lilike_lgy10#ni25.dat

Resolved Specific Ion Data Collections

Ion
Ni25+
Temperature Range
11.63 eV → 1.163 x 105 eV

ADF04

Filename
lilike_lgy10#ni25.dat
Full Path
adf04/copaw#li/lilike_lgy10#ni25.dat
Download data
  • Spontaneous Emission: Ni+25(i) → Ni+25(j) + hv
  • Electron Impact Excitation: Ni+25(i) + e → Ni+25(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 427133.0 cm-1
2p1 2P1.5 601899.0 cm-1
3s1 2S0.5 10872700.0 cm-1
3p1 2P0.5 10991100.0 cm-1
3p1 2P1.5 11041600.0 cm-1
3d1 2D1.5 11089100.0 cm-1
3d1 2D2.5 11105700.0 cm-1
4s1 2S0.5 14618800.0 cm-1
4p1 2P0.5 14667400.0 cm-1
4p1 2P1.5 14688200.0 cm-1
4d1 2D1.5 14707900.0 cm-1
4d1 2D2.5 14714800.0 cm-1
4f1 2F2.5 14715900.0 cm-1
4f1 2F3.5 14719400.0 cm-1
5s1 2S0.5 16338200.0 cm-1
5p1 2P0.5 16362800.0 cm-1
5p1 2P1.5 16373100.0 cm-1
5d1 2D1.5 16383100.0 cm-1
5d1 2D2.5 16386600.0 cm-1
5f1 2F2.5 16387200.0 cm-1
5f1 2F3.5 16389000.0 cm-1
5g1 2G3.5 16389000.0 cm-1
5g1 2G4.5 16390100.0 cm-1
1s1 2s2 2S0.5 62176800.0 cm-1
1s1 2s1 2p1 4P0.5 62279100.0 cm-1
1s1 2s1 2p1 4P1.5 62326400.0 cm-1
1s1 2s1 2p1 4P2.5 62443800.0 cm-1
1s1 2s1 2p1 2P0.5 62636700.0 cm-1
1s1 2s1 2p1 2P1.5 62739500.0 cm-1
1s1 2p2 4P0.5 62800000.0 cm-1
1s1 2s1 2p1 2P0.5 62858900.0 cm-1
1s1 2p2 4P1.5 62884500.0 cm-1
1s1 2s1 2p1 2P1.5 62887600.0 cm-1
1s1 2p2 4P2.5 62954900.0 cm-1
1s1 2p2 2D1.5 63107200.0 cm-1
1s1 2p2 2P0.5 63120600.0 cm-1
1s1 2p2 2D2.5 63183700.0 cm-1
1s1 2p2 2P1.5 63301200.0 cm-1
1s1 2p2 2S0.5 63467800.0 cm-1
1s1 2s1 3s1 4S1.5 73216200.0 cm-1
1s1 2s1 3s1 2S0.5 73332300.0 cm-1
1s1 2s1 3p1 4P0.5 73366400.0 cm-1
1s1 2s1 3p1 4P1.5 73372000.0 cm-1
1s1 2s1 3p1 4P2.5 73411300.0 cm-1
1s1 2s1 3p1 2P1.5 73420700.0 cm-1
1s1 2s1 3p1 2P0.5 73420800.0 cm-1
1s1 2s1 3d1 4D0.5 73492400.0 cm-1
1s1 2s1 3d1 4D1.5 73498100.0 cm-1
1s1 2s1 3d1 4D2.5 73506600.0 cm-1
1s1 2s1 3s1 2S0.5 73512000.0 cm-1
1s1 2s1 3d1 4D3.5 73517900.0 cm-1
1s1 2p1 3s1 4P0.5 73545300.0 cm-1
1s1 2s1 3d1 2D2.5 73565400.0 cm-1
1s1 2s1 3d1 2D1.5 73566300.0 cm-1
1s1 2p1 3s1 4P1.5 73580600.0 cm-1
1s1 2p1 3p1 4D0.5 73616000.0 cm-1
1s1 2s1 3p1 2P0.5 73619000.0 cm-1
1s1 2p1 3p1 4D1.5 73642300.0 cm-1
1s1 2s1 3p1 2P1.5 73669900.0 cm-1
1s1 2p1 3s1 2P0.5 73676200.0 cm-1
1s1 2p1 3s1 4P2.5 73703100.0 cm-1
1s1 2p1 3p1 2P1.5 73704800.0 cm-1
1s1 2p1 3p1 4D2.5 73710700.0 cm-1
1s1 2p1 3p1 4P0.5 73736300.0 cm-1
1s1 2p1 3d1 4F1.5 73748600.0 cm-1
1s1 2p1 3p1 2P0.5 73750000.0 cm-1
