nalike_lgy09#ti11.dat
Resolved Specific Ion Data Collections
- Ion
- Ti11+
- Temperature Range
- 2.482 eV → 2.482 x 104 eV
ADF04
- Filename
- nalike_lgy09#ti11.dat
- Full Path
- adf04/copaw#na/nalike_lgy09#ti11.dat
Download data
- Spontaneous Emission: Ti+11(i) → Ti+11(j) + hv
- Electron Impact Excitation: Ti+11(i) + e → Ti+11(j) + e
| 3s1 2S0.5 | 0.0 cm-1 |
| 3p1 2P0.5 | 208263.0 cm-1 |
| 3p1 2P1.5 | 216371.0 cm-1 |
| 3d1 2D1.5 | 502598.0 cm-1 |
| 3d1 2D2.5 | 503699.0 cm-1 |
| 4s1 2S0.5 | 1131680.0 cm-1 |
| 4p1 2P0.5 | 1212490.0 cm-1 |
| 4p1 2P1.5 | 1215540.0 cm-1 |
| 4d1 2D1.5 | 1319500.0 cm-1 |
| 4d1 2D2.5 | 1319980.0 cm-1 |
| 4f1 2F2.5 | 1357980.0 cm-1 |
| 4f1 2F3.5 | 1358140.0 cm-1 |
| 5s1 2S0.5 | 1603750.0 cm-1 |
| 5p1 2P0.5 | 1643150.0 cm-1 |
| 5p1 2P1.5 | 1644620.0 cm-1 |
| 5d1 2D1.5 | 1694500.0 cm-1 |
| 5d1 2D2.5 | 1694750.0 cm-1 |
| 5f1 2F2.5 | 1714130.0 cm-1 |
| 5f1 2F3.5 | 1714210.0 cm-1 |
| 5g1 2G3.5 | 1715630.0 cm-1 |
| 5g1 2G4.5 | 1715680.0 cm-1 |
| 6s1 2S0.5 | 1845770.0 cm-1 |
| 6p1 2P0.5 | 1867850.0 cm-1 |
| 6p1 2P1.5 | 1868660.0 cm-1 |
| 6d1 2D1.5 | 1896500.0 cm-1 |
| 6d1 2D2.5 | 1896640.0 cm-1 |
| 6f1 2F2.5 | 1907800.0 cm-1 |
| 6f1 2F3.5 | 1907850.0 cm-1 |
| 6g1 2G3.5 | 1908800.0 cm-1 |
| 6g1 2G4.5 | 1908820.0 cm-1 |
| 6h1 2H4.5 | 1908860.0 cm-1 |
| 6h1 2H5.5 | 1908870.0 cm-1 |
| 2p5 3s2 2P1.5 | 3654380.0 cm-1 |
| 2p5 3s2 2P0.5 | 3699020.0 cm-1 |
| 2p5 3s1 3p1 4S1.5 | 3791620.0 cm-1 |
| 2p5 3s1 3p1 4D3.5 | 3815500.0 cm-1 |
| 2p5 3s1 3p1 4D2.5 | 3815850.0 cm-1 |
| 2p5 3s1 3p1 4D1.5 | 3821090.0 cm-1 |
| 2p5 3s1 3p1 4D0.5 | 3830120.0 cm-1 |
| 2p5 3s1 3p1 4P2.5 | 3836480.0 cm-1 |
| 2p5 3s1 3p1 2D1.5 | 3838630.0 cm-1 |
| 2p5 3s1 3p1 4P0.5 | 3851180.0 cm-1 |
| 2p5 3s1 3p1 2P0.5 | 3863550.0 cm-1 |
| 2p5 3s1 3p1 4P1.5 | 3867200.0 cm-1 |
| 2p5 3s1 3p1 2P1.5 | 3876700.0 cm-1 |
| 2p5 3s1 3p1 2D2.5 | 3878050.0 cm-1 |
| 2p5 3s1 3p1 2S0.5 | 3881480.0 cm-1 |
| 2p5 3s1 3p1 2D2.5 | 3910250.0 cm-1 |
| 2p5 3s1 3p1 2P1.5 | 3919960.0 cm-1 |
| 2p5 3s1 3p1 2P0.5 | 3953570.0 cm-1 |
| 2p5 3s1 3p1 2D1.5 | 3957530.0 cm-1 |
| 2p5 3s1 3p1 2S0.5 | 4025440.0 cm-1 |
| 2p5 3p2 2P0.5 | 4036100.0 cm-1 |
| 2p5 3p2 2P1.5 | 4038300.0 cm-1 |
| 2p5 3p2 4P2.5 | 4042090.0 cm-1 |
| 2p5 3p2 2F3.5 | 4045540.0 cm-1 |
| 2p5 3p2 4P1.5 | 4050000.0 cm-1 |
| 2p5 3p2 4P0.5 | 4057220.0 cm-1 |
| 2p5 3p2 2D2.5 | 4060780.0 cm-1 |
| 2p5 3p2 4D3.5 | 4061940.0 cm-1 |
| 2p5 3p2 4D2.5 | 4064520.0 cm-1 |
| 2p5 3p2 2D1.5 | 4065540.0 cm-1 |
| 2p5 3p2 4D0.5 | 4088890.0 cm-1 |
| 2p5 3p2 2F2.5 | 4095630.0 cm-1 |
| 2p5 3p2 2D1.5 | 4095720.0 cm-1 |
| 2p5 3p2 4D1.5 | 4099230.0 cm-1 |
| 2p5 3p2 2S0.5 | 4107220.0 cm-1 |
| 2p5 3p2 4S1.5 | 4112660.0 cm-1 |
| 2p5 3p2 2D2.5 | 4116320.0 cm-1 |
