blike_lgy12#o3.dat

Resolved Specific Ion Data Collections

Ion
O3+
Temperature Range
0.276 eV → 2757 eV

ADF04

Filename
blike_lgy12#o3.dat
Full Path
adf04/copaw#b/blike_lgy12#o3.dat
Download data
  • Spontaneous Emission: O+3(i) → O+3(j) + hv
  • Electron Impact Excitation: O+3(i) + e → O+3(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 385.9 cm-1
2s1 2p2 4P0.5 71439.8 cm-1
2s1 2p2 4P1.5 71570.1 cm-1
2s1 2p2 4P2.5 71755.5 cm-1
2s1 2p2 2D1.5 126936.0 cm-1
2s1 2p2 2D2.5 126950.0 cm-1
2s1 2p2 2S0.5 164366.0 cm-1
2s1 2p2 2P0.5 180481.0 cm-1
2s1 2p2 2P1.5 180724.0 cm-1
2p3 4S1.5 231537.0 cm-1
2p3 2D1.5 255156.0 cm-1
2p3 2D2.5 255185.0 cm-1
2p3 2P0.5 289015.0 cm-1
2p3 2P1.5 289023.0 cm-1
2s2 3s1 2S0.5 354828.0 cm-1
2s2 3p1 2P0.5 387488.0 cm-1
2s2 3p1 2P1.5 387583.0 cm-1
2s2 3d1 2D1.5 417865.0 cm-1
2s2 3d1 2D2.5 417886.0 cm-1
2s1 2p1 3s1 4P0.5 437554.0 cm-1
2s1 2p1 3s1 4P1.5 437691.0 cm-1
2s1 2p1 3s1 4P2.5 437922.0 cm-1
2s1 2p1 3s1 2P0.5 454271.0 cm-1
2s1 2p1 3s1 2P1.5 454525.0 cm-1
2s1 2p1 3p1 2P0.5 465727.0 cm-1
2s1 2p1 3p1 2P1.5 465844.0 cm-1
2s1 2p1 3p1 4D0.5 467219.0 cm-1
2s1 2p1 3p1 4D1.5 467298.0 cm-1
2s1 2p1 3p1 4D2.5 467432.0 cm-1
2s1 2p1 3p1 4D3.5 467628.0 cm-1
2s1 2p1 3p1 4S1.5 473417.0 cm-1
2s1 2p1 3p1 4P0.5 476866.0 cm-1
2s1 2p1 3p1 4P1.5 476959.0 cm-1
2s1 2p1 3p1 4P2.5 477101.0 cm-1
2s1 2p1 3p1 2D1.5 483009.0 cm-1
2s1 2p1 3p1 2D2.5 483238.0 cm-1
2s2 4s1 2S0.5 486106.0 cm-1
2s1 2p1 3p1 2S0.5 495621.0 cm-1
2s1 2p1 3d1 4F1.5 496681.0 cm-1
2s1 2p1 3d1 4F2.5 496756.0 cm-1
2s1 2p1 3d1 4F3.5 496863.0 cm-1
2s1 2p1 3d1 4F4.5 497002.0 cm-1
2s2 4p1 2P0.5 501942.0 cm-1
2s2 4p1 2P1.5 501987.0 cm-1
2s1 2p1 3d1 4D0.5 502346.0 cm-1
2s1 2p1 3d1 4D1.5 502370.0 cm-1
2s1 2p1 3d1 4D2.5 502412.0 cm-1
2s1 2p1 3d1 4D3.5 502476.0 cm-1
2s1 2p1 3d1 2D1.5 504800.0 cm-1
2s1 2p1 3d1 2D2.5 504846.0 cm-1
2s1 2p1 3d1 4P2.5 505682.0 cm-1
2s1 2p1 3d1 4P1.5 505768.0 cm-1
2s1 2p1 3d1 4P0.5 505822.0 cm-1
2s2 4d1 2D1.5 512179.0 cm-1
2s2 4d1 2D2.5 512187.0 cm-1
2s2 4f1 2F2.5 514563.0 cm-1
2s2 4f1 2F3.5 514577.0 cm-1
2s1 2p1 3d1 2F2.5 516636.0 cm-1
2s1 2p1 3d1 2F3.5 516845.0 cm-1
2s1 2p1 3d1 2P1.5 520133.0 cm-1
2s1 2p1 3d1 2P0.5 520266.0 cm-1
2s1 2p1 3s1 2P0.5 524489.0 cm-1
2s1 2p1 3s1 2P1.5 524502.0 cm-1
2s1 2p1 3p1 2D1.5 555275.0 cm-1
2s1 2p1 3p1 2D2.5 555318.0 cm-1
2s1 2p1 3p1 2P0.5 556349.0 cm-1
2s1 2p1 3p1 2P1.5 556421.0 cm-1
2s1 2p1 3p1 2S0.5 563325.0 cm-1
2s1 2p1 4s1 4P0.5 573442.0 cm-1
2s1 2p1 4s1 4P1.5 573569.0 cm-1
2s1 2p1 4s1 4P2.5 573783.0 cm-1
2p2 3s1 4P0.5 578396.0 cm-1
2p2 3s1 4P1.5 578531.0 cm-1
2p2 3s1 4P2.5 578763.0 cm-1