1s1 2p1 3p1 2D1.5 73771900.0 cm-1
1s1 2p1 3d1 4F2.5 73774000.0 cm-1
1s1 2s1 3d1 2D1.5 73782500.0 cm-1
1s1 2s1 3d1 2D2.5 73796000.0 cm-1
1s1 2p1 3s1 2P1.5 73810100.0 cm-1
1s1 2p1 3d1 4D2.5 73814300.0 cm-1
1s1 2p1 3d1 4F3.5 73822000.0 cm-1
1s1 2p1 3p1 4D3.5 73825500.0 cm-1
1s1 2p1 3d1 2D1.5 73832400.0 cm-1
1s1 2p1 3p1 4P1.5 73835000.0 cm-1
1s1 2p1 3d1 4D0.5 73853100.0 cm-1
1s1 2p1 3d1 4D1.5 73855600.0 cm-1
1s1 2p1 3p1 4P2.5 73857700.0 cm-1
1s1 2p1 3d1 2F2.5 73860300.0 cm-1
1s1 2p1 3p1 4S1.5 73863900.0 cm-1
1s1 2p1 3s1 2P1.5 73891700.0 cm-1
1s1 2p1 3s1 2P0.5 73899200.0 cm-1
1s1 2p1 3d1 4F4.5 73926400.0 cm-1
1s1 2p1 3p1 2D2.5 73934000.0 cm-1
1s1 2p1 3p1 2S0.5 73945500.0 cm-1
1s1 2p1 3d1 2D2.5 73949000.0 cm-1
1s1 2p1 3d1 4D3.5 73964900.0 cm-1
1s1 2p1 3d1 4P1.5 73983900.0 cm-1
1s1 2p1 3d1 4P2.5 73988400.0 cm-1
1s1 2p1 3d1 4P0.5 73990100.0 cm-1
1s1 2p1 3p1 2D1.5 74004300.0 cm-1
1s1 2p1 3p1 2P0.5 74005200.0 cm-1
1s1 2p1 3d1 2F3.5 74011100.0 cm-1
1s1 2p1 3d1 2P1.5 74013400.0 cm-1
1s1 2p1 3p1 2D2.5 74026300.0 cm-1
1s1 2p1 3p1 2P1.5 74061200.0 cm-1
1s1 2p1 3d1 2P0.5 74065200.0 cm-1
1s1 2p1 3p1 2S0.5 74107400.0 cm-1
1s1 2p1 3d1 2D1.5 74116400.0 cm-1
1s1 2p1 3d1 2D2.5 74123200.0 cm-1
1s1 2p1 3d1 2F3.5 74140000.0 cm-1
1s1 2p1 3d1 2P0.5 74166600.0 cm-1
1s1 2p1 3d1 2F2.5 74166800.0 cm-1
1s1 2p1 3d1 2P1.5 74196200.0 cm-1
1s1 2s1 4s1 4S1.5 77068100.0 cm-1
1s1 2s1 4s1 2S0.5 77106000.0 cm-1
1s1 2s1 4p1 4P0.5 77123300.0 cm-1
1s1 2s1 4p1 4P1.5 77126800.0 cm-1
1s1 2s1 4p1 4P2.5 77140500.0 cm-1
1s1 2s1 4p1 2P1.5 77153000.0 cm-1
1s1 2s1 4p1 2P0.5 77155900.0 cm-1
1s1 2s1 4d1 4D0.5 77176600.0 cm-1
1s1 2s1 4d1 4D1.5 77177800.0 cm-1
1s1 2s1 4d1 4D2.5 77180000.0 cm-1
1s1 2s1 4d1 4D3.5 77183900.0 cm-1
1s1 2s1 4d1 2D2.5 77198800.0 cm-1
1s1 2s1 4d1 2D1.5 77200300.0 cm-1
1s1 2s1 4f1 4F1.5 77210800.0 cm-1
1s1 2s1 4f1 4F2.5 77211400.0 cm-1
1s1 2s1 4f1 4F3.5 77212400.0 cm-1
1s1 2s1 4f1 4F4.5 77214500.0 cm-1
1s1 2s1 4f1 2F3.5 77218500.0 cm-1
1s1 2s1 4f1 2F2.5 77219400.0 cm-1
1s1 2s1 4s1 2S0.5 77335800.0 cm-1
1s1 2p1 4s1 4P0.5 77342600.0 cm-1
1s1 2p1 4s1 4P1.5 77370300.0 cm-1
1s1 2p1 4p1 4D0.5 77376800.0 cm-1
1s1 2s1 4p1 2P0.5 77382100.0 cm-1
1s1 2p1 4s1 2P0.5 77397700.0 cm-1
1s1 2p1 4p1 4D1.5 77400300.0 cm-1
1s1 2s1 4p1 2P1.5 77404800.0 cm-1
1s1 2p1 4p1 4S1.5 77413800.0 cm-1
1s1 2p1 4d1 4F1.5 77430800.0 cm-1
1s1 2p1 4p1 4D2.5 77431200.0 cm-1