| 2p5 3s1 3d1 4P0.5 | 4118180.0 cm-1 |
| 2p5 3s1 3d1 4P1.5 | 4122730.0 cm-1 |
| 2p5 3s1 3d1 4P2.5 | 4130830.0 cm-1 |
| 2p5 3s1 3d1 4F4.5 | 4131260.0 cm-1 |
| 2p5 3s1 3d1 4F3.5 | 4136140.0 cm-1 |
| 2p5 3s1 3d1 4F2.5 | 4142100.0 cm-1 |
| 2p5 3p2 2P1.5 | 4147520.0 cm-1 |
| 2p5 3s1 3d1 4F1.5 | 4149900.0 cm-1 |
| 2p5 3s1 3d1 4D3.5 | 4155660.0 cm-1 |
| 2p5 3p2 2P0.5 | 4155660.0 cm-1 |
| 2p5 3s1 3d1 2F2.5 | 4158600.0 cm-1 |
| 2p5 3s1 3d1 4D0.5 | 4171520.0 cm-1 |
| 2p5 3s1 3d1 4D1.5 | 4171810.0 cm-1 |
| 2p5 3p2 2P1.5 | 4187350.0 cm-1 |
| 2p5 3s1 3d1 4D2.5 | 4188440.0 cm-1 |
| 2p5 3s1 3d1 2D1.5 | 4193520.0 cm-1 |
| 2p5 3s1 3d1 2F3.5 | 4196100.0 cm-1 |
| 2p5 3s1 3d1 2D2.5 | 4196860.0 cm-1 |
| 2p5 3p2 2P0.5 | 4205830.0 cm-1 |
| 2p5 3s1 3d1 2F3.5 | 4219960.0 cm-1 |
| 2p5 3s1 3d1 2P0.5 | 4227510.0 cm-1 |
| 2p5 3s1 3d1 2P1.5 | 4231150.0 cm-1 |
| 2p5 3s1 3d1 2D2.5 | 4233890.0 cm-1 |
| 2p5 3s1 3d1 2D1.5 | 4254070.0 cm-1 |
| 2p5 3s1 3d1 2F2.5 | 4271040.0 cm-1 |
| 2p5 3s1 3d1 2P0.5 | 4272990.0 cm-1 |
| 2p5 3p1 3d1 4D0.5 | 4288220.0 cm-1 |
| 2p5 3p1 3d1 4D1.5 | 4292330.0 cm-1 |
| 2p5 3s1 3d1 2P1.5 | 4296560.0 cm-1 |
| 2p5 3p1 3d1 4D2.5 | 4298920.0 cm-1 |
| 2p5 3p1 3d1 4D3.5 | 4307520.0 cm-1 |
| 2p5 3p1 3d1 4G5.5 | 4313340.0 cm-1 |
| 2p5 3p1 3d1 4G4.5 | 4313590.0 cm-1 |
| 2p5 3p1 3d1 4G3.5 | 4315660.0 cm-1 |
| 2p5 3p1 3d1 2D2.5 | 4320830.0 cm-1 |
| 2p5 3p1 3d1 2D1.5 | 4323800.0 cm-1 |
| 2p5 3p1 3d1 4G2.5 | 4325750.0 cm-1 |
| 2p5 3p1 3d1 2F3.5 | 4327630.0 cm-1 |
| 2p5 3p1 3d1 2P0.5 | 4332080.0 cm-1 |
| 2p5 3p1 3d1 2G3.5 | 4337540.0 cm-1 |
| 2p5 3p1 3d1 4F4.5 | 4342570.0 cm-1 |
| 2p5 3p1 3d1 4S1.5 | 4345050.0 cm-1 |
| 2p5 3p1 3d1 4P0.5 | 4345520.0 cm-1 |
| 2p5 3p1 3d1 4F1.5 | 4349510.0 cm-1 |
| 2p5 3p1 3d1 4P2.5 | 4351490.0 cm-1 |
| 2p5 3p1 3d1 4D3.5 | 4352290.0 cm-1 |
| 2p5 3p1 3d1 4P1.5 | 4353860.0 cm-1 |
| 2p5 3p1 3d1 4F2.5 | 4354690.0 cm-1 |
| 2p5 3p1 3d1 4F2.5 | 4360060.0 cm-1 |
| 2p5 3p1 3d1 4D1.5 | 4360800.0 cm-1 |
| 2p5 3p1 3d1 4F4.5 | 4362480.0 cm-1 |
| 2p5 3p1 3d1 2F2.5 | 4364400.0 cm-1 |
| 2p5 3p1 3d1 4F3.5 | 4367580.0 cm-1 |
| 2p5 3p1 3d1 4D0.5 | 4369240.0 cm-1 |
| 2p5 3p1 3d1 4D3.5 | 4369840.0 cm-1 |
| 2p5 3p1 3d1 2F2.5 | 4371360.0 cm-1 |
| 2p5 3p1 3d1 2P1.5 | 4371580.0 cm-1 |
| 2p5 3p1 3d1 2F3.5 | 4372920.0 cm-1 |
| 2p5 3p1 3d1 2F2.5 | 4375230.0 cm-1 |
| 2p5 3p1 3d1 4D2.5 | 4377620.0 cm-1 |
| 2p5 3p1 3d1 2D1.5 | 4378850.0 cm-1 |
| 2p5 3p1 3d1 2G4.5 | 4379910.0 cm-1 |
| 2p5 3p1 3d1 4F3.5 | 4382480.0 cm-1 |
| 2p5 3p1 3d1 2D1.5 | 4384340.0 cm-1 |
| 2p5 3p1 3d1 2D2.5 | 4386510.0 cm-1 |
| 2p5 3p1 3d1 4D0.5 | 4391130.0 cm-1 |
| 2p5 3p1 3d1 4P0.5 | 4399150.0 cm-1 |
| 2p5 3p1 3d1 4D1.5 | 4399680.0 cm-1 |
| 2p5 3p1 3d1 4F1.5 | 4406150.0 cm-1 |
| 2p5 3p1 3d1 4D2.5 | 4408390.0 cm-1 |
