Resolved Specific Ion Data Collections

Temperature Range
2.912 eV → 2.912 x 104 eV


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  • Spontaneous Emission: Cl+12(i) → Cl+12(j) + hv
  • Electron Impact Excitation: Cl+12(i) + e → Cl+12(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 17409.8 cm-1
2s1 2p2 4P0.5 211270.0 cm-1
2s1 2p2 4P1.5 217740.0 cm-1
2s1 2p2 4P2.5 226610.0 cm-1
2s1 2p2 2D1.5 377770.0 cm-1
2s1 2p2 2D2.5 378309.0 cm-1
2s1 2p2 2S0.5 476620.0 cm-1
2s1 2p2 2P0.5 504100.0 cm-1
2s1 2p2 2P1.5 512199.0 cm-1
2p3 4S1.5 663040.0 cm-1
2p3 2D1.5 749520.0 cm-1
2p3 2D2.5 750580.0 cm-1
2p3 2P0.5 840270.0 cm-1
2p3 2P1.5 843080.0 cm-1
2s2 3s1 2S0.5 2971330.0 cm-1
2s2 3p1 2P0.5 3076570.0 cm-1
2s2 3p1 2P1.5 3081360.0 cm-1
2s2 3d1 2D1.5 3180870.0 cm-1
2s2 3d1 2D2.5 3182310.0 cm-1
2s1 2p1 3s1 4P0.5 3188050.0 cm-1
2s1 2p1 3s1 4P1.5 3193610.0 cm-1
2s1 2p1 3s1 4P2.5 3204110.0 cm-1
2s1 2p1 3s1 2P0.5 3241800.0 cm-1
2s1 2p1 3s1 2P1.5 3253440.0 cm-1
2s1 2p1 3p1 4D0.5 3282270.0 cm-1
2s1 2p1 3p1 4D1.5 3287330.0 cm-1
2s1 2p1 3p1 2P0.5 3292550.0 cm-1
2s1 2p1 3p1 2P1.5 3294580.0 cm-1
2s1 2p1 3p1 4D2.5 3295770.0 cm-1
2s1 2p1 3p1 4D3.5 3305070.0 cm-1
2s1 2p1 3p1 4S1.5 3315220.0 cm-1
2s1 2p1 3p1 4P0.5 3323660.0 cm-1
2s1 2p1 3p1 4P1.5 3329710.0 cm-1
2s1 2p1 3p1 4P2.5 3334200.0 cm-1
2s1 2p1 3p1 2D1.5 3341260.0 cm-1
2s1 2p1 3p1 2D2.5 3351820.0 cm-1
2s1 2p1 3d1 4F1.5 3373800.0 cm-1
2s1 2p1 3d1 4F2.5 3377170.0 cm-1
2s1 2p1 3p1 2S0.5 3380290.0 cm-1
2s1 2p1 3d1 4F3.5 3382190.0 cm-1
2s1 2p1 3d1 4F4.5 3389490.0 cm-1
2s1 2p1 3d1 4D2.5 3404370.0 cm-1
2s1 2p1 3d1 4D0.5 3404590.0 cm-1
2s1 2p1 3d1 4D1.5 3404600.0 cm-1
2s1 2p1 3s1 2P0.5 3408790.0 cm-1
2s1 2p1 3s1 2P1.5 3408870.0 cm-1
2s1 2p1 3d1 2D1.5 3411200.0 cm-1
2s1 2p1 3d1 4D3.5 3412290.0 cm-1
2s1 2p1 3d1 2D2.5 3412660.0 cm-1
2s1 2p1 3d1 4P2.5 3419670.0 cm-1
2s1 2p1 3d1 4P1.5 3420780.0 cm-1
2s1 2p1 3d1 4P0.5 3421800.0 cm-1
2s1 2p1 3d1 2F2.5 3461910.0 cm-1
2s1 2p1 3d1 2F3.5 3472250.0 cm-1
2s1 2p1 3d1 2P1.5 3475370.0 cm-1
2s1 2p1 3d1 2P0.5 3481260.0 cm-1
2s1 2p1 3p1 2P0.5 3511930.0 cm-1
2s1 2p1 3p1 2P1.5 3514180.0 cm-1
2s1 2p1 3p1 2D1.5 3517600.0 cm-1
2s1 2p1 3p1 2D2.5 3517610.0 cm-1
2s1 2p1 3p1 2S0.5 3543260.0 cm-1
2p2 3s1 4P0.5 3564240.0 cm-1
2p2 3s1 4P1.5 3570440.0 cm-1
2p2 3s1 4P2.5 3579780.0 cm-1
2s1 2p1 3d1 2F3.5 3607420.0 cm-1
2s1 2p1 3d1 2F2.5 3607760.0 cm-1
2s1 2p1 3d1 2D1.5 3619600.0 cm-1
2s1 2p1 3d1 2D2.5 3621540.0 cm-1
2p2 3s1 2P0.5 3622940.0 cm-1
2p2 3s1 2P1.5 3632630.0 cm-1
2s1 2p1 3d1 2P0.5 3638280.0 cm-1
2s1 2p1 3d1 2P1.5 3640260.0 cm-1
