Resolved Specific Ion Data Collections

Temperature Range
3.378 eV → 3.378 x 104 eV


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  • Spontaneous Emission: Ar+13(i) → Ar+13(j) + hv
  • Electron Impact Excitation: Ar+13(i) + e → Ar+13(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 22407.4 cm-1
2s1 2p2 4P0.5 224823.0 cm-1
2s1 2p2 4P1.5 233401.0 cm-1
2s1 2p2 4P2.5 245706.0 cm-1
2s1 2p2 2D1.5 413607.0 cm-1
2s1 2p2 2D2.5 414903.0 cm-1
2s1 2p2 2S0.5 519297.0 cm-1
2s1 2p2 2P0.5 551534.0 cm-1
2s1 2p2 2P1.5 561983.0 cm-1
2p3 4S1.5 717780.0 cm-1
2p3 2D1.5 817586.0 cm-1
2p3 2D2.5 820329.0 cm-1
2p3 2P0.5 918439.0 cm-1
2p3 2P1.5 923073.0 cm-1
2s2 3s1 2S0.5 3417360.0 cm-1
2s2 3p1 2P0.5 3530740.0 cm-1
2s2 3p1 2P1.5 3537000.0 cm-1
2s2 3d1 2D1.5 3644120.0 cm-1
2s2 3d1 2D2.5 3646020.0 cm-1
2s1 2p1 3s1 4P0.5 3649360.0 cm-1
2s1 2p1 3s1 4P1.5 3656480.0 cm-1
2s1 2p1 3s1 4P2.5 3670270.0 cm-1
2s1 2p1 3s1 2P0.5 3707520.0 cm-1
2s1 2p1 3s1 2P1.5 3722740.0 cm-1
2s1 2p1 3p1 4D0.5 3750880.0 cm-1
2s1 2p1 3p1 4D1.5 3757280.0 cm-1
2s1 2p1 3p1 2P0.5 3764540.0 cm-1
2s1 2p1 3p1 2P1.5 3766880.0 cm-1
2s1 2p1 3p1 4D2.5 3767910.0 cm-1
2s1 2p1 3p1 4D3.5 3780140.0 cm-1
2s1 2p1 3p1 4S1.5 3789170.0 cm-1
2s1 2p1 3p1 4P0.5 3796730.0 cm-1
2s1 2p1 3p1 4P1.5 3805110.0 cm-1
2s1 2p1 3p1 4P2.5 3810490.0 cm-1
2s1 2p1 3p1 2D1.5 3816280.0 cm-1
2s1 2p1 3p1 2D2.5 3829960.0 cm-1
2s1 2p1 3d1 4F1.5 3850450.0 cm-1
2s1 2p1 3d1 4F2.5 3854790.0 cm-1
2s1 2p1 3p1 2S0.5 3859660.0 cm-1
2s1 2p1 3d1 4F3.5 3861310.0 cm-1
2s1 2p1 3d1 4F4.5 3871050.0 cm-1
2s1 2p1 3d1 4D2.5 3884020.0 cm-1
2s1 2p1 3d1 4D1.5 3884740.0 cm-1
2s1 2p1 3d1 4D0.5 3884880.0 cm-1
2s1 2p1 3s1 2P0.5 3887120.0 cm-1
2s1 2p1 3s1 2P1.5 3887480.0 cm-1
2s1 2p1 3d1 2D1.5 3892700.0 cm-1
2s1 2p1 3d1 2D2.5 3895090.0 cm-1
2s1 2p1 3d1 4D3.5 3895270.0 cm-1
2s1 2p1 3d1 4P2.5 3903260.0 cm-1
2s1 2p1 3d1 4P1.5 3904450.0 cm-1
2s1 2p1 3d1 4P0.5 3905600.0 cm-1
2s1 2p1 3d1 2F2.5 3947060.0 cm-1
2s1 2p1 3d1 2F3.5 3960460.0 cm-1
2s1 2p1 3d1 2P1.5 3962380.0 cm-1
2s1 2p1 3d1 2P0.5 3970000.0 cm-1
2s1 2p1 3p1 2P0.5 3998370.0 cm-1
2s1 2p1 3p1 2P1.5 4001030.0 cm-1
2s1 2p1 3p1 2D2.5 4005220.0 cm-1
2s1 2p1 3p1 2D1.5 4005480.0 cm-1
2s1 2p1 3p1 2S0.5 4032870.0 cm-1
2p2 3s1 4P0.5 4054030.0 cm-1
2p2 3s1 4P1.5 4062160.0 cm-1
2p2 3s1 4P2.5 4074110.0 cm-1
2s1 2p1 3d1 2F3.5 4102570.0 cm-1
2s1 2p1 3d1 2F2.5 4103040.0 cm-1
2s1 2p1 3d1 2D1.5 4115140.0 cm-1
2p2 3s1 2P0.5 4117440.0 cm-1
2s1 2p1 3d1 2D2.5 4117680.0 cm-1
2p2 3s1 2P1.5 4129540.0 cm-1
2s1 2p1 3d1 2P0.5 4135020.0 cm-1
