Resolved Specific Ion Data Collections

Temperature Range
3.878 eV → 3.878 x 104 eV


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  • Spontaneous Emission: K+14(i) → K+14(j) + hv
  • Electron Impact Excitation: K+14(i) + e → K+14(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 29016.7 cm-1
2s1 2p2 4P0.5 248324.0 cm-1
2s1 2p2 4P1.5 259627.0 cm-1
2s1 2p2 4P2.5 274201.0 cm-1
2s1 2p2 2D1.5 443964.0 cm-1
2s1 2p2 2D2.5 445512.0 cm-1
2s1 2p2 2S0.5 552838.0 cm-1
2s1 2p2 2P0.5 588276.0 cm-1
2s1 2p2 2P1.5 599078.0 cm-1
2p3 4S1.5 775283.0 cm-1
2p3 2D1.5 874321.0 cm-1
2p3 2D2.5 877405.0 cm-1
2p3 2P0.5 979274.0 cm-1
2p3 2P1.5 985693.0 cm-1
2s2 3s1 2S0.5 3894790.0 cm-1
2s2 3p1 2P0.5 4016370.0 cm-1
2s2 3p1 2P1.5 4024390.0 cm-1
2s2 3d1 2D1.5 4139120.0 cm-1
2s2 3d1 2D2.5 4141580.0 cm-1
2s1 2p1 3s1 4P0.5 4142180.0 cm-1
2s1 2p1 3s1 4P1.5 4151140.0 cm-1
2s1 2p1 3s1 4P2.5 4168980.0 cm-1
2s1 2p1 3s1 2P0.5 4204860.0 cm-1
2s1 2p1 3s1 2P1.5 4224480.0 cm-1
2s1 2p1 3p1 4D0.5 4250990.0 cm-1
2s1 2p1 3p1 4D1.5 4258970.0 cm-1
2s1 2p1 3p1 2P0.5 4268780.0 cm-1
2s1 2p1 3p1 2P1.5 4271250.0 cm-1
2s1 2p1 3p1 4D2.5 4272250.0 cm-1
2s1 2p1 3p1 4D3.5 4288090.0 cm-1
2s1 2p1 3p1 4S1.5 4295500.0 cm-1
2s1 2p1 3p1 4P0.5 4301640.0 cm-1
2s1 2p1 3p1 4P1.5 4313030.0 cm-1
2s1 2p1 3p1 4P2.5 4319340.0 cm-1
2s1 2p1 3p1 2D1.5 4323540.0 cm-1
2s1 2p1 3p1 2D2.5 4340900.0 cm-1
2s1 2p1 3d1 4F1.5 4359000.0 cm-1
2s1 2p1 3d1 4F2.5 4364500.0 cm-1
2s1 2p1 3p1 2S0.5 4371620.0 cm-1
2s1 2p1 3d1 4F3.5 4372820.0 cm-1
2s1 2p1 3d1 4F4.5 4385620.0 cm-1
2s1 2p1 3d1 4D2.5 4395650.0 cm-1
2s1 2p1 3d1 4D1.5 4396970.0 cm-1
2s1 2p1 3d1 4D0.5 4397130.0 cm-1
2s1 2p1 3s1 2P0.5 4397950.0 cm-1
2s1 2p1 3s1 2P1.5 4398280.0 cm-1
2s1 2p1 3d1 2D1.5 4406830.0 cm-1
2s1 2p1 3d1 2D2.5 4410250.0 cm-1
2s1 2p1 3d1 4D3.5 4411120.0 cm-1
2s1 2p1 3d1 4P2.5 4419750.0 cm-1
2s1 2p1 3d1 4P1.5 4421020.0 cm-1
2s1 2p1 3d1 4P0.5 4422290.0 cm-1
2s1 2p1 3d1 2F2.5 4464530.0 cm-1
2s1 2p1 3d1 2F3.5 4481570.0 cm-1
2s1 2p1 3d1 2P1.5 4481960.0 cm-1
2s1 2p1 3d1 2P0.5 4491650.0 cm-1
2s1 2p1 3p1 2P0.5 4517180.0 cm-1
2s1 2p1 3p1 2D1.5 4520240.0 cm-1
2s1 2p1 3p1 2D2.5 4525370.0 cm-1
2s1 2p1 3p1 2P1.5 4526040.0 cm-1
2s1 2p1 3p1 2S0.5 4554890.0 cm-1
2p2 3s1 4P0.5 4576100.0 cm-1
2p2 3s1 4P1.5 4586580.0 cm-1
2p2 3s1 4P2.5 4601580.0 cm-1
2s1 2p1 3d1 2F3.5 4630410.0 cm-1
2s1 2p1 3d1 2F2.5 4631030.0 cm-1
2s1 2p1 3d1 2D1.5 4643300.0 cm-1
2p2 3s1 2P0.5 4644320.0 cm-1
2s1 2p1 3d1 2D2.5 4646570.0 cm-1
2p2 3s1 2P1.5 4659100.0 cm-1
2s1 2p1 3d1 2P0.5 4664180.0 cm-1
