lilike_lgy10#mn22.dat

Resolved Specific Ion Data Collections

Ion
Mn22+
Temperature Range
9.134 eV → 9.134 x 104 eV

ADF04

Filename
lilike_lgy10#mn22.dat
Full Path
adf04/copaw#li/lilike_lgy10#mn22.dat
Download data
  • Spontaneous Emission: Mn+22(i) → Mn+22(j) + hv
  • Electron Impact Excitation: Mn+22(i) + e → Mn+22(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 374987.0 cm-1
2p1 2P1.5 482134.0 cm-1
3s1 2S0.5 8523870.0 cm-1
3p1 2P0.5 8627750.0 cm-1
3p1 2P1.5 8658880.0 cm-1
3d1 2D1.5 8700180.0 cm-1
3d1 2D2.5 8710300.0 cm-1
4s1 2S0.5 11457300.0 cm-1
4p1 2P0.5 11500100.0 cm-1
4p1 2P1.5 11513000.0 cm-1
4d1 2D1.5 11530100.0 cm-1
4d1 2D2.5 11534300.0 cm-1
4f1 2F2.5 11535200.0 cm-1
4f1 2F3.5 11537400.0 cm-1
5s1 2S0.5 12803400.0 cm-1
5p1 2P0.5 12825000.0 cm-1
5p1 2P1.5 12831400.0 cm-1
5d1 2D1.5 12840100.0 cm-1
5d1 2D2.5 12842200.0 cm-1
5f1 2F2.5 12842700.0 cm-1
5f1 2F3.5 12843800.0 cm-1
5g1 2G3.5 12843800.0 cm-1
5g1 2G4.5 12844500.0 cm-1
1s1 2s2 2S0.5 49184300.0 cm-1
1s1 2s1 2p1 4P0.5 49275100.0 cm-1
1s1 2s1 2p1 4P1.5 49306500.0 cm-1
1s1 2s1 2p1 4P2.5 49375600.0 cm-1
1s1 2s1 2p1 2P0.5 49584600.0 cm-1
1s1 2s1 2p1 2P1.5 49643500.0 cm-1
1s1 2p2 4P0.5 49714700.0 cm-1
1s1 2s1 2p1 2P0.5 49752200.0 cm-1
1s1 2p2 4P1.5 49761700.0 cm-1
1s1 2s1 2p1 2P1.5 49772000.0 cm-1
1s1 2p2 4P2.5 49810700.0 cm-1
1s1 2p2 2D1.5 49958000.0 cm-1
1s1 2p2 2P0.5 49981100.0 cm-1
1s1 2p2 2D2.5 49995100.0 cm-1
1s1 2p2 2P1.5 50087000.0 cm-1
1s1 2p2 2S0.5 50248100.0 cm-1
1s1 2s1 3s1 4S1.5 57860000.0 cm-1
1s1 2s1 3s1 2S0.5 57960200.0 cm-1
1s1 2s1 3p1 4P0.5 57991300.0 cm-1
1s1 2s1 3p1 4P1.5 57995400.0 cm-1
1s1 2s1 3p1 4P2.5 58018500.0 cm-1
1s1 2s1 3p1 2P1.5 58026600.0 cm-1
1s1 2s1 3p1 2P0.5 58027000.0 cm-1
1s1 2s1 3d1 4D0.5 58091200.0 cm-1
1s1 2s1 3d1 4D1.5 58094700.0 cm-1
1s1 2s1 3d1 4D2.5 58100100.0 cm-1
1s1 2s1 3d1 4D3.5 58107300.0 cm-1
1s1 2s1 3s1 2S0.5 58117200.0 cm-1
1s1 2p1 3s1 4P0.5 58147400.0 cm-1
1s1 2s1 3d1 2D2.5 58151400.0 cm-1
1s1 2s1 3d1 2D1.5 58151700.0 cm-1
1s1 2p1 3s1 4P1.5 58172300.0 cm-1
1s1 2s1 3p1 2P0.5 58209300.0 cm-1
1s1 2p1 3p1 4D0.5 58210900.0 cm-1
1s1 2p1 3p1 4D1.5 58229600.0 cm-1
1s1 2s1 3p1 2P1.5 58239300.0 cm-1
1s1 2p1 3s1 4P2.5 58243600.0 cm-1
1s1 2p1 3s1 2P0.5 58263100.0 cm-1
1s1 2p1 3p1 4D2.5 58272800.0 cm-1
1s1 2p1 3p1 4S1.5 58275000.0 cm-1
1s1 2p1 3p1 2P0.5 58296000.0 cm-1