2p2 3p1 2S0.5 3642910.0 cm-1
2p2 3p1 4D0.5 3652210.0 cm-1
2p2 3p1 4D1.5 3655900.0 cm-1
2p2 3s1 2D2.5 3658520.0 cm-1
2p2 3s1 2D1.5 3659480.0 cm-1
2p2 3p1 4D2.5 3662350.0 cm-1
2p2 3p1 4D3.5 3671040.0 cm-1
2p2 3p1 4P0.5 3671580.0 cm-1
2p2 3p1 4P1.5 3672900.0 cm-1
2p2 3p1 4P2.5 3677840.0 cm-1
2p2 3p1 2D1.5 3685660.0 cm-1
2p2 3p1 2D2.5 3697580.0 cm-1
2p2 3p1 2P1.5 3714960.0 cm-1
2p2 3p1 2P0.5 3717200.0 cm-1
2p2 3p1 4S1.5 3720320.0 cm-1
2p2 3d1 4F1.5 3734030.0 cm-1
2p2 3d1 4F2.5 3737450.0 cm-1
2p2 3d1 4F3.5 3742480.0 cm-1
2p2 3p1 2F2.5 3748390.0 cm-1
2p2 3d1 4F4.5 3749250.0 cm-1
2p2 3p1 2F3.5 3751980.0 cm-1
2p2 3d1 4D1.5 3755480.0 cm-1
2p2 3d1 4D0.5 3756230.0 cm-1
2p2 3d1 4D2.5 3759450.0 cm-1
2p2 3d1 4D3.5 3762410.0 cm-1
2p2 3d1 2P1.5 3763040.0 cm-1
2p2 3d1 2F2.5 3767760.0 cm-1
2p2 3d1 2P0.5 3771940.0 cm-1
2p2 3d1 2F3.5 3779860.0 cm-1
2p2 3p1 2D1.5 3785150.0 cm-1
2p2 3p1 2D2.5 3785840.0 cm-1
2p2 3d1 4P2.5 3787280.0 cm-1
2p2 3d1 4P1.5 3790950.0 cm-1
2p2 3d1 4P0.5 3792620.0 cm-1
2p2 3s1 2S0.5 3797290.0 cm-1
2p2 3p1 2P0.5 3806800.0 cm-1
2p2 3p1 2P1.5 3814870.0 cm-1
2p2 3d1 2G3.5 3828680.0 cm-1
2p2 3d1 2G4.5 3830440.0 cm-1
2p2 3d1 2D2.5 3834000.0 cm-1
2p2 3d1 2D1.5 3834740.0 cm-1
2p2 3d1 2D1.5 3853180.0 cm-1
2p2 3d1 2D2.5 3857370.0 cm-1
2p2 3d1 2F3.5 3864370.0 cm-1
2p2 3d1 2F2.5 3868970.0 cm-1
2p2 3d1 2P0.5 3879880.0 cm-1
2p2 3d1 2P1.5 3884810.0 cm-1
2p2 3d1 2S0.5 3893180.0 cm-1
2p2 3p1 2P0.5 3902180.0 cm-1
2p2 3p1 2P1.5 3904190.0 cm-1
2p2 3d1 2D2.5 3987370.0 cm-1
2p2 3d1 2D1.5 3989380.0 cm-1
2s2 4s1 2S0.5 4040050.0 cm-1
2s2 4p1 2P0.5 4082610.0 cm-1
2s2 4p1 2P1.5 4084580.0 cm-1
2s2 4d1 2D1.5 4120000.0 cm-1
2s2 4d1 2D2.5 4120580.0 cm-1
2s2 4f1 2F2.5 4140980.0 cm-1
2s2 4f1 2F3.5 4141240.0 cm-1
2s1 2p1 4s1 4P0.5 4255940.0 cm-1
2s1 2p1 4s1 4P1.5 4261110.0 cm-1
2s1 2p1 4s1 4P2.5 4271740.0 cm-1
2s1 2p1 4s1 2P0.5 4276250.0 cm-1
2s1 2p1 4s1 2P1.5 4288070.0 cm-1
2s1 2p1 4p1 4D0.5 4294630.0 cm-1
2s1 2p1 4p1 4D1.5 4298190.0 cm-1
2s1 2p1 4p1 4D2.5 4303460.0 cm-1
2s1 2p1 4p1 2P1.5 4304060.0 cm-1
2s1 2p1 4p1 2P0.5 4305150.0 cm-1
2s1 2p1 4p1 4P0.5 4310680.0 cm-1
2s1 2p1 4p1 4S1.5 4312320.0 cm-1
2s1 2p1 4p1 4D3.5 4312610.0 cm-1
2s1 2p1 4p1 4P1.5 4319160.0 cm-1
2s1 2p1 4p1 4P2.5 4320380.0 cm-1
2s1 2p1 4p1 2D1.5 4322550.0 cm-1
2s1 2p1 4d1 4F1.5 4329240.0 cm-1
2s1 2p1 4p1 2D2.5 4330750.0 cm-1
2s1 2p1 4d1 4F2.5 4331920.0 cm-1
2s1 2p1 4d1 4F3.5 4336360.0 cm-1
2s1 2p1 4d1 4D2.5 4340300.0 cm-1
2s1 2p1 4p1 2S0.5 4341370.0 cm-1
2s1 2p1 4d1 4D1.5 4341680.0 cm-1
2s1 2p1 4d1 4D0.5 4342310.0 cm-1
2s1 2p1 4d1 4F4.5 4344760.0 cm-1
