Resolved Specific Ion Data Collections

Temperature Range
0.155 eV → 1551 eV


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  • Spontaneous Emission: N+2(i) → N+2(j) + hv
  • Electron Impact Excitation: N+2(i) + e → N+2(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 176.3 cm-1
2s1 2p2 4P0.5 53609.2 cm-1
2s1 2p2 4P1.5 53671.5 cm-1
2s1 2p2 4P2.5 53775.0 cm-1
2s1 2p2 2D1.5 105573.0 cm-1
2s1 2p2 2D2.5 105577.0 cm-1
2s1 2p2 2S0.5 135400.0 cm-1
2s1 2p2 2P0.5 154230.0 cm-1
2s1 2p2 2P1.5 154352.0 cm-1
2p3 4S1.5 186655.0 cm-1
2p3 2D1.5 210852.0 cm-1
2p3 2D2.5 210855.0 cm-1
2s2 3s1 2S0.5 217287.0 cm-1
2p3 2P0.5 240160.0 cm-1
2p3 2P1.5 240174.0 cm-1
2s2 3p1 2P0.5 242034.0 cm-1
2s2 3p1 2P1.5 242074.0 cm-1
2s2 3d1 2D1.5 264305.0 cm-1
2s2 3d1 2D2.5 264313.0 cm-1
2s1 2p1 3s1 4P0.5 285389.0 cm-1
2s1 2p1 3s1 4P1.5 285453.0 cm-1
2s1 2p1 3s1 4P2.5 285559.0 cm-1
2s1 2p1 3s1 2P0.5 297413.0 cm-1
2s1 2p1 3s1 2P1.5 297511.0 cm-1
2s2 4s1 2S0.5 299496.0 cm-1
2s1 2p1 3p1 2P0.5 307251.0 cm-1
2s1 2p1 3p1 2P1.5 307305.0 cm-1
2s1 2p1 3p1 4D0.5 307919.0 cm-1
2s1 2p1 3p1 4D1.5 307954.0 cm-1
2s1 2p1 3p1 4D2.5 308015.0 cm-1
2s1 2p1 3p1 4D3.5 308104.0 cm-1
2s2 4p1 2P0.5 311445.0 cm-1
2s2 4p1 2P1.5 311476.0 cm-1
2s1 2p1 3p1 4S1.5 312509.0 cm-1
2s1 2p1 3p1 4P0.5 314789.0 cm-1
2s1 2p1 3p1 4P1.5 314831.0 cm-1
2s1 2p1 3p1 4P2.5 314896.0 cm-1
2s2 4d1 2D1.5 316832.0 cm-1
2s2 4d1 2D2.5 316851.0 cm-1
2s2 4f1 2F2.5 318904.0 cm-1
2s2 4f1 2F3.5 318905.0 cm-1
2s1 2p1 3p1 2D1.5 320571.0 cm-1
2s1 2p1 3p1 2D2.5 320660.0 cm-1
2s1 2p1 3p1 2S0.5 328647.0 cm-1
2s1 2p1 3d1 4F1.5 331158.0 cm-1
2s1 2p1 3d1 4F2.5 331192.0 cm-1
2s1 2p1 3d1 4F3.5 331241.0 cm-1
2s1 2p1 3d1 4F4.5 331304.0 cm-1
2s1 2p1 3d1 4D0.5 334561.0 cm-1
2s1 2p1 3d1 4D1.5 334572.0 cm-1
2s1 2p1 3d1 4D2.5 334591.0 cm-1
2s1 2p1 3d1 4D3.5 334619.0 cm-1
2s1 2p1 3d1 2D1.5 336963.0 cm-1
2s1 2p1 3d1 2D2.5 336982.0 cm-1
2s1 2p1 3d1 4P2.5 337177.0 cm-1
2s1 2p1 3d1 4P1.5 337214.0 cm-1
2s1 2p1 3d1 4P0.5 337240.0 cm-1
2s1 2p1 3d1 2F2.5 343770.0 cm-1
2s1 2p1 3d1 2F3.5 343869.0 cm-1
2s1 2p1 3d1 2P1.5 346794.0 cm-1
2s1 2p1 3d1 2P0.5 346851.0 cm-1
2s1 2p1 3s1 2P0.5 357951.0 cm-1
2s1 2p1 3s1 2P1.5 357956.0 cm-1
2s1 2p1 4s1 4P0.5 371327.0 cm-1
2s1 2p1 4s1 4P1.5 371385.0 cm-1
2s1 2p1 4s1 4P2.5 371484.0 cm-1
2s1 2p1 4s1 2P0.5 376371.0 cm-1
2s1 2p1 4s1 2P1.5 376485.0 cm-1
2s1 2p1 4p1 2P0.5 378271.0 cm-1
2s1 2p1 4p1 2P1.5 378321.0 cm-1
2s1 2p1 3p1 2D1.5 378457.0 cm-1
2s1 2p1 3p1 2D2.5 378503.0 cm-1