1s1 2p1 3p1 4P0.5 58313300.0 cm-1
1s1 2p1 3d1 4F1.5 58314000.0 cm-1
1s1 2p1 3p1 2P1.5 58329700.0 cm-1
1s1 2p1 3d1 4F2.5 58332000.0 cm-1
1s1 2p1 3p1 4D3.5 58338200.0 cm-1
1s1 2s1 3d1 2D1.5 58340400.0 cm-1
1s1 2p1 3s1 2P1.5 58344600.0 cm-1
1s1 2s1 3d1 2D2.5 58347700.0 cm-1
1s1 2p1 3p1 4P1.5 58362400.0 cm-1
1s1 2p1 3d1 4F3.5 58363600.0 cm-1
1s1 2p1 3d1 2D2.5 58366100.0 cm-1
1s1 2p1 3d1 2D1.5 58375300.0 cm-1
1s1 2p1 3p1 2D1.5 58377600.0 cm-1
1s1 2p1 3p1 4P2.5 58379700.0 cm-1
1s1 2p1 3d1 4D0.5 58398500.0 cm-1
1s1 2p1 3d1 4D1.5 58401000.0 cm-1
1s1 2p1 3d1 2F2.5 58405000.0 cm-1
1s1 2p1 3s1 2P1.5 58414600.0 cm-1
1s1 2p1 3d1 4F4.5 58421600.0 cm-1
1s1 2p1 3s1 2P0.5 58421700.0 cm-1
1s1 2p1 3p1 2D2.5 58436900.0 cm-1
1s1 2p1 3d1 4D2.5 58448400.0 cm-1
1s1 2p1 3p1 2S0.5 58459000.0 cm-1
1s1 2p1 3d1 4D3.5 58460900.0 cm-1
1s1 2p1 3d1 4P2.5 58479300.0 cm-1
1s1 2p1 3d1 4P1.5 58479600.0 cm-1
1s1 2p1 3d1 4P0.5 58483700.0 cm-1
1s1 2p1 3d1 2F3.5 58497700.0 cm-1
1s1 2p1 3d1 2P1.5 58508400.0 cm-1
1s1 2p1 3p1 2P0.5 58512600.0 cm-1
1s1 2p1 3p1 2D1.5 58513600.0 cm-1
1s1 2p1 3p1 2D2.5 58524300.0 cm-1
1s1 2p1 3d1 2P0.5 58546600.0 cm-1
1s1 2p1 3p1 2P1.5 58548700.0 cm-1
1s1 2p1 3p1 2S0.5 58594700.0 cm-1
1s1 2p1 3d1 2D1.5 58597600.0 cm-1
1s1 2p1 3d1 2D2.5 58603000.0 cm-1
1s1 2p1 3d1 2F3.5 58619500.0 cm-1
1s1 2p1 3d1 2F2.5 58637700.0 cm-1
1s1 2p1 3d1 2P0.5 58647100.0 cm-1
1s1 2p1 3d1 2P1.5 58666300.0 cm-1
1s1 2s1 4s1 4S1.5 60887400.0 cm-1
1s1 2s1 4s1 2S0.5 60920300.0 cm-1
1s1 2s1 4p1 4P0.5 60935500.0 cm-1
1s1 2s1 4p1 4P1.5 60938100.0 cm-1
1s1 2s1 4p1 4P2.5 60946000.0 cm-1
1s1 2s1 4p1 2P1.5 60957400.0 cm-1
1s1 2s1 4p1 2P0.5 60959500.0 cm-1
1s1 2s1 4d1 4D0.5 60977800.0 cm-1
1s1 2s1 4d1 4D1.5 60978600.0 cm-1
1s1 2s1 4d1 4D2.5 60980000.0 cm-1
1s1 2s1 4d1 4D3.5 60982300.0 cm-1
1s1 2s1 4d1 2D2.5 60996200.0 cm-1
1s1 2s1 4d1 2D1.5 60997200.0 cm-1
1s1 2s1 4f1 4F1.5 61006200.0 cm-1
1s1 2s1 4f1 4F2.5 61006600.0 cm-1
1s1 2s1 4f1 4F3.5 61007300.0 cm-1
1s1 2s1 4f1 4F4.5 61008500.0 cm-1
1s1 2s1 4f1 2F3.5 61012400.0 cm-1
1s1 2s1 4f1 2F2.5 61013000.0 cm-1
1s1 2s1 4s1 2S0.5 61120700.0 cm-1
1s1 2p1 4s1 4P0.5 61128400.0 cm-1
1s1 2p1 4s1 4P1.5 61148300.0 cm-1
1s1 2p1 4p1 4D0.5 61158700.0 cm-1
1s1 2s1 4p1 2P0.5 61159800.0 cm-1
1s1 2p1 4s1 2P0.5 61174300.0 cm-1
1s1 2p1 4p1 4D1.5 61174500.0 cm-1
1s1 2s1 4p1 2P1.5 61175100.0 cm-1
