1 3p1 2D2.5 9898180.0 cm-1
2s1 2p1 3p1 2P1.5 9907910.0 cm-1
2p2 3s1 4P0.5 9914280.0 cm-1
2s1 2p1 3p1 2S0.5 9957120.0 cm-1
2p2 3s1 4P1.5 9995700.0 cm-1
2p2 3s1 4P2.5 10048400.0 cm-1
2p2 3s1 2P0.5 10061400.0 cm-1
2p2 3p1 4D0.5 10070100.0 cm-1
2s1 2p1 3d1 2F3.5 10071700.0 cm-1
2s1 2p1 3d1 2F2.5 10073100.0 cm-1
2s1 2p1 3d1 2D1.5 10083800.0 cm-1
2s1 2p1 3d1 2D2.5 10099600.0 cm-1
2p2 3s1 2P1.5 10105200.0 cm-1
2p2 3p1 4D1.5 10119000.0 cm-1
2s1 2p1 3d1 2P0.5 10119500.0 cm-1
2s1 2p1 3d1 2P1.5 10136300.0 cm-1
2p2 3p1 2S0.5 10140500.0 cm-1
2p2 3p1 4P1.5 10177400.0 cm-1
2p2 3p1 4D2.5 10191100.0 cm-1
2p2 3s1 2D2.5 10207600.0 cm-1
2p2 3p1 4P0.5 10208700.0 cm-1
2p2 3p1 4P2.5 10212300.0 cm-1
2p2 3s1 2D1.5 10228800.0 cm-1
2p2 3p1 2D1.5 10230600.0 cm-1
2p2 3p1 4D3.5 10244000.0 cm-1
2p2 3d1 4F1.5 10263400.0 cm-1
2p2 3p1 4S1.5 10290000.0 cm-1
2p2 3d1 4F2.5 10292700.0 cm-1
2p2 3p1 2P1.5 10301400.0 cm-1
2p2 3p1 2D2.5 10304200.0 cm-1
2p2 3p1 2P0.5 10338800.0 cm-1
2p2 3d1 2P1.5 10347700.0 cm-1
2p2 3d1 4F3.5 10349200.0 cm-1
2p2 3d1 4D2.5 10355700.0 cm-1
2p2 3d1 4D0.5 10355700.0 cm-1
2p2 3p1 2F2.5 10388100.0 cm-1
2p2 3d1 4D3.5 10388200.0 cm-1
2p2 3d1 4D1.5 10392500.0 cm-1
2p2 3d1 4F4.5 10394200.0 cm-1
2p2 3d1 2F2.5 10394900.0 cm-1
2p2 3p1 2F3.5 10404500.0 cm-1
2p2 3p1 2D1.5 10420300.0 cm-1
2p2 3s1 2S0.5 10432000.0 cm-1
2p2 3p1 2D2.5 10438800.0 cm-1
2p2 3d1 4P2.5 10441100.0 cm-1
2p2 3p1 2P0.5 10450600.0 cm-1
2p2 3d1 4P1.5 10455600.0 cm-1
2p2 3d1 2P0.5 10462500.0 cm-1
2p2 3d1 4P0.5 10468200.0 cm-1
2p2 3d1 2F3.5 10475100.0 cm-1
2p2 3d1 2D2.5 10512800.0 cm-1
2p2 3d1 2D1.5 10514900.0 cm-1
2p2 3p1 2P1.5 10532200.0 cm-1
2p2 3d1 2G3.5 10540600.0 cm-1
2p2 3d1 2G4.5 10559900.0 cm-1
2p2 3d1 2D1.5 10585400.0 cm-1
2p2 3d1 2D2.5 10591700.0 cm-1
2p2 3d1 2P0.5 10613300.0 cm-1
2p2 3d1 2F3.5 10618700.0 cm-1
2p2 3p1 2P0.5 10630300.0 cm-1
2p2 3p1 2P1.5 10653400.0 cm-1
2p2 3d1 2S0.5 10656500.0 cm-1
2p2 3d1 2F2.5 10661200.0 cm-1
2p2 3d1 2P1.5 10663100.0 cm-1
2p2 3d1 2D2.5 10816700.0 cm-1
2p2 3d1 2D1.5 10825100.0 cm-1
2s2 4s1 2S0.5 12010500.0 cm-1
2s2 4p1 2P0.5 12088600.0 cm-1
2s2 4p1 2P1.5 12104400.0 cm-1
2s2 4d1 2D1.5 12169000.0 cm-1
2s2 4d1 2D2.5 12174000.0 cm-1
2s2 4f1 2F2.5 12211900.0 cm-1
2s2 4f1 2F3.5 12214300.0 cm-1
2s1 2p1 4s1 4P0.5 12379500.0 cm-1
2s1 2p1 4s1 4P1.5 12412200.0 cm-1
2s1 2p1 4s1 2P0.5 12432900.0 cm-1
2s1 2p1 4p1 4D0.5 12449200.0 cm-1
2s1 2p1 4p1 4D1.5 12471800.0 cm-1
2s1 2p1 4p1 4S1.5 12484900.0 cm-1
2s1 2p1 4p1 4P0.5 12502800.0 cm-1
2s1 2p1 4p1 4D2.5 12505000.0 cm-1
2s1 2p1 4p1 2P0.5 12507900.0 cm-1
2s1 2p1 4s1 4P2.5 12510600.0 cm-1
2s1 2p1 4p1 2D1.5 12518200.0 cm-1
2s1 2p1 4d1 4F1.5 12526200.0 cm-1
2s1 2p1 4s1 2P1.5 12535900.0 cm-1
2s1 2p1 4d1 4F2.5 12539200.0 cm-1
2s1 2p1 4d1 4P2.5 12562500.0 cm-1
