Resolved Specific Ion Data Collections

Temperature Range
4.412 eV → 4.412 x 104 eV


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  • Spontaneous Emission: Ca+15(i) → Ca+15(j) + hv
  • Electron Impact Excitation: Ca+15(i) + e → Ca+15(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 36179.3 cm-1
2s1 2p2 4P0.5 262735.0 cm-1
2s1 2p2 4P1.5 277173.0 cm-1
2s1 2p2 4P2.5 296635.0 cm-1
2s1 2p2 2D1.5 482411.0 cm-1
2s1 2p2 2D2.5 485396.0 cm-1
2s1 2p2 2S0.5 596818.0 cm-1
2s1 2p2 2P0.5 639125.0 cm-1
2s1 2p2 2P1.5 652423.0 cm-1
2p3 4S1.5 833697.0 cm-1
2p3 2D1.5 945752.0 cm-1
2p3 2D2.5 951789.0 cm-1
2p3 2P0.5 1061500.0 cm-1
2p3 2P1.5 1071330.0 cm-1
2s2 3s1 2S0.5 4403740.0 cm-1
2s2 3p1 2P0.5 4533570.0 cm-1
2s2 3p1 2P1.5 4543700.0 cm-1
2s2 3d1 2D1.5 4666030.0 cm-1
2s1 2p1 3s1 4P0.5 4666630.0 cm-1
2s2 3d1 2D2.5 4669170.0 cm-1
2s1 2p1 3s1 4P1.5 4677730.0 cm-1
2s1 2p1 3s1 4P2.5 4700510.0 cm-1
2s1 2p1 3s1 2P0.5 4733980.0 cm-1
2s1 2p1 3s1 2P1.5 4758920.0 cm-1
2s1 2p1 3p1 4D0.5 4782720.0 cm-1
2s1 2p1 3p1 4D1.5 4792540.0 cm-1
2s1 2p1 3p1 2P0.5 4805450.0 cm-1
2s1 2p1 3p1 2P1.5 4807770.0 cm-1
2s1 2p1 3p1 4D2.5 4808990.0 cm-1
2s1 2p1 3p1 4D3.5 4829250.0 cm-1
2s1 2p1 3p1 4S1.5 4834460.0 cm-1
2s1 2p1 3p1 4P0.5 4838550.0 cm-1
2s1 2p1 3p1 4P1.5 4853730.0 cm-1
2s1 2p1 3p1 4P2.5 4861000.0 cm-1
2s1 2p1 3p1 2D1.5 4863410.0 cm-1
2s1 2p1 3p1 2D2.5 4884950.0 cm-1
2s1 2p1 3d1 4F1.5 4899610.0 cm-1
2s1 2p1 3d1 4F2.5 4906460.0 cm-1
2s1 2p1 3p1 2S0.5 4916470.0 cm-1
2s1 2p1 3d1 4F3.5 4916910.0 cm-1
2s1 2p1 3d1 4F4.5 4933510.0 cm-1
2s1 2p1 3d1 4D2.5 4939460.0 cm-1
2s1 2p1 3s1 2P0.5 4940620.0 cm-1
2s1 2p1 3s1 2P1.5 4941220.0 cm-1
2s1 2p1 3d1 4D1.5 4941910.0 cm-1
2s1 2p1 3d1 4D0.5 4942430.0 cm-1
2s1 2p1 3d1 2D1.5 4953710.0 cm-1
2s1 2p1 3d1 2D2.5 4958380.0 cm-1
2s1 2p1 3d1 4D3.5 4960170.0 cm-1
2s1 2p1 3d1 4P2.5 4969440.0 cm-1
2s1 2p1 3d1 4P1.5 4970810.0 cm-1
2s1 2p1 3d1 4P0.5 4972190.0 cm-1
2s1 2p1 3d1 2F2.5 5014600.0 cm-1
2s1 2p1 3d1 2P1.5 5034430.0 cm-1
2s1 2p1 3d1 2F3.5 5035900.0 cm-1
2s1 2p1 3d1 2P0.5 5046540.0 cm-1
2s1 2p1 3p1 2P0.5 5068590.0 cm-1
2s1 2p1 3p1 2D1.5 5072080.0 cm-1
2s1 2p1 3p1 2D2.5 5078350.0 cm-1
2s1 2p1 3p1 2P1.5 5079590.0 cm-1
2s1 2p1 3p1 2S0.5 5109550.0 cm-1
2p2 3s1 4P0.5 5130670.0 cm-1
2p2 3s1 4P1.5 5143970.0 cm-1
2p2 3s1 4P2.5 5162480.0 cm-1
2s1 2p1 3d1 2F3.5 5191240.0 cm-1
2s1 2p1 3d1 2F2.5 5192010.0 cm-1
2p2 3s1 2P0.5 5203840.0 cm-1
2s1 2p1 3d1 2D1.5 5204370.0 cm-1
2s1 2p1 3d1 2D2.5 5208510.0 cm-1
2p2 3s1 2P1.5 5221550.0 cm-1
2s1 2p1 3d1 2P0.5 5225900.0 cm-1
2s1 2p1 3d1 2P1.5 5230870.0 cm-1
