lilike_lgy10#v20.dat

Resolved Specific Ion Data Collections

Ion
V20+
Temperature Range
7.600 eV → 7.600 x 104 eV

ADF04

Filename
lilike_lgy10#v20.dat
Full Path
adf04/copaw#li/lilike_lgy10#v20.dat
Download data
  • Spontaneous Emission: V+20(i) → V+20(j) + hv
  • Electron Impact Excitation: V+20(i) + e → V+20(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 340896.0 cm-1
2p1 2P1.5 415478.0 cm-1
3s1 2S0.5 7121280.0 cm-1
3p1 2P0.5 7215690.0 cm-1
3p1 2P1.5 7237420.0 cm-1
3d1 2D1.5 7274630.0 cm-1
3d1 2D2.5 7281650.0 cm-1
4s1 2S0.5 9569510.0 cm-1
4p1 2P0.5 9608370.0 cm-1
4p1 2P1.5 9617380.0 cm-1
4d1 2D1.5 9632800.0 cm-1
4d1 2D2.5 9635740.0 cm-1
4f1 2F2.5 9636570.0 cm-1
4f1 2F3.5 9638050.0 cm-1
5s1 2S0.5 10692400.0 cm-1
5p1 2P0.5 10712100.0 cm-1
5p1 2P1.5 10716600.0 cm-1
5d1 2D1.5 10724400.0 cm-1
5d1 2D2.5 10725900.0 cm-1
5f1 2F2.5 10726400.0 cm-1
5f1 2F3.5 10727100.0 cm-1
5g1 2G3.5 10727100.0 cm-1
5g1 2G4.5 10727600.0 cm-1
1s1 2s2 2S0.5 41385500.0 cm-1
1s1 2s1 2p1 4P0.5 41468600.0 cm-1
1s1 2s1 2p1 4P1.5 41491400.0 cm-1
1s1 2s1 2p1 4P2.5 41538400.0 cm-1
1s1 2s1 2p1 2P0.5 41747000.0 cm-1
1s1 2s1 2p1 2P1.5 41786100.0 cm-1
1s1 2p2 4P0.5 41858100.0 cm-1
1s1 2s1 2p1 2P0.5 41888500.0 cm-1
1s1 2p2 4P1.5 41889000.0 cm-1
1s1 2s1 2p1 2P1.5 41903400.0 cm-1
1s1 2p2 4P2.5 41925400.0 cm-1
1s1 2p2 2D1.5 42067600.0 cm-1
1s1 2p2 2D2.5 42089000.0 cm-1
1s1 2p2 2P0.5 42094600.0 cm-1
1s1 2p2 2P1.5 42165500.0 cm-1
1s1 2p2 2S0.5 42321200.0 cm-1
1s1 2s1 3s1 4S1.5 48648200.0 cm-1
1s1 2s1 3s1 2S0.5 48738500.0 cm-1
1s1 2s1 3p1 4P0.5 48767400.0 cm-1
1s1 2s1 3p1 4P1.5 48770600.0 cm-1
1s1 2s1 3p1 4P2.5 48786200.0 cm-1
1s1 2s1 3p1 2P1.5 48793100.0 cm-1
1s1 2s1 3p1 2P0.5 48793700.0 cm-1
1s1 2s1 3d1 4D0.5 48852800.0 cm-1
1s1 2s1 3d1 4D1.5 48855300.0 cm-1
1s1 2s1 3d1 4D2.5 48859200.0 cm-1
1s1 2s1 3d1 4D3.5 48864300.0 cm-1
1s1 2s1 3s1 2S0.5 48881000.0 cm-1
1s1 2s1 3d1 2D2.5 48905700.0 cm-1
1s1 2s1 3d1 2D1.5 48905800.0 cm-1
1s1 2p1 3s1 4P0.5 48909000.0 cm-1
1s1 2p1 3s1 4P1.5 48927800.0 cm-1
1s1 2s1 3p1 2P0.5 48963500.0 cm-1
1s1 2p1 3p1 4D0.5 48967400.0 cm-1
1s1 2p1 3s1 4P2.5 48975600.0 cm-1
1s1 2p1 3p1 4D1.5 48981600.0 cm-1
1s1 2s1 3p1 2P1.5 48983600.0 cm-1
1s1 2p1 3p1 4D2.5 49012100.0 cm-1
1s1 2p1 3s1 2P0.5 49014700.0 cm-1
1s1 2p1 3p1 2P1.5 49018000.0 cm-1
1s1 2p1 3p1 2P0.5 49031200.0 cm-1
1s1 2p1 3p1 4P0.5 49053400.0 cm-1