2s1 2p1 3d1 2P1.5 4137690.0 cm-1
2p2 3p1 2S0.5 4140800.0 cm-1
2p2 3p1 4D0.5 4149310.0 cm-1
2p2 3p1 4D1.5 4153900.0 cm-1
2p2 3s1 2D2.5 4157980.0 cm-1
2p2 3s1 2D1.5 4159620.0 cm-1
2p2 3p1 4D2.5 4162370.0 cm-1
2p2 3p1 4P0.5 4172030.0 cm-1
2p2 3p1 4P1.5 4173030.0 cm-1
2p2 3p1 4D3.5 4173590.0 cm-1
2p2 3p1 4P2.5 4179300.0 cm-1
2p2 3p1 2D1.5 4186880.0 cm-1
2p2 3p1 2D2.5 4202500.0 cm-1
2p2 3p1 2P1.5 4219310.0 cm-1
2p2 3p1 2P0.5 4222650.0 cm-1
2p2 3p1 4S1.5 4224840.0 cm-1
2p2 3d1 4F1.5 4238270.0 cm-1
2p2 3d1 4F2.5 4242750.0 cm-1
2p2 3d1 4F3.5 4249370.0 cm-1
2p2 3p1 2F2.5 4255050.0 cm-1
2p2 3d1 4F4.5 4258200.0 cm-1
2p2 3p1 2F3.5 4259680.0 cm-1
2p2 3d1 2P1.5 4262090.0 cm-1
2p2 3d1 4D0.5 4263250.0 cm-1
2p2 3d1 4D2.5 4266850.0 cm-1
2p2 3d1 4D3.5 4271030.0 cm-1
2p2 3d1 4D1.5 4271810.0 cm-1
2p2 3d1 2F2.5 4276370.0 cm-1
2p2 3d1 2P0.5 4283360.0 cm-1
2p2 3d1 2F3.5 4292040.0 cm-1
2p2 3p1 2D1.5 4294160.0 cm-1
2p2 3p1 2D2.5 4295420.0 cm-1
2p2 3d1 4P2.5 4297920.0 cm-1
2p2 3d1 4P1.5 4302530.0 cm-1
2p2 3d1 4P0.5 4303990.0 cm-1
2p2 3s1 2S0.5 4306700.0 cm-1
2p2 3p1 2P0.5 4317020.0 cm-1
2p2 3p1 2P1.5 4327960.0 cm-1
2p2 3d1 2G3.5 4342510.0 cm-1
2p2 3d1 2G4.5 4344970.0 cm-1
2p2 3d1 2D2.5 4348260.0 cm-1
2p2 3d1 2D1.5 4349330.0 cm-1
2p2 3d1 2D1.5 4368530.0 cm-1
2p2 3d1 2D2.5 4373630.0 cm-1
2p2 3d1 2F3.5 4382040.0 cm-1
2p2 3d1 2F2.5 4388360.0 cm-1
2p2 3d1 2P0.5 4397240.0 cm-1
2p2 3d1 2P1.5 4403860.0 cm-1
2p2 3d1 2S0.5 4411940.0 cm-1
2p2 3p1 2P0.5 4419300.0 cm-1
2p2 3p1 2P1.5 4421990.0 cm-1
2p2 3d1 2D2.5 4512480.0 cm-1
2p2 3d1 2D1.5 4515070.0 cm-1
2s2 4s1 2S0.5 4644020.0 cm-1
2s2 4p1 2P0.5 4690070.0 cm-1
2s2 4p1 2P1.5 4692640.0 cm-1
2s2 4d1 2D1.5 4730990.0 cm-1
2s2 4d1 2D2.5 4731750.0 cm-1
2s2 4f1 2F2.5 4753820.0 cm-1
2s2 4f1 2F3.5 4754160.0 cm-1
2s1 2p1 4s1 4P0.5 4875010.0 cm-1
2s1 2p1 4s1 4P1.5 4881610.0 cm-1
2s1 2p1 4s1 4P2.5 4895660.0 cm-1
2s1 2p1 4s1 2P0.5 4897300.0 cm-1
2s1 2p1 4s1 2P1.5 4912820.0 cm-1
2s1 2p1 4p1 4D0.5 4916750.0 cm-1
2s1 2p1 4p1 4D1.5 4921340.0 cm-1
2s1 2p1 4p1 2P1.5 4927690.0 cm-1
2s1 2p1 4p1 4D2.5 4928060.0 cm-1
2s1 2p1 4p1 2P0.5 4929740.0 cm-1
2s1 2p1 4p1 4P0.5 4935190.0 cm-1
2s1 2p1 4p1 4S1.5 4938050.0 cm-1
2s1 2p1 4p1 4D3.5 4940290.0 cm-1
2s1 2p1 4p1 4P1.5 4946710.0 cm-1
2s1 2p1 4p1 4P2.5 4948060.0 cm-1
2s1 2p1 4p1 2D1.5 4949590.0 cm-1
2s1 2p1 4d1 4F1.5 4954710.0 cm-1
2s1 2p1 4d1 4F2.5 4958070.0 cm-1
2s1 2p1 4p1 2D2.5 4959350.0 cm-1
2s1 2p1 4d1 4F3.5 4963770.0 cm-1
2s1 2p1 4d1 4P2.5 4967140.0 cm-1
2s1 2p1 4d1 4D1.5 4969020.0 cm-1
