Resolved Specific Ion Data Collections

Temperature Range
0.069 eV → 689 eV


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  • Spontaneous Emission: C+1(i) → C+1(j) + hv
  • Electron Impact Excitation: C+1(i) + e → C+1(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 63.4 cm-1
2s1 2p2 4P0.5 43003.3 cm-1
2s1 2p2 4P1.5 43025.2 cm-1
2s1 2p2 4P2.5 43053.6 cm-1
2s1 2p2 2D1.5 74930.1 cm-1
2s1 2p2 2D2.5 74932.6 cm-1
2s1 2p2 2S0.5 96493.7 cm-1
2s1 2p2 2P0.5 110624.0 cm-1
2s1 2p2 2P1.5 110666.0 cm-1
2s2 3s1 2S0.5 142027.0 cm-1
2s2 3p1 2P0.5 142821.0 cm-1
2s2 3p1 2P1.5 150462.0 cm-1
2p3 4S1.5 150467.0 cm-1
2s2 3d1 2D1.5 156375.0 cm-1
2s2 3d1 2D2.5 158612.0 cm-1
2p3 2D1.5 158614.0 cm-1
2p3 2D2.5 161011.0 cm-1
2s2 4s1 2S0.5 161022.0 cm-1
2s2 4p1 2P0.5 165273.0 cm-1
2s2 4p1 2P1.5 165297.0 cm-1
2s1 2p1 3s1 4P0.5 165338.0 cm-1
2s1 2p1 3s1 4P1.5 167607.0 cm-1
2s1 2p1 3s1 4P2.5 167608.0 cm-1
2s2 4d1 2D1.5 168315.0 cm-1
2s2 4d1 2D2.5 168315.0 cm-1
2p3 2P0.5 168730.0 cm-1
2p3 2P1.5 168748.0 cm-1
2s2 4f1 2F2.5 173339.0 cm-1
2s2 4f1 2F3.5 173373.0 cm-1
2s1 2p1 3p1 2P0.5 180055.0 cm-1
2s1 2p1 3p1 2P1.5 180069.0 cm-1
2s1 2p1 3p1 4D0.5 180093.0 cm-1
2s1 2p1 3p1 4D1.5 180127.0 cm-1
2s1 2p1 3p1 4D2.5 180578.0 cm-1
2s1 2p1 3p1 4D3.5 180597.0 cm-1
2s1 2p1 3p1 2P0.5 183170.0 cm-1
2s1 2p1 3p1 2P1.5 184077.0 cm-1
2s1 2p1 3s1 2P1.5 184088.0 cm-1
2s1 2p1 3p1 4P0.5 184199.0 cm-1
2s1 2p1 3p1 4P1.5 184214.0 cm-1
2s1 2p1 3p1 4P2.5 184238.0 cm-1
2s1 2p1 3p1 2D1.5 188327.0 cm-1
2s1 2p1 3p1 2D2.5 188366.0 cm-1
2s1 2p1 3p1 2S0.5 193593.0 cm-1
2s1 2p1 3d1 4F1.5 197226.0 cm-1
2s1 2p1 3d1 4F2.5 197239.0 cm-1
2s1 2p1 3d1 4F3.5 197256.0 cm-1
2s1 2p1 3d1 4F4.5 197280.0 cm-1
2s1 2p1 3d1 4D0.5 198396.0 cm-1
2s1 2p1 3d1 4D1.5 198400.0 cm-1
2s1 2p1 3d1 4D2.5 198407.0 cm-1
2s1 2p1 3d1 4D3.5 198417.0 cm-1
2s1 2p1 3d1 4P2.5 200234.0 cm-1
2s1 2p1 3d1 4P1.5 200252.0 cm-1
2s1 2p1 3d1 4P0.5 200262.0 cm-1
2s1 2p1 3d1 2D1.5 201021.0 cm-1
2s1 2p1 3d1 2D2.5 201031.0 cm-1
2s1 2p1 3d1 2F2.5 203052.0 cm-1
2s1 2p1 3d1 2F3.5 203088.0 cm-1
2s1 2p1 3d1 2P1.5 205985.0 cm-1
2s1 2p1 3d1 2P0.5 206001.0 cm-1
2s1 2p1 4s1 4P0.5 212605.0 cm-1
2s1 2p1 4s1 4P1.5 212628.0 cm-1
2s1 2p1 4s1 4P2.5 212665.0 cm-1
2s1 2p1 4s1 2P0.5 216452.0 cm-1
2s1 2p1 4s1 2P1.5 216490.0 cm-1
2s1 2p1 4p1 2P0.5 217002.0 cm-1
2s1 2p1 4p1 2P1.5 217024.0 cm-1
2s1 2p1 4p1 4D0.5 217612.0 cm-1
2s1 2p1 4p1 4D1.5 217624.0 cm-1
2s1 2p1 4p1 4D2.5 217644.0 cm-1
2s1 2p1 4p1 4D3.5 217673.0 cm-1
2s1 2p1 4p1 4S1.5 218607.0 cm-1