2s1 2p1 4p1 2P0.5 578930.0 cm-1
2s1 2p1 4p1 2P1.5 579101.0 cm-1
2s1 2p1 4s1 2P0.5 580044.0 cm-1
2s1 2p1 4s1 2P1.5 580294.0 cm-1
2s1 2p1 4p1 4D0.5 584783.0 cm-1
2s1 2p1 4p1 4D1.5 584851.0 cm-1
2s1 2p1 3d1 2F2.5 584892.0 cm-1
2s1 2p1 3d1 2F3.5 584904.0 cm-1
2s1 2p1 4p1 4D2.5 584966.0 cm-1
2s1 2p1 4p1 4D3.5 585131.0 cm-1
2s1 2p1 3d1 2D1.5 585993.0 cm-1
2s1 2p1 3d1 2D2.5 586030.0 cm-1
2s1 2p1 4p1 4S1.5 586971.0 cm-1
2s1 2p1 4p1 4P0.5 588836.0 cm-1
2s1 2p1 4p1 4P1.5 588916.0 cm-1
2s1 2p1 4p1 4P2.5 589024.0 cm-1
2s1 2p1 4p1 2D1.5 590221.0 cm-1
2s1 2p1 4p1 2D2.5 590405.0 cm-1
2s1 2p1 3d1 2P0.5 594358.0 cm-1
2s1 2p1 3d1 2P1.5 594387.0 cm-1
2s1 2p1 4d1 4F1.5 594853.0 cm-1
2s1 2p1 4d1 4F2.5 594923.0 cm-1
2s1 2p1 4d1 4F3.5 595026.0 cm-1
2s1 2p1 4d1 4F4.5 595165.0 cm-1
2s1 2p1 4d1 4D0.5 596715.0 cm-1
2s1 2p1 4d1 4D1.5 596736.0 cm-1
2s1 2p1 4d1 4D2.5 596775.0 cm-1
2s1 2p1 4d1 4D3.5 596849.0 cm-1
2s1 2p1 4d1 4P2.5 597864.0 cm-1
2s1 2p1 4d1 4P1.5 597961.0 cm-1
2s1 2p1 4d1 4P0.5 598015.0 cm-1
2s1 2p1 4f1 4F1.5 598579.0 cm-1
2s1 2p1 4f1 4F2.5 598593.0 cm-1
2s1 2p1 4f1 4F3.5 598620.0 cm-1
2s1 2p1 4f1 2F2.5 598643.0 cm-1
2s1 2p1 4f1 4F4.5 598670.0 cm-1
2s1 2p1 4f1 2F3.5 598703.0 cm-1
2s1 2p1 4p1 2S0.5 599170.0 cm-1
2p2 3p1 2S0.5 599461.0 cm-1
2s1 2p1 4d1 2D1.5 600069.0 cm-1
2s1 2p1 4d1 2D2.5 600131.0 cm-1
2s1 2p1 4f1 4D3.5 601251.0 cm-1
2s1 2p1 4f1 4D2.5 601338.0 cm-1
2s1 2p1 4f1 4D1.5 601405.0 cm-1
2s1 2p1 4f1 4D0.5 601445.0 cm-1
2s1 2p1 4f1 4G2.5 601526.0 cm-1
2s1 2p1 4f1 4G3.5 601595.0 cm-1
2s1 2p1 4f1 4G4.5 601693.0 cm-1
2s1 2p1 4f1 4G5.5 601816.0 cm-1
2s1 2p1 4f1 2D2.5 601844.0 cm-1
2s1 2p1 4f1 2D1.5 601976.0 cm-1
2s1 2p1 4f1 2G3.5 602121.0 cm-1
2s1 2p1 4f1 2G4.5 602312.0 cm-1
2p2 3s1 2P0.5 603559.0 cm-1
2s1 2p1 4d1 2F2.5 603647.0 cm-1
2p2 3s1 2P1.5 603761.0 cm-1
2s1 2p1 4d1 2F3.5 603840.0 cm-1
2s1 2p1 4d1 2P1.5 604716.0 cm-1
2s1 2p1 4d1 2P0.5 604843.0 cm-1
2p2 3p1 4D0.5 606004.0 cm-1
2p2 3p1 4D1.5 606084.0 cm-1
2p2 3p1 4D2.5 606219.0 cm-1
2p2 3p1 4D3.5 606407.0 cm-1
2p2 3s1 2D1.5 610432.0 cm-1
2p2 3s1 2D2.5 610455.0 cm-1
2p2 3p1 4P0.5 610478.0 cm-1
2p2 3p1 4P1.5 610558.0 cm-1
2p2 3p1 4P2.5 610693.0 cm-1
2p2 3p1 2D1.5 615446.0 cm-1
2p2 3p1 2D2.5 615680.0 cm-1
2p2 3p1 2P1.5 624279.0 cm-1
2p2 3p1 2P0.5 624307.0 cm-1
2p2 3p1 4S1.5 627969.0 cm-1
2p2 3d1 4F1.5 633789.0 cm-1
2p2 3d1 4F2.5 633862.0 cm-1
2p2 3d1 4F3.5 633964.0 cm-1
2p2 3d1 4F4.5 634098.0 cm-1
2p2 3p1 2F2.5 636346.0 cm-1
2p2 3p1 2F3.5 636425.0 cm-1
2p2 3d1 2P1.5 637503.0 cm-1
2p2 3d1 2P0.5 637703.0 cm-1
2p2 3d1 4D0.5 638889.0 cm-1
2p2 3d1 4D1.5 638905.0 cm-1