1s1 2p1 4p1 4S1.5 61186500.0 cm-1
1s1 2p1 4p1 4D2.5 61196700.0 cm-1
1s1 2p1 4p1 4P0.5 61200600.0 cm-1
1s1 2p1 4d1 4F1.5 61200900.0 cm-1
1s1 2s1 4d1 2D1.5 61207100.0 cm-1
1s1 2p1 4p1 2P0.5 61210000.0 cm-1
1s1 2s1 4d1 2D2.5 61212400.0 cm-1
1s1 2p1 4d1 4F2.5 61212900.0 cm-1
1s1 2p1 4p1 2D1.5 61215900.0 cm-1
1s1 2p1 4d1 4D2.5 61220800.0 cm-1
1s1 2p1 4f1 4G2.5 61227700.0 cm-1
1s1 2p1 4s1 4P2.5 61228300.0 cm-1
1s1 2p1 4f1 4F3.5 61230700.0 cm-1
1s1 2s1 4f1 2F3.5 61233300.0 cm-1
1s1 2s1 4f1 2F2.5 61233700.0 cm-1
1s1 2p1 4d1 4F3.5 61234500.0 cm-1
1s1 2p1 4d1 2D1.5 61235100.0 cm-1
1s1 2p1 4d1 4D0.5 61240200.0 cm-1
1s1 2p1 4d1 4D1.5 61240300.0 cm-1
1s1 2p1 4d1 2F2.5 61247900.0 cm-1
1s1 2p1 4f1 4G3.5 61249100.0 cm-1
1s1 2p1 4f1 4F1.5 61249800.0 cm-1
1s1 2p1 4f1 2F2.5 61250600.0 cm-1
1s1 2p1 4f1 4G4.5 61252500.0 cm-1
1s1 2p1 4s1 2P1.5 61254700.0 cm-1
1s1 2p1 4f1 2D2.5 61255800.0 cm-1
1s1 2p1 4f1 4D3.5 61258300.0 cm-1
1s1 2p1 4p1 4D3.5 61271700.0 cm-1
1s1 2p1 4p1 4P1.5 61273700.0 cm-1
1s1 2p1 4p1 4P2.5 61276200.0 cm-1
1s1 2p1 4p1 2P1.5 61285100.0 cm-1
1s1 2p1 4p1 2D2.5 61302100.0 cm-1
1s1 2p1 4d1 4F4.5 61305400.0 cm-1
1s1 2p1 4d1 2D2.5 61311700.0 cm-1
1s1 2p1 4d1 4D3.5 61313000.0 cm-1
1s1 2p1 4p1 2S0.5 61315100.0 cm-1
1s1 2p1 4d1 4P1.5 61319900.0 cm-1
1s1 2p1 4d1 4P2.5 61321300.0 cm-1
1s1 2p1 4d1 4P0.5 61322100.0 cm-1
1s1 2p1 4d1 2P1.5 61328600.0 cm-1
1s1 2p1 4f1 2F3.5 61330300.0 cm-1
1s1 2p1 4f1 4F4.5 61331800.0 cm-1
1s1 2p1 4f1 4F2.5 61333200.0 cm-1
1s1 2p1 4f1 2G3.5 61334600.0 cm-1
1s1 2p1 4d1 2F3.5 61335200.0 cm-1
1s1 2p1 4f1 4G5.5 61337000.0 cm-1
1s1 2p1 4f1 4D1.5 61338700.0 cm-1
1s1 2p1 4f1 2G4.5 61339900.0 cm-1
1s1 2p1 4f1 4D2.5 61340200.0 cm-1
1s1 2p1 4f1 4D0.5 61342400.0 cm-1
1s1 2p1 4d1 2P0.5 61343800.0 cm-1
1s1 2p1 4f1 2D1.5 61346800.0 cm-1
1s1 2p1 4s1 2P0.5 61377600.0 cm-1
1s1 2p1 4s1 2P1.5 61378200.0 cm-1
1s1 2p1 4p1 2P0.5 61414000.0 cm-1
1s1 2p1 4p1 2D1.5 61414600.0 cm-1
1s1 2p1 4p1 2D2.5 61421500.0 cm-1
1s1 2p1 4p1 2P1.5 61427000.0 cm-1
1s1 2p1 4p1 2S0.5 61439500.0 cm-1
1s1 2p1 4d1 2D1.5 61450800.0 cm-1
1s1 2p1 4d1 2D2.5 61453400.0 cm-1
1s1 2p1 4d1 2F3.5 61454100.0 cm-1
1s1 2p1 4d1 2F2.5 61461400.0 cm-1
1s1 2p1 4f1 2F2.5 61464800.0 cm-1
1s1 2p1 4d1 2P0.5 61466500.0 cm-1
1s1 2p1 4f1 2F3.5 61466700.0 cm-1
1s1 2p1 4d1 2P1.5 61473800.0 cm-1
1s1 2p1 4f1 2G3.5 61475500.0 cm-1