1s1 2p1 4p1 4P0.5 77432900.0 cm-1
1s1 2s1 4d1 2D1.5 77439900.0 cm-1
1s1 2p1 4p1 2P0.5 77447000.0 cm-1
1s1 2p1 4d1 4F2.5 77447400.0 cm-1
1s1 2s1 4d1 2D2.5 77449300.0 cm-1
1s1 2p1 4p1 2D1.5 77452000.0 cm-1
1s1 2p1 4d1 4D2.5 77458300.0 cm-1
1s1 2p1 4f1 4G2.5 77462700.0 cm-1
1s1 2p1 4f1 2G3.5 77467200.0 cm-1
1s1 2s1 4f1 2F2.5 77469700.0 cm-1
1s1 2s1 4f1 2F3.5 77472400.0 cm-1
1s1 2p1 4d1 4D1.5 77477500.0 cm-1
1s1 2p1 4d1 4F3.5 77478300.0 cm-1
1s1 2p1 4d1 2D1.5 77481600.0 cm-1
1s1 2p1 4d1 4D0.5 77482200.0 cm-1
1s1 2p1 4d1 2F2.5 77488100.0 cm-1
1s1 2p1 4f1 4G3.5 77493000.0 cm-1
1s1 2p1 4f1 4F1.5 77494500.0 cm-1
1s1 2p1 4f1 2F2.5 77496200.0 cm-1
1s1 2p1 4f1 4G4.5 77498300.0 cm-1
1s1 2p1 4f1 2D2.5 77500500.0 cm-1
1s1 2p1 4f1 4D3.5 77504000.0 cm-1
1s1 2p1 4s1 4P2.5 77511200.0 cm-1
1s1 2p1 4s1 2P1.5 77535700.0 cm-1
1s1 2p1 4p1 4P1.5 77558900.0 cm-1
1s1 2p1 4p1 4P2.5 77562400.0 cm-1
1s1 2p1 4p1 4D3.5 77562400.0 cm-1
1s1 2p1 4p1 2P1.5 77577200.0 cm-1
1s1 2p1 4p1 2D2.5 77595400.0 cm-1
1s1 2p1 4d1 4F4.5 77603000.0 cm-1
1s1 2p1 4d1 2D2.5 77607700.0 cm-1
1s1 2p1 4p1 2S0.5 77608400.0 cm-1
1s1 2p1 4d1 4D3.5 77610100.0 cm-1
1s1 2p1 4d1 4P1.5 77616900.0 cm-1
1s1 2p1 4d1 4P0.5 77619600.0 cm-1
1s1 2p1 4d1 4P2.5 77620400.0 cm-1
1s1 2p1 4d1 2P1.5 77627700.0 cm-1
1s1 2p1 4f1 2F3.5 77631100.0 cm-1
1s1 2p1 4f1 4F4.5 77633700.0 cm-1
1s1 2p1 4f1 4F2.5 77634200.0 cm-1
1s1 2p1 4d1 2F3.5 77635600.0 cm-1
1s1 2p1 4f1 4F3.5 77636900.0 cm-1
1s1 2p1 4f1 4G5.5 77639900.0 cm-1
1s1 2p1 4f1 4D1.5 77640400.0 cm-1
1s1 2p1 4f1 2G4.5 77642400.0 cm-1
1s1 2p1 4f1 4D2.5 77643100.0 cm-1
1s1 2p1 4f1 4D0.5 77644900.0 cm-1
1s1 2p1 4d1 2P0.5 77645400.0 cm-1
1s1 2p1 4f1 2D1.5 77650700.0 cm-1
1s1 2p1 4s1 2P0.5 77671600.0 cm-1
1s1 2p1 4s1 2P1.5 77672100.0 cm-1
1s1 2p1 4p1 2P0.5 77713300.0 cm-1
1s1 2p1 4p1 2D1.5 77714000.0 cm-1
1s1 2p1 4p1 2D2.5 77726400.0 cm-1
1s1 2p1 4p1 2P1.5 77734000.0 cm-1
1s1 2p1 4p1 2S0.5 77745700.0 cm-1
1s1 2p1 4d1 2D1.5 77760800.0 cm-1
1s1 2p1 4d1 2D2.5 77764300.0 cm-1
1s1 2p1 4d1 2F3.5 77765000.0 cm-1
1s1 2p1 4d1 2F2.5 77775400.0 cm-1
1s1 2p1 4d1 2P0.5 77777000.0 cm-1
1s1 2p1 4f1 2F2.5 77779000.0 cm-1
1s1 2p1 4f1 2F3.5 77782200.0 cm-1
1s1 2p1 4d1 2P1.5 77787900.0 cm-1
1s1 2p1 4f1 2G3.5 77790900.0 cm-1
1s1 2p1 4f1 2G4.5 77792000.0 cm-1
1s1 2p1 4f1 2D1.5 77795900.0 cm-1
1s1 2p1 4f1 2D2.5 77800100.0 cm-1
------------------------------------------------------------------------