2s1 2p1 3d1 2P1.5 4667800.0 cm-1
2p2 3p1 2S0.5 4671090.0 cm-1
2p2 3p1 4D0.5 4679110.0 cm-1
2p2 3p1 4D1.5 4684480.0 cm-1
2p2 3s1 2D2.5 4690660.0 cm-1
2p2 3s1 2D1.5 4693270.0 cm-1
2p2 3p1 4D2.5 4695430.0 cm-1
2p2 3p1 4P0.5 4705550.0 cm-1
2p2 3p1 4P1.5 4705850.0 cm-1
2p2 3p1 4D3.5 4709640.0 cm-1
2p2 3p1 4P2.5 4713750.0 cm-1
2p2 3p1 2D1.5 4721170.0 cm-1
2p2 3p1 2D2.5 4741170.0 cm-1
2p2 3p1 2P1.5 4756800.0 cm-1
2p2 3p1 2P0.5 4761700.0 cm-1
2p2 3p1 4S1.5 4762620.0 cm-1
2p2 3d1 4F1.5 4775090.0 cm-1
2p2 3d1 4F2.5 4780870.0 cm-1
2p2 3d1 4F3.5 4789470.0 cm-1
2p2 3p1 2F2.5 4795090.0 cm-1
2p2 3d1 4F4.5 4800780.0 cm-1
2p2 3p1 2F3.5 4800950.0 cm-1
2p2 3d1 2P1.5 4801620.0 cm-1
2p2 3d1 4D0.5 4803290.0 cm-1
2p2 3d1 4D2.5 4807110.0 cm-1
2p2 3d1 4D3.5 4812910.0 cm-1
2p2 3d1 4D1.5 4813900.0 cm-1
2p2 3d1 2F2.5 4818290.0 cm-1
2p2 3d1 2P0.5 4828660.0 cm-1
2p2 3p1 2D1.5 4836270.0 cm-1
2p2 3d1 2F3.5 4838210.0 cm-1
2p2 3p1 2D2.5 4838370.0 cm-1
2p2 3d1 4P2.5 4841930.0 cm-1
2p2 3s1 2S0.5 4847070.0 cm-1
2p2 3d1 4P1.5 4847590.0 cm-1
2p2 3d1 4P0.5 4851190.0 cm-1
2p2 3p1 2P0.5 4860280.0 cm-1
2p2 3p1 2P1.5 4874850.0 cm-1
2p2 3d1 2G3.5 4889840.0 cm-1
2p2 3d1 2G4.5 4893210.0 cm-1
2p2 3d1 2D2.5 4895780.0 cm-1
2p2 3d1 2D1.5 4897200.0 cm-1
2p2 3d1 2D1.5 4917360.0 cm-1
2p2 3d1 2D2.5 4923330.0 cm-1
2p2 3d1 2F3.5 4933350.0 cm-1
2p2 3d1 2F2.5 4941830.0 cm-1
2p2 3d1 2P0.5 4947970.0 cm-1
2p2 3d1 2P1.5 4956720.0 cm-1
2p2 3d1 2S0.5 4964300.0 cm-1
2p2 3p1 2P0.5 4969750.0 cm-1
2p2 3p1 2P1.5 4973290.0 cm-1
2p2 3d1 2D2.5 5071190.0 cm-1
2p2 3d1 2D1.5 5074430.0 cm-1
2s2 4s1 2S0.5 5290420.0 cm-1
2s2 4p1 2P0.5 5339960.0 cm-1
2s2 4p1 2P1.5 5343260.0 cm-1
2s2 4d1 2D1.5 5384530.0 cm-1
2s2 4d1 2D2.5 5385520.0 cm-1
2s2 4f1 2F2.5 5409280.0 cm-1
2s2 4f1 2F3.5 5409730.0 cm-1
2s1 2p1 4s1 4P0.5 5536550.0 cm-1
2s1 2p1 4s1 4P1.5 5544850.0 cm-1
2s1 2p1 4s1 2P0.5 5561070.0 cm-1
2s1 2p1 4s1 4P2.5 5563120.0 cm-1
2s1 2p1 4s1 2P1.5 5581100.0 cm-1
2s1 2p1 4p1 4D0.5 5581340.0 cm-1
2s1 2p1 4p1 4D1.5 5587140.0 cm-1
2s1 2p1 4p1 2P1.5 5593980.0 cm-1
2s1 2p1 4p1 4D2.5 5595550.0 cm-1
2s1 2p1 4p1 2P0.5 5597240.0 cm-1
2s1 2p1 4p1 4P0.5 5602480.0 cm-1
2s1 2p1 4p1 4S1.5 5606530.0 cm-1
2s1 2p1 4p1 4D3.5 5611660.0 cm-1
2s1 2p1 4p1 4P1.5 5617690.0 cm-1
2s1 2p1 4p1 4P2.5 5619310.0 cm-1
2s1 2p1 4p1 2D1.5 5620520.0 cm-1
2s1 2p1 4d1 4F1.5 5622810.0 cm-1
2s1 2p1 4d1 4F2.5 5626930.0 cm-1
2s1 2p1 4p1 2D2.5 5631600.0 cm-1
2s1 2p1 4d1 4F3.5 5634140.0 cm-1
2s1 2p1 4d1 4P2.5 5636780.0 cm-1
2s1 2p1 4d1 4D1.5 5639220.0 cm-1