1s1 2p1 4f1 2G4.5 61476000.0 cm-1
1s1 2p1 4f1 2D1.5 61480700.0 cm-1
1s1 2p1 4f1 2D2.5 61483400.0 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 = 1.28249
         2S = 1.04607
         2P = 0.94835
         3S = 1.03266
         3P = 0.94163
         3D = 0.87711
         4S = 1.03161
         4P = 0.94008
         4D = 0.87911
         4F = 1.05064
         5S = 1.03319
         5P = 0.94174
         5D = 0.88301
         5F = 0.85701
         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 1822.2936 Rydbergs (24794.126722 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.026341216 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (65.85304 eV) was used
 from the last threshold up to 2.836619 Z**2 Rydbergs (18680 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (65.85304 eV) was used
 from first threshold up to 2.836619 Z**2 Rydbergs (18680 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 = 1.28759
         2S = 1.04785
         2P = 0.95046
         3S = 1.03530
         3P = 0.94222
         3D = 0.88119
         4S = 1.03519
         4P = 0.94294
         4D = 0.88519
         4F = 1.02826

 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 1635.1614 Rydbergs (22248.006008 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.026341216 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (65.85304 eV) was used
 from the last threshold up to 2.836619 Z**2 Rydbergs (18680 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (65.85304 eV) was used
 from first threshold up to 2.836619 Z**2 Rydbergs (18680 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    3.41410
  3    4.40374
  4   77.63449
  5   78.58111
  6   78.87426
  7   79.23412
  8   79.32662
  9  104.35010
 10  104.74778
 11  104.87135
 12  105.02289
 13  105.06198
 16  116.61630
 17  116.81924
 18  116.88257
 19  116.96003
 20  116.98008
 25  447.35922
 26  448.21581
 27  448.46185
 29  451.01340
 30  451.56927
 31  452.23450
 32  452.55344
 33  452.71747
 34  452.75392
 35  453.11843
 36  454.45799
 37  454.74960
 38  454.56734
 39  455.64264
 40  457.06421

 Produced by: Guiyun Liang
 Date:        25/08/10
------------------------------------------------------------------------

Contributors

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

Data Classes