1s1 2p1 3d1 4F1.5 49054400.0 cm-1
1s1 2p1 3p1 4D3.5 49055400.0 cm-1
1s1 2p1 3p1 4S1.5 49062300.0 cm-1
1s1 2p1 3d1 4F2.5 49067900.0 cm-1
1s1 2p1 3s1 2P1.5 49071400.0 cm-1
1s1 2s1 3d1 2D1.5 49076000.0 cm-1
1s1 2s1 3d1 2D2.5 49081000.0 cm-1
1s1 2p1 3p1 4P1.5 49085900.0 cm-1
1s1 2p1 3d1 4F3.5 49090800.0 cm-1
1s1 2p1 3d1 2D2.5 49097900.0 cm-1
1s1 2p1 3p1 2D1.5 49099000.0 cm-1
1s1 2p1 3p1 4P2.5 49099500.0 cm-1
1s1 2p1 3d1 2D1.5 49102400.0 cm-1
1s1 2p1 3d1 4D0.5 49126800.0 cm-1
1s1 2p1 3d1 4F4.5 49128500.0 cm-1
1s1 2p1 3d1 4D1.5 49128800.0 cm-1
1s1 2p1 3d1 4D2.5 49132900.0 cm-1
1s1 2p1 3s1 2P1.5 49134900.0 cm-1
1s1 2p1 3s1 2P0.5 49141100.0 cm-1
1s1 2p1 3p1 2D2.5 49147000.0 cm-1
1s1 2p1 3d1 2F2.5 49157900.0 cm-1
1s1 2p1 3d1 4D3.5 49167400.0 cm-1
1s1 2p1 3p1 2S0.5 49174100.0 cm-1
1s1 2p1 3d1 4P2.5 49183000.0 cm-1
1s1 2p1 3d1 4P1.5 49185100.0 cm-1
1s1 2p1 3d1 4P0.5 49188200.0 cm-1
1s1 2p1 3d1 2F3.5 49198400.0 cm-1
1s1 2p1 3d1 2P1.5 49215000.0 cm-1
1s1 2p1 3p1 2P0.5 49223000.0 cm-1
1s1 2p1 3p1 2D1.5 49224400.0 cm-1
1s1 2p1 3p1 2D2.5 49230500.0 cm-1
1s1 2p1 3d1 2P0.5 49243900.0 cm-1
1s1 2p1 3p1 2P1.5 49248700.0 cm-1
1s1 2p1 3d1 2D1.5 49293600.0 cm-1
1s1 2p1 3p1 2S0.5 49294100.0 cm-1
1s1 2p1 3d1 2D2.5 49298000.0 cm-1
1s1 2p1 3d1 2F3.5 49314400.0 cm-1
1s1 2p1 3d1 2F2.5 49327700.0 cm-1
1s1 2p1 3d1 2P0.5 49341700.0 cm-1
1s1 2p1 3d1 2P1.5 49355500.0 cm-1
1s1 2s1 4s1 4S1.5 51182500.0 cm-1
1s1 2s1 4s1 2S0.5 51212200.0 cm-1
1s1 2s1 4p1 4P0.5 51226100.0 cm-1
1s1 2s1 4p1 4P1.5 51228100.0 cm-1
1s1 2s1 4p1 4P2.5 51233300.0 cm-1
1s1 2s1 4p1 2P1.5 51244000.0 cm-1
1s1 2s1 4p1 2P0.5 51245600.0 cm-1
1s1 2s1 4d1 4D0.5 51262200.0 cm-1
1s1 2s1 4d1 4D1.5 51262800.0 cm-1
1s1 2s1 4d1 4D2.5 51263800.0 cm-1
1s1 2s1 4d1 4D3.5 51265400.0 cm-1
1s1 2s1 4d1 2D2.5 51278500.0 cm-1
1s1 2s1 4d1 2D1.5 51279200.0 cm-1
1s1 2s1 4f1 4F1.5 51287300.0 cm-1
1s1 2s1 4f1 4F2.5 51287600.0 cm-1
1s1 2s1 4f1 4F3.5 51288100.0 cm-1
1s1 2s1 4f1 4F4.5 51288900.0 cm-1
1s1 2s1 4f1 2F3.5 51292700.0 cm-1
1s1 2s1 4f1 2F2.5 51293100.0 cm-1
1s1 2s1 4s1 2S0.5 51393900.0 cm-1
1s1 2p1 4s1 4P0.5 51401900.0 cm-1
1s1 2p1 4s1 4P1.5 51417200.0 cm-1
1s1 2s1 4p1 2P0.5 51428200.0 cm-1
1s1 2p1 4p1 4D0.5 51429500.0 cm-1
1s1 2s1 4p1 2P1.5 51439800.0 cm-1
1s1 2p1 4p1 4D1.5 51441100.0 cm-1
1s1 2p1 4s1 2P0.5 51442200.0 cm-1
1s1 2p1 4p1 4S1.5 51452100.0 cm-1
1s1 2p1 4p1 4D2.5 51458200.0 cm-1