2s1 2p1 4d1 4D0.5 5640310.0 cm-1
2s1 2p1 4p1 2S0.5 5642600.0 cm-1
2s1 2p1 4d1 2D1.5 5646540.0 cm-1
2s1 2p1 4d1 4F4.5 5649210.0 cm-1
2s1 2p1 4d1 2D2.5 5651420.0 cm-1
2s1 2p1 4f1 4G2.5 5652970.0 cm-1
2s1 2p1 4f1 4D3.5 5653670.0 cm-1
2s1 2p1 4d1 4D3.5 5655830.0 cm-1
2s1 2p1 4d1 4D2.5 5658710.0 cm-1
2s1 2p1 4f1 4F1.5 5660050.0 cm-1
2s1 2p1 4d1 4P1.5 5660120.0 cm-1
2s1 2p1 4d1 4P0.5 5660830.0 cm-1
2s1 2p1 4f1 4F4.5 5661010.0 cm-1
2s1 2p1 4f1 4F2.5 5661210.0 cm-1
2s1 2p1 4f1 4G3.5 5661810.0 cm-1
2s1 2p1 4f1 2F2.5 5665330.0 cm-1
2s1 2p1 4f1 2G3.5 5665510.0 cm-1
2s1 2p1 4d1 2F2.5 5669930.0 cm-1
2s1 2p1 4d1 2P1.5 5677580.0 cm-1
2s1 2p1 4f1 4G4.5 5680060.0 cm-1
2s1 2p1 4f1 4F3.5 5680600.0 cm-1
2s1 2p1 4d1 2F3.5 5681500.0 cm-1
2s1 2p1 4f1 4D2.5 5682400.0 cm-1
2s1 2p1 4f1 4G5.5 5682430.0 cm-1
2s1 2p1 4f1 2F3.5 5682940.0 cm-1
2s1 2p1 4d1 2P0.5 5684500.0 cm-1
2s1 2p1 4f1 4D1.5 5684750.0 cm-1
2s1 2p1 4f1 2G4.5 5685750.0 cm-1
2s1 2p1 4f1 4D0.5 5686200.0 cm-1
2s1 2p1 4f1 2D2.5 5686390.0 cm-1
2s1 2p1 4f1 2D1.5 5689880.0 cm-1
2s1 2p1 4s1 2P0.5 5787240.0 cm-1
2s1 2p1 4s1 2P1.5 5787740.0 cm-1
2s1 2p1 4p1 2D1.5 5834450.0 cm-1
2s1 2p1 4p1 2D2.5 5836470.0 cm-1
2s1 2p1 4p1 2P0.5 5836510.0 cm-1
2s1 2p1 4p1 2P1.5 5839410.0 cm-1
2s1 2p1 4p1 2S0.5 5847390.0 cm-1
2s1 2p1 4d1 2F3.5 5877990.0 cm-1
2s1 2p1 4d1 2F2.5 5878020.0 cm-1
2s1 2p1 4d1 2D1.5 5878980.0 cm-1
2s1 2p1 4d1 2D2.5 5880250.0 cm-1
2s1 2p1 4d1 2P0.5 5888660.0 cm-1
2s1 2p1 4d1 2P1.5 5889700.0 cm-1
2s1 2p1 4f1 2F2.5 5896890.0 cm-1
2s1 2p1 4f1 2F3.5 5897360.0 cm-1
2s1 2p1 4f1 2G3.5 5904220.0 cm-1
2s1 2p1 4f1 2G4.5 5904660.0 cm-1
2s1 2p1 4f1 2D1.5 5909070.0 cm-1
2s1 2p1 4f1 2D2.5 5909470.0 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 = 1.38433
         2S = 1.24945
         2P = 1.17349
         3S = 1.59525
         3P = 1.36693
         3D = 1.47974
         4S = 1.48780
         4P = 1.37360
         4D = 1.53422
         4F = 1.49809

 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 746.8942 Rydbergs (10162.242485 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.01333388 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.666776 eV) was used
 from the last threshold up to 0.975672 Z**2 Rydbergs (2601.9 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.666776 eV) was used
 from first threshold up to 0.975672 Z**2 Rydbergs (2601.9 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:        03/05/12


  • Guiyun Liang
  • Nigel Badnell
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