| 2p5 3p1 3d1 4P1.5 | 4416230.0 cm-1 |
| 2p5 3p1 3d1 2P0.5 | 4416780.0 cm-1 |
| 2p5 3p1 3d1 4P2.5 | 4416820.0 cm-1 |
| 2p5 3p1 3d1 2F3.5 | 4417120.0 cm-1 |
| 2p5 3p1 3d1 2P1.5 | 4418080.0 cm-1 |
| 2p5 3p1 3d1 2D2.5 | 4419290.0 cm-1 |
| 2p5 3p1 3d1 2S0.5 | 4425210.0 cm-1 |
| 2p5 3p1 3d1 2G4.5 | 4425970.0 cm-1 |
| 2p5 3p1 3d1 2D2.5 | 4438560.0 cm-1 |
| 2p5 3p1 3d1 2G3.5 | 4441950.0 cm-1 |
| 2p5 3p1 3d1 2D1.5 | 4446230.0 cm-1 |
| 2p5 3p1 3d1 2P0.5 | 4456030.0 cm-1 |
| 2p5 3p1 3d1 2P1.5 | 4459390.0 cm-1 |
| 2p5 3p1 3d1 2F2.5 | 4463320.0 cm-1 |
| 2p5 3p1 3d1 2P1.5 | 4472780.0 cm-1 |
| 2p5 3p1 3d1 2F3.5 | 4481190.0 cm-1 |
| 2p5 3p1 3d1 2P0.5 | 4488770.0 cm-1 |
| 2p5 3p1 3d1 2D2.5 | 4494570.0 cm-1 |
| 2p5 3p1 3d1 2D1.5 | 4497860.0 cm-1 |
| 2p5 3p1 3d1 2S0.5 | 4509020.0 cm-1 |
| 2p5 3p1 3d1 2D1.5 | 4540710.0 cm-1 |
| 2p5 3p1 3d1 2D2.5 | 4544780.0 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 = 1.40584 2S = 1.08858 2P = 1.03224 3S = 1.02698 3P = 0.99501 3D = 0.99283 4S = 1.01803 4P = 0.98951 4D = 0.98594 4F = 0.95176 5S = 1.01507 5P = 0.98780 5D = 0.98391 5F = 0.95142 5G = 0.94226 6S = 1.01413 6P = 0.98742 6D = 0.98423 6F = 0.95342 6G = 0.94350 6H = 1.16029 An exchange calculation was performed up to J=12 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 132.9436 Rydbergs (1808.830622 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.01646326 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.005000 Z**2 Rydbergs (8.23163 eV) was used from the last threshold up to 0.559427 Z**2 Rydbergs (921 eV) in the excitation calculation. A coarse energy mesh of 0.005000 Z**2 Rydbergs (8.23163 eV) was used from first threshold up to 0.559427 Z**2 Rydbergs (921 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: 17/03/09 ------------------------------------------------------------------------ Result of ICFT R-matrix calculation for inner 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 = 1.40576 2S = 1.08143 2P = 1.02079 3S = 1.15121 3P = 1.11057 3D = 1.14604 An exchange calculation was performed up to J=12 A non-exchange calculation was then performed up to J=40 Followed by a top-up calculation to J -> infinity. 25 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 538.3791 Rydbergs (7325.186035 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.01646326 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (16.46326 eV) was used from the last threshold up to 2.237710 Z**2 Rydbergs (3684 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (16.46326 eV) was used from first threshold up to 2.237710 Z**2 Rydbergs (3684 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: 29/04/09 ------------------------------------------------------------------------