2s1 2p1 4p1 4P0.5 221098.0 cm-1
2s1 2p1 4p1 4P1.5 221110.0 cm-1
2s1 2p1 4p1 4P2.5 221131.0 cm-1
2s1 2p1 4p1 2D1.5 221515.0 cm-1
2s1 2p1 4p1 2D2.5 221551.0 cm-1
2s1 2p1 3s1 2P0.5 222901.0 cm-1
2s1 2p1 3s1 2P1.5 222904.0 cm-1
2s1 2p1 4d1 4F1.5 222960.0 cm-1
2s1 2p1 4d1 4F2.5 222972.0 cm-1
2s1 2p1 4d1 4F3.5 222989.0 cm-1
2s1 2p1 4d1 4F4.5 223013.0 cm-1
2s1 2p1 4d1 4D0.5 223556.0 cm-1
2s1 2p1 4d1 4D1.5 223560.0 cm-1
2s1 2p1 4d1 4D2.5 223566.0 cm-1
2s1 2p1 4d1 4D3.5 223576.0 cm-1
2s1 2p1 4d1 4P2.5 224046.0 cm-1
2s1 2p1 4d1 4P1.5 224064.0 cm-1
2s1 2p1 4d1 4P0.5 224075.0 cm-1
2s1 2p1 4d1 2D1.5 224418.0 cm-1
2s1 2p1 4d1 2D2.5 224429.0 cm-1
2s1 2p1 4f1 2F2.5 224471.0 cm-1
2s1 2p1 4f1 2F3.5 224479.0 cm-1
2s1 2p1 4f1 4F1.5 224483.0 cm-1
2s1 2p1 4f1 4F2.5 224486.0 cm-1
2s1 2p1 4f1 4F3.5 224491.0 cm-1
2s1 2p1 4f1 4F4.5 224496.0 cm-1
2s1 2p1 4p1 2S0.5 225009.0 cm-1
2s1 2p1 4f1 4G2.5 225078.0 cm-1
2s1 2p1 4f1 4G3.5 225090.0 cm-1
2s1 2p1 4f1 4G4.5 225106.0 cm-1
2s1 2p1 4f1 4G5.5 225128.0 cm-1
2s1 2p1 4f1 2G3.5 225181.0 cm-1
2s1 2p1 4f1 4D3.5 225205.0 cm-1
2s1 2p1 4f1 2G4.5 225214.0 cm-1
2s1 2p1 4f1 4D2.5 225221.0 cm-1
2s1 2p1 4f1 4D1.5 225233.0 cm-1
2s1 2p1 4f1 4D0.5 225241.0 cm-1
2s1 2p1 4f1 2D2.5 225276.0 cm-1
2s1 2p1 4f1 2D1.5 225299.0 cm-1
2s1 2p1 4d1 2F2.5 225765.0 cm-1
2s1 2p1 4d1 2F3.5 225801.0 cm-1
2s1 2p1 4d1 2P1.5 227531.0 cm-1
2s1 2p1 4d1 2P0.5 227550.0 cm-1
2s1 2p1 3p1 2P0.5 239401.0 cm-1
2s1 2p1 3p1 2P1.5 239412.0 cm-1
2s1 2p1 3p1 2D1.5 239464.0 cm-1
2s1 2p1 3p1 2D2.5 239469.0 cm-1
2s1 2p1 3p1 2S0.5 244784.0 cm-1
2s1 2p1 3d1 2F3.5 252957.0 cm-1
2s1 2p1 3d1 2F2.5 252957.0 cm-1
2s1 2p1 3d1 2D1.5 253953.0 cm-1
2s1 2p1 3d1 2D2.5 253956.0 cm-1
2p2 3s1 4P0.5 255680.0 cm-1
2p2 3s1 4P1.5 255704.0 cm-1
2p2 3s1 4P2.5 255745.0 cm-1
2s1 2p1 3d1 2P0.5 256682.0 cm-1
2s1 2p1 3d1 2P1.5 256685.0 cm-1
2p2 3s1 2P0.5 264041.0 cm-1
2p2 3s1 2P1.5 264074.0 cm-1
2p2 3p1 2S0.5 266799.0 cm-1
2s1 2p1 4s1 2P0.5 267160.0 cm-1
2s1 2p1 4s1 2P1.5 267160.0 cm-1
2p2 3p1 4D0.5 270237.0 cm-1
2p2 3p1 4D1.5 270251.0 cm-1
2p2 3p1 4D2.5 270275.0 cm-1
2p2 3p1 4D3.5 270308.0 cm-1
2s1 2p1 4p1 2D2.5 271672.0 cm-1
2s1 2p1 4p1 2D1.5 271674.0 cm-1
2p2 3p1 4P0.5 272497.0 cm-1
2p2 3p1 4P1.5 272511.0 cm-1
2p2 3p1 4P2.5 272534.0 cm-1
2s1 2p1 4p1 2S0.5 274792.0 cm-1
2p2 3s1 2D1.5 275339.0 cm-1
2p2 3s1 2D2.5 275345.0 cm-1
2p2 3p1 2D1.5 275506.0 cm-1
2p2 3p1 2D2.5 275541.0 cm-1
2s1 2p1 4p1 2P0.5 276593.0 cm-1
2s1 2p1 4p1 2P1.5 276611.0 cm-1
2s1 2p1 4d1 2F2.5 277504.0 cm-1