2s1 2p1 4d1 4F3.5 12569600.0 cm-1
2s1 2p1 4d1 4D1.5 12570600.0 cm-1
2s1 2p1 4d1 4D0.5 12573700.0 cm-1
2s1 2p1 4f1 4G2.5 12574200.0 cm-1
2s1 2p1 4f1 4D3.5 12577200.0 cm-1
2s1 2p1 4d1 2D1.5 12587200.0 cm-1
2s1 2p1 4d1 2F2.5 12594500.0 cm-1
2s1 2p1 4p1 4P1.5 12594900.0 cm-1
2s1 2p1 4p1 4D3.5 12598400.0 cm-1
2s1 2p1 4p1 4P2.5 12598900.0 cm-1
2s1 2p1 4f1 4F1.5 12606800.0 cm-1
2s1 2p1 4p1 2P1.5 12608400.0 cm-1
2s1 2p1 4f1 4G3.5 12608700.0 cm-1
2s1 2p1 4f1 2F2.5 12609300.0 cm-1
2s1 2p1 4f1 4G4.5 12609900.0 cm-1
2s1 2p1 4f1 2D2.5 12615100.0 cm-1
2s1 2p1 4f1 2G3.5 12616800.0 cm-1
2s1 2p1 4p1 2D2.5 12625200.0 cm-1
2s1 2p1 4p1 2S0.5 12636500.0 cm-1
2s1 2p1 4d1 4F4.5 12660200.0 cm-1
2s1 2p1 4d1 4D3.5 12667700.0 cm-1
2s1 2p1 4d1 4D2.5 12670600.0 cm-1
2s1 2p1 4d1 4P1.5 12673600.0 cm-1
2s1 2p1 4d1 4P0.5 12674700.0 cm-1
2s1 2p1 4d1 2D2.5 12684300.0 cm-1
2s1 2p1 4d1 2P1.5 12695700.0 cm-1
2s1 2p1 4d1 2F3.5 12705500.0 cm-1
2s1 2p1 4f1 4F3.5 12709100.0 cm-1
2s1 2p1 4f1 4F4.5 12709700.0 cm-1
2s1 2p1 4f1 4F2.5 12711200.0 cm-1
2s1 2p1 4d1 2P0.5 12711500.0 cm-1
2s1 2p1 4f1 2F3.5 12714200.0 cm-1
2s1 2p1 4f1 4G5.5 12714400.0 cm-1
2s1 2p1 4f1 4D1.5 12715300.0 cm-1
2s1 2p1 4f1 4D0.5 12718400.0 cm-1
2s1 2p1 4f1 2G4.5 12718900.0 cm-1
2s1 2p1 4f1 4D2.5 12719200.0 cm-1
2s1 2p1 4f1 2D1.5 12725500.0 cm-1
2s1 2p1 4s1 2P0.5 12815000.0 cm-1
2s1 2p1 4s1 2P1.5 12816800.0 cm-1
2s1 2p1 4p1 2D1.5 12891300.0 cm-1
2s1 2p1 4p1 2P0.5 12892800.0 cm-1
2s1 2p1 4p1 2D2.5 12902500.0 cm-1
2s1 2p1 4p1 2P1.5 12908500.0 cm-1
2s1 2p1 4p1 2S0.5 12918000.0 cm-1
2s1 2p1 4d1 2D1.5 12969300.0 cm-1
2s1 2p1 4d1 2F2.5 12970100.0 cm-1
2s1 2p1 4d1 2F3.5 12970800.0 cm-1
2s1 2p1 4d1 2D2.5 12975700.0 cm-1
2s1 2p1 4d1 2P0.5 12983600.0 cm-1
2s1 2p1 4d1 2P1.5 12988700.0 cm-1
2s1 2p1 4f1 2F2.5 13001900.0 cm-1
2s1 2p1 4f1 2F3.5 13004300.0 cm-1
2s1 2p1 4f1 2G3.5 13012700.0 cm-1
2s1 2p1 4f1 2G4.5 13014800.0 cm-1
2s1 2p1 4f1 2D1.5 13019200.0 cm-1
2s1 2p1 4f1 2D2.5 13021400.0 cm-1
O+22        27        23      15815200.(  )

        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 = 1.37884
         2S = 1.25183
         2P = 1.17534
         3S = 1.58037
         3P = 1.37421
         3D = 1.48690
         4S = 1.50278
         4P = 1.38487
         4D = 1.53772
         4F = 1.58350

 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 1721.0997 Rydbergs (23417.282518 eV)

 A fine energy mesh of 0.000002 Z**2 Rydbergs (0.013170608 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 0.871030 Z**2 Rydbergs (5736 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 0.871030 Z**2 Rydbergs (5736 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:        25/06/12


  • Guiyun Liang
  • Nigel Badnell
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