1s1 2p1 4p1 4P0.5 51462800.0 cm-1
1s1 2p1 4d1 4F1.5 51465200.0 cm-1
1s1 2p1 4s1 4P2.5 51469900.0 cm-1
1s1 2s1 4d1 2D1.5 51469900.0 cm-1
1s1 2p1 4p1 2P0.5 51470000.0 cm-1
1s1 2s1 4d1 2D2.5 51473300.0 cm-1
1s1 2p1 4d1 4F2.5 51475700.0 cm-1
1s1 2p1 4p1 2D1.5 51476300.0 cm-1
1s1 2p1 4d1 4D2.5 51483200.0 cm-1
1s1 2p1 4f1 4G2.5 51489000.0 cm-1
1s1 2p1 4d1 4F3.5 51490800.0 cm-1
1s1 2p1 4f1 4F3.5 51491300.0 cm-1
1s1 2s1 4f1 2F2.5 51491300.0 cm-1
1s1 2p1 4d1 2D1.5 51491900.0 cm-1
1s1 2s1 4f1 2F3.5 51492600.0 cm-1
1s1 2p1 4s1 2P1.5 51495400.0 cm-1
1s1 2p1 4d1 4D0.5 51497200.0 cm-1
1s1 2p1 4d1 4D1.5 51498000.0 cm-1
1s1 2p1 4d1 2F2.5 51504200.0 cm-1
1s1 2p1 4f1 2F3.5 51505000.0 cm-1
1s1 2p1 4f1 4F1.5 51505300.0 cm-1
1s1 2p1 4f1 2F2.5 51505800.0 cm-1
1s1 2p1 4f1 4G4.5 51507500.0 cm-1
1s1 2p1 4p1 4D3.5 51507500.0 cm-1
1s1 2p1 4f1 2D2.5 51511000.0 cm-1
1s1 2p1 4p1 4P1.5 51512100.0 cm-1
1s1 2p1 4f1 4D3.5 51513400.0 cm-1
1s1 2p1 4p1 4P2.5 51514100.0 cm-1
1s1 2p1 4p1 2P1.5 51520100.0 cm-1
1s1 2p1 4p1 2D2.5 51536200.0 cm-1
1s1 2p1 4d1 4F4.5 51537300.0 cm-1
1s1 2p1 4d1 2D2.5 51544300.0 cm-1
1s1 2p1 4d1 4D3.5 51544900.0 cm-1
1s1 2p1 4p1 2S0.5 51549300.0 cm-1
1s1 2p1 4d1 4P1.5 51551700.0 cm-1
1s1 2p1 4d1 4P2.5 51552100.0 cm-1
1s1 2p1 4d1 4P0.5 51553600.0 cm-1
1s1 2p1 4d1 2P1.5 51559600.0 cm-1
1s1 2p1 4f1 4G3.5 51560000.0 cm-1
1s1 2p1 4f1 4F4.5 51561000.0 cm-1
1s1 2p1 4f1 4F2.5 51562800.0 cm-1
1s1 2p1 4f1 2G3.5 51563500.0 cm-1
1s1 2p1 4d1 2F3.5 51565100.0 cm-1
1s1 2p1 4f1 4G5.5 51565500.0 cm-1
1s1 2p1 4f1 4D1.5 51567800.0 cm-1
1s1 2p1 4f1 2G4.5 51568500.0 cm-1
1s1 2p1 4f1 4D2.5 51568900.0 cm-1
1s1 2p1 4f1 4D0.5 51571100.0 cm-1
1s1 2p1 4d1 2P0.5 51572800.0 cm-1
1s1 2p1 4f1 2D1.5 51574600.0 cm-1
1s1 2p1 4s1 2P0.5 51609500.0 cm-1
1s1 2p1 4s1 2P1.5 51610000.0 cm-1
1s1 2p1 4p1 2P0.5 51642400.0 cm-1
1s1 2p1 4p1 2D1.5 51642900.0 cm-1
1s1 2p1 4p1 2D2.5 51647300.0 cm-1
1s1 2p1 4p1 2P1.5 51651500.0 cm-1
1s1 2p1 4p1 2S0.5 51664400.0 cm-1
1s1 2p1 4d1 2D1.5 51673300.0 cm-1
1s1 2p1 4d1 2D2.5 51675400.0 cm-1
1s1 2p1 4d1 2F3.5 51676300.0 cm-1
1s1 2p1 4d1 2F2.5 51681800.0 cm-1
1s1 2p1 4f1 2F2.5 51685000.0 cm-1
1s1 2p1 4f1 2F3.5 51686400.0 cm-1
1s1 2p1 4d1 2P0.5 51688600.0 cm-1
1s1 2p1 4d1 2P1.5 51693800.0 cm-1
1s1 2p1 4f1 2G3.5 51694900.0 cm-1
1s1 2p1 4f1 2G4.5 51695200.0 cm-1
1s1 2p1 4f1 2D1.5 51700100.0 cm-1