2s1 2p1 4d1 4D0.5 4969860.0 cm-1
2s1 2p1 4p1 2S0.5 4970190.0 cm-1
2s1 2p1 4d1 4F4.5 4975120.0 cm-1
2s1 2p1 4d1 2D1.5 4975280.0 cm-1
2s1 2p1 4d1 2D2.5 4979320.0 cm-1
2s1 2p1 4d1 4D3.5 4981510.0 cm-1
2s1 2p1 4f1 4G2.5 4982780.0 cm-1
2s1 2p1 4f1 4F3.5 4983340.0 cm-1
2s1 2p1 4d1 4D2.5 4984260.0 cm-1
2s1 2p1 4d1 4P1.5 4985450.0 cm-1
2s1 2p1 4d1 4P0.5 4986100.0 cm-1
2s1 2p1 4f1 4F1.5 4988140.0 cm-1
2s1 2p1 4f1 4F4.5 4988970.0 cm-1
2s1 2p1 4f1 4F2.5 4989250.0 cm-1
2s1 2p1 4f1 2F3.5 4989900.0 cm-1
2s1 2p1 4f1 2F2.5 4992990.0 cm-1
2s1 2p1 4f1 2G3.5 4993120.0 cm-1
2s1 2p1 4d1 2F2.5 4995790.0 cm-1
2s1 2p1 4d1 2P1.5 5002530.0 cm-1
2s1 2p1 4f1 4G4.5 5003760.0 cm-1
2s1 2p1 4f1 4G3.5 5004380.0 cm-1
2s1 2p1 4d1 2F3.5 5005560.0 cm-1
2s1 2p1 4f1 4G5.5 5005850.0 cm-1
2s1 2p1 4f1 4D2.5 5006130.0 cm-1
2s1 2p1 4f1 4D3.5 5006470.0 cm-1
2s1 2p1 4f1 4D1.5 5008220.0 cm-1
2s1 2p1 4d1 2P0.5 5008320.0 cm-1
2s1 2p1 4f1 2G4.5 5008930.0 cm-1
2s1 2p1 4f1 4D0.5 5009470.0 cm-1
2s1 2p1 4f1 2D2.5 5009760.0 cm-1
2s1 2p1 4f1 2D1.5 5012880.0 cm-1
2s1 2p1 4s1 2P0.5 5108360.0 cm-1
2s1 2p1 4s1 2P1.5 5108760.0 cm-1
2s1 2p1 4p1 2D1.5 5152110.0 cm-1
2s1 2p1 4p1 2D2.5 5153650.0 cm-1
2s1 2p1 4p1 2P0.5 5154150.0 cm-1
2s1 2p1 4p1 2P1.5 5156370.0 cm-1
2s1 2p1 4p1 2S0.5 5163970.0 cm-1
2s1 2p1 4d1 2F3.5 5192110.0 cm-1
2s1 2p1 4d1 2F2.5 5192150.0 cm-1
2s1 2p1 4d1 2D1.5 5193210.0 cm-1
2s1 2p1 4d1 2D2.5 5194190.0 cm-1
2s1 2p1 4d1 2P0.5 5202250.0 cm-1
2s1 2p1 4d1 2P1.5 5203050.0 cm-1
2s1 2p1 4f1 2F2.5 5209600.0 cm-1
2s1 2p1 4f1 2F3.5 5209960.0 cm-1
2s1 2p1 4f1 2G3.5 5216470.0 cm-1
2s1 2p1 4f1 2G4.5 5216810.0 cm-1
2s1 2p1 4f1 2D1.5 5221090.0 cm-1
2s1 2p1 4f1 2D2.5 5221400.0 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 = 1.38536
         2S = 1.24902
         2P = 1.17321
         3S = 1.59800
         3P = 1.36562
         3D = 1.47826
         4S = 1.48396
         4P = 1.37121
         4D = 1.53345
         4F = 1.47479

 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 647.0784 Rydbergs (8804.148710 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.01149707 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.299414 eV) was used
 from the last threshold up to 0.985295 Z**2 Rydbergs (2265.601275 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.299414 eV) was used
 from first threshold up to 0.985295 Z**2 Rydbergs (2265.601275 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:        20/01/12


  • Guiyun Liang
  • Nigel Badnell
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