2s1 2p1 4p1 4D0.5 380026.0 cm-1
2s1 2p1 4p1 4D1.5 380057.0 cm-1
2s1 2p1 4p1 4D2.5 380108.0 cm-1
2s1 2p1 4p1 4D3.5 380182.0 cm-1
2s1 2p1 4p1 4S1.5 381324.0 cm-1
2s1 2p1 4p1 2S0.5 381570.0 cm-1
2s1 2p1 4p1 4P0.5 382607.0 cm-1
2s1 2p1 4p1 4P1.5 382641.0 cm-1
2s1 2p1 4p1 4P2.5 382691.0 cm-1
2s1 2p1 3p1 2P0.5 382869.0 cm-1
2s1 2p1 3p1 2P1.5 382904.0 cm-1
2s1 2p1 4d1 4F1.5 386892.0 cm-1
2s1 2p1 4d1 4F2.5 386926.0 cm-1
2s1 2p1 4d1 4F3.5 386973.0 cm-1
2s1 2p1 4d1 4F4.5 387035.0 cm-1
2s1 2p1 4p1 2D1.5 387412.0 cm-1
2s1 2p1 4p1 2D2.5 387467.0 cm-1
2s1 2p1 4d1 4D0.5 388381.0 cm-1
2s1 2p1 4d1 4D1.5 388390.0 cm-1
2s1 2p1 4d1 4D2.5 388406.0 cm-1
2s1 2p1 4d1 4D3.5 388437.0 cm-1
2s1 2p1 4d1 2D1.5 388762.0 cm-1
2s1 2p1 4d1 2D2.5 388787.0 cm-1
2s1 2p1 4d1 4P2.5 389080.0 cm-1
2s1 2p1 4d1 4P1.5 389122.0 cm-1
2s1 2p1 4d1 4P0.5 389148.0 cm-1
2s1 2p1 4f1 2F2.5 389994.0 cm-1
2s1 2p1 4f1 2F3.5 390015.0 cm-1
2s1 2p1 4f1 4F1.5 390027.0 cm-1
2s1 2p1 4f1 4F2.5 390035.0 cm-1
2s1 2p1 4f1 4F3.5 390048.0 cm-1
2s1 2p1 4f1 4F4.5 390063.0 cm-1
2s1 2p1 4f1 4G2.5 391330.0 cm-1
2s1 2p1 4f1 4G3.5 391361.0 cm-1
2s1 2p1 4f1 4G4.5 391406.0 cm-1
2s1 2p1 4f1 4G5.5 391462.0 cm-1
2s1 2p1 4f1 4D3.5 391473.0 cm-1
2s1 2p1 4f1 4D2.5 391514.0 cm-1
2s1 2p1 4f1 4D1.5 391547.0 cm-1
2s1 2p1 4f1 4D0.5 391566.0 cm-1
2s1 2p1 4f1 2G3.5 391608.0 cm-1
2s1 2p1 4f1 2G4.5 391695.0 cm-1
2s1 2p1 4f1 2D2.5 391742.0 cm-1
2s1 2p1 4f1 2D1.5 391803.0 cm-1
2s1 2p1 4d1 2F2.5 392365.0 cm-1
2s1 2p1 4d1 2F3.5 392459.0 cm-1
2s1 2p1 4d1 2P1.5 394541.0 cm-1
2s1 2p1 4d1 2P0.5 394600.0 cm-1
2s1 2p1 3p1 2S0.5 395305.0 cm-1
2p2 3s1 4P0.5 401353.0 cm-1
2p2 3s1 4P1.5 401416.0 cm-1
2p2 3s1 4P2.5 401522.0 cm-1
2s1 2p1 3d1 2F2.5 404224.0 cm-1
2s1 2p1 3d1 2F3.5 404225.0 cm-1
2s1 2p1 3d1 2D1.5 406330.0 cm-1
2s1 2p1 3d1 2D2.5 406343.0 cm-1
2s1 2p1 3d1 2P0.5 410239.0 cm-1
2s1 2p1 3d1 2P1.5 410250.0 cm-1
2p2 3s1 2P0.5 416974.0 cm-1
2p2 3s1 2P1.5 417085.0 cm-1
2p2 3p1 2S0.5 417730.0 cm-1
2p2 3p1 4D0.5 422642.0 cm-1
2p2 3p1 4D1.5 422680.0 cm-1
2p2 3p1 4D2.5 422742.0 cm-1
2p2 3p1 4D3.5 422829.0 cm-1
2p2 3s1 2D1.5 425384.0 cm-1
2p2 3s1 2D2.5 425386.0 cm-1
2p2 3p1 4P0.5 425932.0 cm-1
2p2 3p1 4P1.5 425968.0 cm-1
2p2 3p1 4P2.5 426030.0 cm-1
2p2 3p1 2D1.5 430262.0 cm-1
2p2 3p1 2D2.5 430369.0 cm-1
2p2 3p1 2P1.5 436517.0 cm-1
2p2 3p1 2P0.5 436533.0 cm-1
2p2 3p1 4S1.5 440637.0 cm-1
2s1 2p1 4s1 2P0.5 440844.0 cm-1
2s1 2p1 4s1 2P1.5 440854.0 cm-1
2p2 3d1 4F1.5 443730.0 cm-1
2p2 3d1 4F2.5 443764.0 cm-1