2p2 3p1 2S0.5 5233800.0 cm-1
2p2 3p1 4D0.5 5242140.0 cm-1
2p2 3p1 4D1.5 5247880.0 cm-1
2p2 3s1 2D2.5 5256990.0 cm-1
2p2 3s1 2D1.5 5260890.0 cm-1
2p2 3p1 4D2.5 5261860.0 cm-1
2p2 3p1 4P1.5 5271580.0 cm-1
2p2 3p1 4P0.5 5272500.0 cm-1
2p2 3p1 4D3.5 5279520.0 cm-1
2p2 3p1 4P2.5 5281440.0 cm-1
2p2 3p1 2D1.5 5288880.0 cm-1
2p2 3p1 2D2.5 5313970.0 cm-1
2p2 3p1 2P1.5 5327740.0 cm-1
2p2 3p1 4S1.5 5333970.0 cm-1
2p2 3p1 2P0.5 5334790.0 cm-1
2p2 3d1 4F1.5 5344670.0 cm-1
2p2 3d1 4F2.5 5352030.0 cm-1
2p2 3d1 4F3.5 5363090.0 cm-1
2p2 3p1 2F2.5 5368980.0 cm-1
2p2 3d1 2P1.5 5374390.0 cm-1
2p2 3p1 2F3.5 5376230.0 cm-1
2p2 3d1 4D0.5 5376690.0 cm-1
2p2 3d1 4F4.5 5377320.0 cm-1
2p2 3d1 4D2.5 5380530.0 cm-1
2p2 3d1 4D3.5 5388380.0 cm-1
2p2 3d1 4D1.5 5389610.0 cm-1
2p2 3d1 2F2.5 5393860.0 cm-1
2p2 3d1 2P0.5 5408190.0 cm-1
2p2 3p1 2D1.5 5411850.0 cm-1
2p2 3p1 2D2.5 5415070.0 cm-1
2p2 3d1 2F3.5 5418800.0 cm-1
2p2 3d1 4P2.5 5419690.0 cm-1
2p2 3s1 2S0.5 5422960.0 cm-1
2p2 3d1 4P1.5 5426470.0 cm-1
2p2 3d1 4P0.5 5430440.0 cm-1
2p2 3p1 2P0.5 5436950.0 cm-1
2p2 3p1 2P1.5 5456030.0 cm-1
2p2 3d1 2G3.5 5471080.0 cm-1
2p2 3d1 2G4.5 5475660.0 cm-1
2p2 3d1 2D2.5 5476880.0 cm-1
2p2 3d1 2D1.5 5478610.0 cm-1
2p2 3d1 2D1.5 5500170.0 cm-1
2p2 3d1 2D2.5 5506920.0 cm-1
2p2 3d1 2F3.5 5518750.0 cm-1
2p2 3d1 2F2.5 5529860.0 cm-1
2p2 3d1 2P0.5 5532460.0 cm-1
2p2 3d1 2P1.5 5543850.0 cm-1
2p2 3d1 2S0.5 5550700.0 cm-1
2p2 3p1 2P0.5 5553940.0 cm-1
2p2 3p1 2P1.5 5558550.0 cm-1
2p2 3d1 2D2.5 5663980.0 cm-1
2p2 3d1 2D1.5 5667950.0 cm-1
2s2 4s1 2S0.5 5979410.0 cm-1
2s2 4p1 2P0.5 6032440.0 cm-1
2s2 4p1 2P1.5 6036610.0 cm-1
2s2 4d1 2D1.5 6080800.0 cm-1
2s2 4d1 2D2.5 6082070.0 cm-1
2s2 4f1 2F2.5 6107540.0 cm-1
2s2 4f1 2F3.5 6108110.0 cm-1
2s1 2p1 4s1 4P0.5 6240720.0 cm-1
2s1 2p1 4s1 4P1.5 6250980.0 cm-1
2s1 2p1 4s1 2P0.5 6267720.0 cm-1
2s1 2p1 4s1 4P2.5 6274410.0 cm-1
2s1 2p1 4p1 4D0.5 6288560.0 cm-1
2s1 2p1 4s1 2P1.5 6293210.0 cm-1
2s1 2p1 4p1 4D1.5 6295760.0 cm-1
2s1 2p1 4p1 2P1.5 6303110.0 cm-1
2s1 2p1 4p1 4D2.5 6306120.0 cm-1
2s1 2p1 4p1 2P0.5 6307820.0 cm-1
2s1 2p1 4p1 4P0.5 6312740.0 cm-1
2s1 2p1 4p1 2D1.5 6317880.0 cm-1
2s1 2p1 4p1 4D3.5 6327020.0 cm-1
2s1 2p1 4p1 4P1.5 6332440.0 cm-1
2s1 2p1 4d1 4F1.5 6333720.0 cm-1
2s1 2p1 4p1 4P2.5 6334420.0 cm-1
2s1 2p1 4p1 4S1.5 6335710.0 cm-1
2s1 2p1 4d1 4F2.5 6338680.0 cm-1
2s1 2p1 4d1 4F3.5 6347660.0 cm-1
2s1 2p1 4p1 2D2.5 6347810.0 cm-1
2s1 2p1 4d1 4P2.5 6349440.0 cm-1
2s1 2p1 4d1 4D1.5 6352510.0 cm-1
2s1 2p1 4d1 4D0.5 6353850.0 cm-1
2s1 2p1 4p1 2S0.5 6358930.0 cm-1
2s1 2p1 4d1 2D1.5 6360940.0 cm-1