1s1 2p1 4f1 2D2.5 51702000.0 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 = 1.28224
         2S = 1.04485
         2P = 0.94626
         3S = 1.03172
         3P = 0.93876
         3D = 0.87527
         4S = 1.03036
         4P = 0.93824
         4D = 0.87687
         4F = 1.03745
         5S = 1.03264
         5P = 0.93998
         5D = 0.88083
         5F = 0.85574
         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 1510.1426 Rydbergs (20547.000216 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.0217696 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (54.424 eV) was used
 from the last threshold up to 2.890269 Z**2 Rydbergs (15730 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (54.424 eV) was used
 from first threshold up to 2.890269 Z**2 Rydbergs (15730 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:        13/10/10
------------------------------------------------------------------------
        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 = 1.28730
         2S = 1.04668
         2P = 0.94847
         3S = 1.03453
         3P = 0.94097
         3D = 0.87832
         4S = 1.03422
         4P = 0.94134
         4D = 0.88237
         4F = 1.05011

 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 1370.2852 Rydbergs (18644.100431 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.027212 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (54.424 eV) was used
 from the last threshold up to 2.890269 Z**2 Rydbergs (15730 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (54.424 eV) was used
 from first threshold up to 2.890269 Z**2 Rydbergs (15730 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   3.10227
  3   3.79028
  4  64.86700
  5  65.72669
  6  65.93063
  7  66.25768
  8  66.32192
  9  87.16324
 10  87.52438
 11  87.61040
 12  87.74818
 13  87.77525
 16  97.396587
 17  97.581027
 18  97.624950
 19  97.695482
 20  97.709334
 25  376.46264
 26  377.24633
 27  377.41036
 29  379.76143
 30  380.12594
 31  380.80028
 32  381.04632
 33  381.12833
 34  381.18301
 35  381.41994
 36  382.68660
 37  382.85063
 38  382.86885
 39  383.59786
 40  384.96477

 Produced by: Guiyun Liang
 Date:        23/08/10
------------------------------------------------------------------------

Contributors

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

Data Classes