lilike_lgy10#cr21.dat
Resolved Specific Ion Data Collections
- Ion
- Cr21+
- Temperature Range
- 8.341 eV → 8.341 x 104 eV
ADF04
- Filename
- lilike_lgy10#cr21.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#cr21.dat
Download data
- Spontaneous Emission: Cr+21(i) → Cr+21(j) + hv
- Electron Impact Excitation: Cr+21(i) + e → Cr+21(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 357874.0 cm-1 |
| 2p1 2P1.5 | 447633.0 cm-1 |
| 3s1 2S0.5 | 7806360.0 cm-1 |
| 3p1 2P0.5 | 7905500.0 cm-1 |
| 3p1 2P1.5 | 7931610.0 cm-1 |
| 3d1 2D1.5 | 7970860.0 cm-1 |
| 3d1 2D2.5 | 7979320.0 cm-1 |
| 4s1 2S0.5 | 10491600.0 cm-1 |
| 4p1 2P0.5 | 10532400.0 cm-1 |
| 4p1 2P1.5 | 10543200.0 cm-1 |
| 4d1 2D1.5 | 10559500.0 cm-1 |
| 4d1 2D2.5 | 10563000.0 cm-1 |
| 4f1 2F2.5 | 10563900.0 cm-1 |
| 4f1 2F3.5 | 10565700.0 cm-1 |
| 5s1 2S0.5 | 11723500.0 cm-1 |
| 5p1 2P0.5 | 11744100.0 cm-1 |
| 5p1 2P1.5 | 11749500.0 cm-1 |
| 5d1 2D1.5 | 11757800.0 cm-1 |
| 5d1 2D2.5 | 11759600.0 cm-1 |
| 5f1 2F2.5 | 11760100.0 cm-1 |
| 5f1 2F3.5 | 11761000.0 cm-1 |
| 5g1 2G3.5 | 11761000.0 cm-1 |
| 5g1 2G4.5 | 11761500.0 cm-1 |
| 1s1 2s2 2S0.5 | 45199100.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 45286000.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 45312800.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 45370100.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 45579800.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 45628000.0 cm-1 |
| 1s1 2p2 4P0.5 | 45700100.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 45733500.0 cm-1 |
| 1s1 2p2 4P1.5 | 45738300.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 45750700.0 cm-1 |
| 1s1 2p2 4P2.5 | 45780800.0 cm-1 |
| 1s1 2p2 2D1.5 | 45925800.0 cm-1 |
| 1s1 2p2 2P0.5 | 45951100.0 cm-1 |
| 1s1 2p2 2D2.5 | 45954100.0 cm-1 |
| 1s1 2p2 2P1.5 | 46038100.0 cm-1 |
| 1s1 2p2 2S0.5 | 46196800.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 53152100.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 53247200.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 53277300.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 53280900.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 53300000.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 53307500.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 53308000.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 53369700.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 53372700.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 53377200.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 53383300.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 53397000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 53426100.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 53426100.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 53426300.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 53447800.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 53484200.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 53487000.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 53503400.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 53506400.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 53508900.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 53536700.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 53539900.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 53544100.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 53561100.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 53580900.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 53581800.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 53593400.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 53593900.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 53597400.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 53605000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 53605600.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 53611700.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 53621200.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 53624500.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 53629600.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 53634300.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 53636200.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 53636400.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 53660100.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 53662400.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 53666400.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 53671400.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 53671600.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 53678300.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 53688500.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 53699500.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 53710600.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 53713300.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 53727500.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 53728900.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 53732400.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 53744500.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 53758100.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 53764600.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 53765900.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 53774000.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 53791600.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 53795200.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 53841000.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 53842100.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 53847100.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 53863500.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 53879100.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 53891000.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 53907400.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 55927300.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 55958600.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 55973200.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 55975400.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 55981900.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 55992900.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 55994800.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 56012200.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 56012900.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 56014100.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 56016000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 56029600.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 56030300.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 56038900.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 56039300.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 56039900.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 56040900.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 56044700.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 56045200.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 56149600.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 56157400.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 56175000.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 56186300.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 56186400.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 56199600.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 56200000.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 56200500.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 56211500.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 56219600.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 56223900.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 56225200.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 56230600.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 56232100.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 56234900.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 56235200.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 56238200.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 56240200.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 56246200.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 56250400.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 56253100.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 56254000.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 56254700.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 56255100.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 56255600.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 56260800.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 56260900.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 56266500.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 56268000.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 56269100.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 56269600.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 56270200.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 56272000.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 56275600.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 56277700.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 56280800.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 56284100.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 56286300.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 56293700.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 56310200.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 56312400.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 56319100.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 56320000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 56323300.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 56326900.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 56327700.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 56328900.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 56335100.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 56336200.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 56337400.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 56339000.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 56340100.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 56341200.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 56342300.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 56344300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 56345200.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 56345500.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 56347800.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 56349400.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 56351700.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 56384800.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 56385400.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 56419500.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 56420000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 56425600.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 56430400.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 56443100.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 56453200.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 56455500.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 56456300.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 56462700.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 56466000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 56467600.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 56468700.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 56474900.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 56476300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 56476700.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 56481500.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 56483800.0 cm-1 |
Contributors
- Guiyun Liang
- Nigel Badnell
R+21 24 22 13800147.( ) ------------------------------------------------------------------------ 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 = 1.28236 2S = 1.04549 2P = 0.94745 3S = 1.03251 3P = 0.93970 3D = 0.87677 4S = 1.03066 4P = 0.93913 4D = 0.87820 4F = 1.03462 5S = 1.03234 5P = 0.94087 5D = 0.88204 5F = 0.85563 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 1671.4105 Rydbergs (22741.211263 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.024000984 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used from the last threshold up to 2.851550 Z**2 Rydbergs (17110 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used from first threshold up to 2.851550 Z**2 Rydbergs (17110 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 = 1.28744 2S = 1.04729 2P = 0.94961 3S = 1.03408 3P = 0.94043 3D = 0.88409 4S = 1.03412 4P = 0.94162 4D = 0.88829 4F = 1.03573 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 1499.8035 Rydbergs (20406.326421 eV) A fine energy mesh of 0.000005 Z**2 Rydbergs (0.03000123 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used from the last threshold up to 2.851550 Z**2 Rydbergs (17110 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used from first threshold up to 2.851550 Z**2 Rydbergs (17110 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 3.25756 3 4.08607 4 71.10243 5 72.00541 6 72.25090 7 72.59445 8 72.67172 9 95.557285 10 95.936555 11 96.040075 12 96.184784 13 96.217407 16 106.78355 17 106.97719 18 107.03014 19 107.10413 20 107.12090 25 411.12724 26 411.94738 27 412.14786 29 414.60828 30 415.06392 31 415.72914 32 416.01163 33 416.13921 34 416.17566 35 416.46727 36 417.77949 37 417.92529 38 418.00731 39 418.81834 40 420.21258 84 488.44825 96 489.08614 97 489.16815 99 489.32307 102 489.85160 103 490.00652 190 513.35318 Produced by: Guiyun Liang Date: 23/08/10 ------------------------------------------------------------------------