2s1 2p1 4d1 2D1.5 4346970.0 cm-1
2s1 2p1 4d1 2D2.5 4350120.0 cm-1
2s1 2p1 4d1 4D3.5 4350880.0 cm-1
2s1 2p1 4d1 4P2.5 4353500.0 cm-1
2s1 2p1 4d1 4P1.5 4354460.0 cm-1
2s1 2p1 4d1 4P0.5 4355050.0 cm-1
2s1 2p1 4f1 4G2.5 4355220.0 cm-1
2s1 2p1 4f1 4F3.5 4355660.0 cm-1
2s1 2p1 4f1 4F1.5 4359150.0 cm-1
2s1 2p1 4f1 4F4.5 4359880.0 cm-1
2s1 2p1 4f1 4F2.5 4360220.0 cm-1
2s1 2p1 4f1 2F3.5 4360920.0 cm-1
2s1 2p1 4f1 2F2.5 4363560.0 cm-1
2s1 2p1 4f1 2G3.5 4363640.0 cm-1
2s1 2p1 4d1 2F2.5 4365300.0 cm-1
2s1 2p1 4d1 2P1.5 4371090.0 cm-1
2s1 2p1 4f1 4G4.5 4371190.0 cm-1
2s1 2p1 4f1 4G3.5 4371900.0 cm-1
2s1 2p1 4f1 4G5.5 4373010.0 cm-1
2s1 2p1 4d1 2F3.5 4373270.0 cm-1
2s1 2p1 4f1 4D2.5 4373600.0 cm-1
2s1 2p1 4f1 4D3.5 4373750.0 cm-1
2s1 2p1 4f1 4D1.5 4375420.0 cm-1
2s1 2p1 4d1 2P0.5 4375820.0 cm-1
2s1 2p1 4f1 2G4.5 4375850.0 cm-1
2s1 2p1 4f1 4D0.5 4376470.0 cm-1
2s1 2p1 4f1 2D2.5 4376890.0 cm-1
2s1 2p1 4f1 2D1.5 4379640.0 cm-1
2s1 2p1 4s1 2P0.5 4472720.0 cm-1
2s1 2p1 4s1 2P1.5 4473040.0 cm-1
2s1 2p1 4p1 2D1.5 4513050.0 cm-1
2s1 2p1 4p1 2D2.5 4514200.0 cm-1
2s1 2p1 4p1 2P0.5 4515060.0 cm-1
2s1 2p1 4p1 2P1.5 4516720.0 cm-1
2s1 2p1 4p1 2S0.5 4523900.0 cm-1
2s1 2p1 4d1 2F3.5 4549650.0 cm-1
2s1 2p1 4d1 2F2.5 4549680.0 cm-1
2s1 2p1 4d1 2D1.5 4550810.0 cm-1
2s1 2p1 4d1 2D2.5 4551560.0 cm-1
2s1 2p1 4d1 2P0.5 4559210.0 cm-1
2s1 2p1 4d1 2P1.5 4559820.0 cm-1
2s1 2p1 4f1 2F2.5 4565740.0 cm-1
2s1 2p1 4f1 2F3.5 4566010.0 cm-1
2s1 2p1 4f1 2G3.5 4572150.0 cm-1
2s1 2p1 4f1 2G4.5 4572410.0 cm-1
2s1 2p1 4f1 2D1.5 4576550.0 cm-1
2s1 2p1 4f1 2D2.5 4576780.0 cm-1
L+12        17        13       5293400.(  )

        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 = 1.38654
         2S = 1.24854
         2P = 1.17292
         3S = 1.60085
         3P = 1.36417
         3D = 1.47653
         4S = 1.47955
         4P = 1.36821
         4D = 1.53241
         4F = 1.44182

 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 564.4400 Rydbergs (7679.770640 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.00979632 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.959264 eV) was used
 from the last threshold up to 1.019464 Z**2 Rydbergs (1997.4 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.959264 eV) was used
 from first threshold up to 1.019464 Z**2 Rydbergs (1997.4 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:        04/05/12

 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 21:19:29 2013


  • Guiyun Liang
  • Nigel Badnell
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