lilike_lgy10#ti19.dat
Resolved Specific Ion Data Collections
- Ion
- Ti19+
- Temperature Range
- 6.893 eV → 6.893 x 104 eV
ADF04
- Filename
- lilike_lgy10#ti19.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#ti19.dat
Download data
- Spontaneous Emission: Ti+19(i) → Ti+19(j) + hv
- Electron Impact Excitation: Ti+19(i) + e → Ti+19(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 324057.0 cm-1 |
| 2p1 2P1.5 | 385469.0 cm-1 |
| 3s1 2S0.5 | 6468450.0 cm-1 |
| 3p1 2P0.5 | 6558160.0 cm-1 |
| 3p1 2P1.5 | 6576080.0 cm-1 |
| 3d1 2D1.5 | 6611260.0 cm-1 |
| 3d1 2D2.5 | 6617040.0 cm-1 |
| 4s1 2S0.5 | 8690840.0 cm-1 |
| 4p1 2P0.5 | 8727760.0 cm-1 |
| 4p1 2P1.5 | 8735200.0 cm-1 |
| 4d1 2D1.5 | 8749790.0 cm-1 |
| 4d1 2D2.5 | 8752210.0 cm-1 |
| 4f1 2F2.5 | 8752990.0 cm-1 |
| 4f1 2F3.5 | 8754210.0 cm-1 |
| 5s1 2S0.5 | 9709920.0 cm-1 |
| 5p1 2P0.5 | 9728590.0 cm-1 |
| 5p1 2P1.5 | 9732320.0 cm-1 |
| 5d1 2D1.5 | 9739720.0 cm-1 |
| 5d1 2D2.5 | 9740950.0 cm-1 |
| 5f1 2F2.5 | 9741390.0 cm-1 |
| 5f1 2F3.5 | 9742010.0 cm-1 |
| 5g1 2G3.5 | 9742020.0 cm-1 |
| 5g1 2G4.5 | 9742390.0 cm-1 |
| 1s1 2s2 2S0.5 | 37743100.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 37822500.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 37841600.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 37879900.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 38085500.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 38117100.0 cm-1 |
| 1s1 2p2 4P0.5 | 38188300.0 cm-1 |
| 1s1 2p2 4P1.5 | 38213100.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 38216400.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 38229100.0 cm-1 |
| 1s1 2p2 4P2.5 | 38243900.0 cm-1 |
| 1s1 2p2 2D1.5 | 38382700.0 cm-1 |
| 1s1 2p2 2D2.5 | 38398600.0 cm-1 |
| 1s1 2p2 2P0.5 | 38411000.0 cm-1 |
| 1s1 2p2 2P1.5 | 38468000.0 cm-1 |
| 1s1 2p2 2S0.5 | 38620500.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 44347600.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 44433200.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 44461000.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 44463700.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 44476300.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 44482700.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 44483300.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 44539900.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 44541900.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 44545100.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 44549400.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 44568600.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 44589300.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 44589400.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 44595600.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 44611700.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 44646400.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 44650300.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 44651400.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 44662600.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 44663500.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 44688700.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 44695900.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 44696300.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 44705700.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 44723600.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 44730100.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 44731200.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 44734600.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 44742700.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 44743000.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 44750600.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 44754600.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 44755800.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 44761800.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 44768100.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 44770200.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 44770500.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 44773200.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 44791800.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 44797900.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 44799500.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 44803600.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 44803800.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 44809100.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 44811500.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 44822600.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 44830200.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 44840300.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 44844600.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 44847200.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 44850000.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 44858600.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 44877800.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 44886800.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 44888100.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 44892700.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 44902400.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 44908200.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 44950900.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 44953000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 44954900.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 44971100.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 44982400.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 44998100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 45009600.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 46652200.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 46680400.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 46693600.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 46695300.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 46699500.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 46709800.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 46711100.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 46727000.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 46727500.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 46728300.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 46729600.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 46742300.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 46742800.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 46750400.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 46750700.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 46751100.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 46751800.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 46755500.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 46755900.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 46852900.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 46861000.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 46874200.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 46884900.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 46887300.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 46894900.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 46897200.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 46898800.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 46907600.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 46911900.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 46916700.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 46917400.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 46920100.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 46922900.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 46924000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 46926700.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 46929000.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 46929300.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 46936200.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 46941500.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 46942100.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 46942500.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 46943700.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 46943800.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 46944500.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 46945100.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 46948700.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 46949400.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 46951300.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 46955400.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 46956000.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 46956100.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 46956500.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 46957100.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 46958100.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 46958200.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 46962200.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 46963600.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 46964000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 46979100.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 46979200.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 46986600.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 46986700.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 46992300.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 46993400.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 46993400.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 46995100.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 47000800.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 47001200.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 47001600.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 47003600.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 47004100.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 47005800.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 47005900.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 47008300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 47008800.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 47009200.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 47011300.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 47013200.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 47014600.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 47050700.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 47051100.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 47081800.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 47082200.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 47085700.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 47089400.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 47102200.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 47110200.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 47112000.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 47113000.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 47117700.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 47120800.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 47122000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 47125100.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 47129500.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 47130300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 47130500.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 47135500.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 47137100.0 cm-1 |
Contributors
- Guiyun Liang
- Nigel Badnell
------------------------------------------------------------------------ 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 = 1.28209 2S = 1.04415 2P = 0.94336 3S = 1.03207 3P = 0.93777 3D = 0.87405 4S = 1.02994 4P = 0.93730 4D = 0.87576 4F = 1.00842 5S = 1.03134 5P = 0.93854 5D = 0.88442 5F = 0.87359 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 1373.8060 Rydbergs (18692.004436 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.019647064 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (49.11766 eV) was used from the last threshold up to 2.921556 Z**2 Rydbergs (14350 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (49.11766 eV) was used from first threshold up to 2.921556 Z**2 Rydbergs (14350 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 = 1.28709 2S = 1.04601 2P = 0.94568 3S = 1.03310 3P = 0.93869 3D = 0.88181 4S = 1.03302 4P = 0.93982 4D = 0.88599 4F = 0.99313 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 1246.6065 Rydbergs (16961.328039 eV) A fine energy mesh of 0.000006 Z**2 Rydbergs (0.029470596 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (49.11766 eV) was used from the last threshold up to 2.921556 Z**2 Rydbergs (14350 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (49.11766 eV) was used from first threshold up to 2.921556 Z**2 Rydbergs (14350 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 2.94814 3 3.51445 4 58.92244 5 59.73921 6 59.90706 7 60.21762 8 60.27047 9 79.16195 10 79.50504 11 79.57585 12 79.70671 13 79.72894 14 79.73587 15 79.74498 16 88.44913 17 88.62437 18 88.66054 19 88.72752 20 88.73891 25 343.32897 26 344.08533 27 344.22202 29 346.46373 30 346.76445 31 347.42056 32 347.68483 33 347.63927 34 347.75773 35 347.93087 36 349.17931 37 349.28866 38 349.36156 39 349.97211 40 351.29345 86 407.60975 165 427.20199 Produced by: Guiyun Liang Date: 09/08/10 ------------------------------------------------------------------------