        Result of ICFT R-matrix calculation for outer shell excitation
        +++++++++++++++++++++++++++++++++++

 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 = 1.28287
         2S = 1.04757
         2P = 0.95474
         3S = 1.03399
         3P = 0.94174
         3D = 0.88392
         4S = 1.03252
         4P = 0.94144
         4D = 0.88552
         4F = 1.04000
         5S = 1.03462
         5P = 0.94344
         5D = 0.88910
         5F = 0.86709
         5G = 1.00000

 An exchange calculation was performed up to J=10
 A non-exchange calculation was then performed up to J=40
 Followed by a top-up calculation to J -> infinity.

 60 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 2314.0045 Rydbergs (31484.345227 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.034015 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (85.0375 eV) was used
 from the last threshold up to 2.767015 Z**2 Rydbergs (23530 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (85.0375 eV) was used
 from first threshold up to 2.767015 Z**2 Rydbergs (23530 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

 Produced by: Guiyun Liang
 Date:        11/10/10
------------------------------------------------------------------------
        Result of ICFT R-matrix calculation for core-excitation
   G.Y. Liang, and N.R. Badnell, A&A (2010)
        +++++++++++++++++++++++++++++++++++

 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 = 1.28813
         2S = 1.04928
         2P = 0.95672
         3S = 1.03607
         3P = 0.94366
         3D = 0.88616
         4S = 1.03600
         4P = 0.94469
         4D = 0.89019
         4F = 1.04177

 An exchange calculation was performed up to J=10
 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 0 Rydbergs (0.000000 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.034015 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (85.0375 eV) was used
 from the last threshold up to 2.767015 Z**2 Rydbergs (23530 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (85.0375 eV) was used
 from first threshold up to 2.767015 Z**2 Rydbergs (23530 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

  NIST v4 energy  (Ryd)
  2    3.89178
  3    5.50927
  4   99.020191
  5  100.09931
  6  100.57828
  7  100.98671
  8  101.13798
  9  133.13657
 10  133.58956
 11  133.79150
 12  133.96346
 13  134.02734
 16  148.80599
 17  149.03718
 18  149.14052
 19  149.22836
 20  149.26108
 25   565.45032
 26   566.46182
 27   566.81722
 29   569.65126
 30   570.60809
 31   571.21864
 32   571.75629
 33   572.08434
 34   572.01144
 35   572.61288
 36   574.01623
 37   574.01623
 38   574.70879
 39   575.84787
 40   577.32413
 86   672.15058
 165  704.86506

 Produced by: Guiyun Liang
 Date:        12/08/10
------------------------------------------------------------------------

Contributors

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

Data Classes