2s1 2p1 4d1 2F3.5 277505.0 cm-1
2s1 2p1 4d1 2D1.5 278516.0 cm-1
2s1 2p1 4d1 2D2.5 278522.0 cm-1
2s1 2p1 4f1 2F2.5 278668.0 cm-1
2s1 2p1 4f1 2F3.5 278668.0 cm-1
2s1 2p1 4f1 2G3.5 278686.0 cm-1
2s1 2p1 4f1 2G4.5 278686.0 cm-1
2s1 2p1 4d1 2P0.5 278831.0 cm-1
2s1 2p1 4d1 2P1.5 278834.0 cm-1
2s1 2p1 4f1 2D1.5 279359.0 cm-1
2s1 2p1 4f1 2D2.5 279360.0 cm-1
2p2 3p1 2P1.5 280770.0 cm-1
2p2 3p1 2P0.5 280775.0 cm-1
2p2 3p1 4S1.5 283551.0 cm-1
2p2 3d1 4F1.5 285798.0 cm-1
2p2 3d1 4F2.5 285811.0 cm-1
2p2 3d1 4F3.5 285829.0 cm-1
2p2 3d1 4F4.5 285852.0 cm-1
2p2 3d1 2P1.5 287487.0 cm-1
2p2 3d1 2P0.5 287517.0 cm-1
2p2 3d1 4D0.5 288133.0 cm-1
2p2 3d1 4D1.5 288136.0 cm-1
2p2 3d1 4D2.5 288142.0 cm-1
2p2 3d1 4D3.5 288152.0 cm-1
2p2 3p1 2F2.5 288234.0 cm-1
2p2 3p1 2F3.5 288246.0 cm-1
2p2 3d1 4P2.5 289273.0 cm-1
2p2 3d1 4P1.5 289290.0 cm-1
2p2 3d1 4P0.5 289301.0 cm-1
2p2 3d1 2F2.5 289856.0 cm-1
2p2 3d1 2F3.5 289900.0 cm-1
2p2 3p1 2D1.5 294178.0 cm-1
2p2 3p1 2D2.5 294178.0 cm-1
2p2 3d1 2D1.5 294487.0 cm-1
2p2 3d1 2D2.5 294500.0 cm-1
2p2 3p1 2P0.5 297185.0 cm-1
2p2 3p1 2P1.5 297208.0 cm-1
2p2 3d1 2F3.5 301015.0 cm-1
2p2 3d1 2F2.5 301021.0 cm-1
2p2 3d1 2G3.5 301065.0 cm-1
2p2 3d1 2G4.5 301088.0 cm-1
2p2 3d1 2D1.5 301125.0 cm-1
2p2 3d1 2D2.5 302375.0 cm-1
2p2 3d1 2S0.5 302376.0 cm-1
2p2 3d1 2P0.5 303266.0 cm-1
2p2 3d1 2P1.5 303270.0 cm-1
2p2 3s1 2S0.5 303705.0 cm-1
2p2 3p1 2P0.5 304335.0 cm-1
2p2 3p1 2P1.5 304365.0 cm-1
2p2 3d1 2D2.5 304459.0 cm-1
2p2 3d1 2D1.5 305331.0 cm-1
 + 1         6         2        196674.(  )

        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 = 1.42633
         2S = 1.25671
         2P = 1.19952
         3S = 1.58317
         3P = 1.33938
         3D = 1.25491
         4S = 1.47430
         4P = 1.50168
         4D = 1.41676
         4F = 1.87478

 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 13.9749 Rydbergs (190.142489 eV)

 A fine energy mesh of 0.000100 Z**2 Rydbergs (0.0013606 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.013606 eV) was used
 from the last threshold up to 5.376452 Z**2 Rydbergs (73.152 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.013606 eV) was used
 from first threshold up to 5.376452 Z**2 Rydbergs (73.152 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:        13/08/12

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

 Date:  Mon Jun  3 14:43:49 2013


  • Guiyun Liang
  • Nigel Badnell
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