2s1 2p1 4f1 4G2.5 6365970.0 cm-1
2s1 2p1 4d1 2D2.5 6366540.0 cm-1
2s1 2p1 4f1 4D3.5 6366840.0 cm-1
2s1 2p1 4d1 4F4.5 6367360.0 cm-1
2s1 2p1 4d1 4D3.5 6374190.0 cm-1
2s1 2p1 4f1 4F1.5 6375080.0 cm-1
2s1 2p1 4f1 4F4.5 6376180.0 cm-1
2s1 2p1 4f1 4F2.5 6376310.0 cm-1
2s1 2p1 4f1 4G3.5 6376840.0 cm-1
2s1 2p1 4d1 4D2.5 6377170.0 cm-1
2s1 2p1 4d1 4P1.5 6378800.0 cm-1
2s1 2p1 4d1 4P0.5 6379570.0 cm-1
2s1 2p1 4f1 2F2.5 6380780.0 cm-1
2s1 2p1 4f1 2G3.5 6381030.0 cm-1
2s1 2p1 4d1 2F2.5 6388150.0 cm-1
2s1 2p1 4d1 2P1.5 6396620.0 cm-1
2s1 2p1 4f1 4G4.5 6400430.0 cm-1
2s1 2p1 4f1 4F3.5 6400880.0 cm-1
2s1 2p1 4d1 2F3.5 6401450.0 cm-1
2s1 2p1 4f1 4D2.5 6402730.0 cm-1
2s1 2p1 4f1 4G5.5 6403080.0 cm-1
2s1 2p1 4f1 2F3.5 6403480.0 cm-1
2s1 2p1 4d1 2P0.5 6404710.0 cm-1
2s1 2p1 4f1 4D1.5 6405330.0 cm-1
2s1 2p1 4f1 2G4.5 6406620.0 cm-1
2s1 2p1 4f1 4D0.5 6406980.0 cm-1
2s1 2p1 4f1 2D2.5 6407100.0 cm-1
2s1 2p1 4f1 2D1.5 6410960.0 cm-1
2s1 2p1 4s1 2P0.5 6509650.0 cm-1
2s1 2p1 4s1 2P1.5 6510260.0 cm-1
2s1 2p1 4p1 2D1.5 6560360.0 cm-1
2s1 2p1 4p1 2P0.5 6562410.0 cm-1
2s1 2p1 4p1 2D2.5 6562970.0 cm-1
2s1 2p1 4p1 2P1.5 6566160.0 cm-1
2s1 2p1 4p1 2S0.5 6574490.0 cm-1
2s1 2p1 4d1 2F3.5 6607580.0 cm-1
2s1 2p1 4d1 2F2.5 6607600.0 cm-1
2s1 2p1 4d1 2D1.5 6608440.0 cm-1
2s1 2p1 4d1 2D2.5 6610060.0 cm-1
2s1 2p1 4d1 2P0.5 6618750.0 cm-1
2s1 2p1 4d1 2P1.5 6620070.0 cm-1
2s1 2p1 4f1 2F2.5 6627920.0 cm-1
2s1 2p1 4f1 2F3.5 6628520.0 cm-1
2s1 2p1 4f1 2G3.5 6635710.0 cm-1
2s1 2p1 4f1 2G4.5 6636260.0 cm-1
2s1 2p1 4f1 2D1.5 6640780.0 cm-1
2s1 2p1 4f1 2D2.5 6641300.0 cm-1
A+15        20        16       7853400.(  )

        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 = 1.38338
         2S = 1.24985
         2P = 1.17377
         3S = 1.59276
         3P = 1.36813
         3D = 1.48103
         4S = 1.49080
         4P = 1.37569
         4D = 1.53488
         4F = 1.51727

 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 842.1541 Rydbergs (11458.348685 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.01530675 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.06135 eV) was used
 from the last threshold up to 0.959283 Z**2 Rydbergs (2936.7 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.06135 eV) was used
 from first threshold up to 0.959283 Z**2 Rydbergs (2936.7 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:        21/03/12

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

 Date:  Tue May 28 21:29:46 2013


  • Guiyun Liang
  • Nigel Badnell
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