2p2 3d1 4F3.5 443812.0 cm-1
2p2 3d1 4F4.5 443874.0 cm-1
2p2 3p1 2F2.5 446419.0 cm-1
2p2 3p1 2F3.5 446453.0 cm-1
2p2 3d1 2P1.5 446899.0 cm-1
2p2 3d1 2P0.5 446988.0 cm-1
2p2 3d1 4D0.5 447626.0 cm-1
2p2 3d1 4D1.5 447634.0 cm-1
2p2 3d1 4D2.5 447650.0 cm-1
2p2 3d1 4D3.5 447676.0 cm-1
2p2 3d1 2F2.5 450188.0 cm-1
2p2 3d1 2F3.5 450303.0 cm-1
2s1 2p1 4p1 2D1.5 450329.0 cm-1
2s1 2p1 4p1 2D2.5 450334.0 cm-1
2p2 3d1 4P2.5 450832.0 cm-1
2p2 3d1 4P1.5 450877.0 cm-1
2p2 3d1 4P0.5 450903.0 cm-1
2s1 2p1 4p1 2S0.5 451298.0 cm-1
2s1 2p1 4p1 2P0.5 451317.0 cm-1
2s1 2p1 4p1 2P1.5 451327.0 cm-1
2s1 2p1 4f1 2G3.5 455974.0 cm-1
2s1 2p1 4f1 2G4.5 455975.0 cm-1
2p2 3p1 2D2.5 456836.0 cm-1
2p2 3p1 2D1.5 456842.0 cm-1
2s1 2p1 4d1 2F3.5 457987.0 cm-1
2s1 2p1 4d1 2F2.5 457988.0 cm-1
2s1 2p1 4d1 2D1.5 458511.0 cm-1
2s1 2p1 4d1 2D2.5 458514.0 cm-1
2s1 2p1 4f1 2F2.5 458628.0 cm-1
2s1 2p1 4f1 2F3.5 458628.0 cm-1
2s1 2p1 4d1 2P0.5 459763.0 cm-1
2s1 2p1 4d1 2P1.5 459771.0 cm-1
2s1 2p1 4f1 2D2.5 460220.0 cm-1
2s1 2p1 4f1 2D1.5 460227.0 cm-1
2p2 3d1 2D1.5 460614.0 cm-1
2p2 3d1 2D2.5 460651.0 cm-1
2p2 3p1 2P0.5 464628.0 cm-1
2p2 3p1 2P1.5 464687.0 cm-1
2p2 3s1 2S0.5 467320.0 cm-1
2p2 3d1 2F3.5 468495.0 cm-1
2p2 3d1 2F2.5 468511.0 cm-1
2p2 3d1 2D1.5 469457.0 cm-1
2p2 3d1 2D2.5 469479.0 cm-1
2p2 3d1 2G3.5 470401.0 cm-1
2p2 3d1 2G4.5 470406.0 cm-1
2p2 3d1 2P0.5 474425.0 cm-1
2p2 3d1 2P1.5 474459.0 cm-1
2p2 3d1 2S0.5 482651.0 cm-1
2p2 3p1 2P0.5 484301.0 cm-1
2p2 3p1 2P1.5 484399.0 cm-1
2p2 3d1 2D2.5 490591.0 cm-1
2p2 3d1 2D1.5 491671.0 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 = 1.42754
         2S = 1.29142
         2P = 1.18509
         3S = 1.55209
         3P = 1.33194
         3D = 1.38132
         4S = 1.53577
         4P = 1.17635
         4D = 1.55789
         4F = 1.95182

 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 31.8020 Rydbergs (432.698012 eV)

 A fine energy mesh of 0.000030 Z**2 Rydbergs (0.00163272 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.054424 eV) was used
 from the last threshold up to 2.615574 Z**2 Rydbergs (142.35 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.054424 eV) was used
 from first threshold up to 2.615574 Z**2 Rydbergs (142.35 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:        21/06/12

 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 18:13:12 2013


  • Guiyun Liang
  • Nigel Badnell
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