2p2 3d1 4D2.5 638938.0 cm-1
2p2 3d1 4D3.5 638992.0 cm-1
2p2 3d1 2F2.5 642308.0 cm-1
2p2 3d1 2F3.5 642554.0 cm-1
2p2 3d1 4P2.5 643585.0 cm-1
2p2 3d1 4P1.5 643680.0 cm-1
2p2 3d1 4P0.5 643736.0 cm-1
2p2 3p1 2D2.5 649220.0 cm-1
2p2 3p1 2D1.5 649235.0 cm-1
2s1 2p1 4s1 2P0.5 651100.0 cm-1
2s1 2p1 4s1 2P1.5 651174.0 cm-1
2p2 3d1 2G3.5 657194.0 cm-1
2p2 3d1 2G4.5 657206.0 cm-1
2p2 3d1 2D1.5 658215.0 cm-1
2p2 3d1 2D2.5 658241.0 cm-1
2p2 3s1 2S0.5 660509.0 cm-1
2p2 3d1 2F3.5 664318.0 cm-1
2p2 3d1 2F2.5 664348.0 cm-1
2p2 3d1 2D1.5 664744.0 cm-1
2p2 3p1 2P0.5 664791.0 cm-1
2p2 3d1 2D2.5 664833.0 cm-1
2p2 3p1 2P1.5 664872.0 cm-1
2s1 2p1 4p1 2P0.5 667777.0 cm-1
2s1 2p1 4p1 2P1.5 667829.0 cm-1
2s1 2p1 4p1 2S0.5 669190.0 cm-1
2s1 2p1 4p1 2D1.5 670994.0 cm-1
2s1 2p1 4p1 2D2.5 671025.0 cm-1
2p2 3d1 2P0.5 677206.0 cm-1
2p2 3d1 2P1.5 677269.0 cm-1
2s1 2p1 4d1 2F3.5 679929.0 cm-1
2s1 2p1 4d1 2F2.5 679931.0 cm-1
2s1 2p1 4d1 2D1.5 680567.0 cm-1
2s1 2p1 4d1 2D2.5 680578.0 cm-1
2s1 2p1 4d1 2P0.5 682794.0 cm-1
2s1 2p1 4d1 2P1.5 682805.0 cm-1
2s1 2p1 4f1 2D1.5 683020.0 cm-1
2s1 2p1 4f1 2D2.5 683022.0 cm-1
2s1 2p1 4f1 2F2.5 684812.0 cm-1
2s1 2p1 4f1 2F3.5 684813.0 cm-1
2p2 3d1 2S0.5 685752.0 cm-1
2s1 2p1 4f1 2G3.5 688385.0 cm-1
2s1 2p1 4f1 2G4.5 688392.0 cm-1
2p2 3p1 2P0.5 695581.0 cm-1
2p2 3p1 2P1.5 695626.0 cm-1
2p2 3d1 2D2.5 709645.0 cm-1
2p2 3d1 2D1.5 709858.0 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
    AUTOSTRUCTURE.

     Calculation details
     +++++++++++++++++++

 The following scaling parameters on bound orbitals were used:

         1S = 1.41103
         2S = 1.24220
         2P = 1.17671
         3S = 1.64434
         3P = 1.34306
         3D = 1.41337
         4S = 1.68623
         4P = 1.29607
         4D = 1.48413
         4F = 2.30820

 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 55.7862 Rydbergs (759.027037 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00122454 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.122454 eV) was used
 from the last threshold up to 1.896565 Z**2 Rydbergs (232.242 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.122454 eV) was used
 from first threshold up to 1.896565 Z**2 Rydbergs (232.242 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

 See:
      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:        18/06/12

 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 19:20:33 2013
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Contributors

  • Guiyun Liang
  • Nigel Badnell
  • Processes
  • States
  • Comments
  • Origins

Data Classes