mglike_dcg00#ti10.dat
Resolved Specific Ion Data Collections
- Ion
- Ti10+
- Temperature Range
- 5.213 eV → 521 eV
ADF04
- Filename
- mglike_dcg00#ti10.dat
- Full Path
- adf04/mglike/mglike_dcg00#ti10.dat
Download data
- Spontaneous Emission: Ti+10(i) → Ti+10(j) + hv
- Electron Impact Excitation: Ti+10(i) + e → Ti+10(j) + e
| 3s2(1s) 1S0.0 | 0.0 cm-1 |
| 3s3p(3p) 3P0.0 | 171780.0 cm-1 |
| 3s3p(3p) 3P1.0 | 174197.0 cm-1 |
| 3s3p(3p) 3P2.0 | 179466.0 cm-1 |
| 3s3p(1p) 1P1.0 | 262549.0 cm-1 |
| 3p2(1d) 1D2.0 | 407763.0 cm-1 |
| 3p2(3p) 3P0.0 | 410985.0 cm-1 |
| 3p2(3p) 3P1.0 | 414173.0 cm-1 |
| 3p2(3p) 3P2.0 | 420127.0 cm-1 |
| 3p2(1s) 1S0.0 | 487144.0 cm-1 |
| 3s3d(3d) 3D1.0 | 503003.0 cm-1 |
| 3s3d(3d) 3D2.0 | 503409.0 cm-1 |
| 3s3d(3d) 3D3.0 | 504022.0 cm-1 |
| 3s3d(1d) 1D2.0 | 576663.0 cm-1 |
| 3p3d(3f) 3F2.0 | 685182.0 cm-1 |
| 3p3d(3f) 3F3.0 | 688734.0 cm-1 |
| 3p3d(3f) 3F4.0 | 692844.0 cm-1 |
| 3p3d(1d) 1D2.0 | 695817.0 cm-1 |
| 3p3d(3p) 3P2.0 | 728955.0 cm-1 |
| 3p3d(3d) 3D1.0 | 729808.0 cm-1 |
| 3p3d(3p) 3P0.0 | 733377.0 cm-1 |
| 3p3d(3p) 3P1.0 | 734125.0 cm-1 |
| 3p3d(3d) 3D3.0 | 734726.0 cm-1 |
| 3p3d(3d) 3D2.0 | 734747.0 cm-1 |
| 3p3d(1f) 1F3.0 | 797805.0 cm-1 |
| 3p3d(1p) 1P1.0 | 807592.0 cm-1 |
| 3d2(3f) 3F2.0 | 1013160.0 cm-1 |
| 3d2(3f) 3F3.0 | 1013790.0 cm-1 |
| 3d2(3f) 3F4.0 | 1014590.0 cm-1 |
| 3d2(3p) 3P0.0 | 1040310.0 cm-1 |
| 3d2(3p) 3P2.0 | 1040460.0 cm-1 |
| 3d2(3p) 3P1.0 | 1040540.0 cm-1 |
| 3d2(1d) 1D2.0 | 1041690.0 cm-1 |
| 3d2(1g) 1G4.0 | 1054250.0 cm-1 |
| 3s4s(3s) 3S1.0 | 1054250.0 cm-1 |
| 3d2(1s) 1S0.0 | 1072890.0 cm-1 |
| 3s4s(1s) 1S0.0 | 1115020.0 cm-1 |
| 3s4p(3p) 3P0.0 | 1139990.0 cm-1 |
| 3s4p(3p) 3P1.0 | 1140730.0 cm-1 |
| 3s4p(3p) 3P2.0 | 1142690.0 cm-1 |
| 3s4p(1p) 1P1.0 | 1151620.0 cm-1 |
| 3s4d(3d) 3D1.0 | 1249700.0 cm-1 |
| 3s4d(3d) 3D2.0 | 1249860.0 cm-1 |
| 3s4d(3d) 3D3.0 | 1250120.0 cm-1 |
| 3s4d(1d) 1D2.0 | 1254440.0 cm-1 |
------------------------------------------------------------------------------- See: Griffin D C, Badnell N R, Pindzola M S and Shaw J A 1999 J. Phys. B 32 2139-52 and 4129-31 for a more complete description. From a 25-term, 45-level ICFT R-matrix close coupling calculation. The 1s, 2s, 2p, and 3s orbital were determined from a configuration- average Hartree-Fock (CAHF) calculation on 3s2. The 3p, 3d, 4s, 4p, and 4d orbitals were determined from CAHF calculations on 3s3p, 3s3d, 3s4s, 3s4p, and 3s4d configurations. For the JPI partial waves from J=0.5 to 10.5 and even and odd parity, we performed an LS R-matrix calculation with exchange for the LSPI partial waves with L = 0 to L = 12 and then transformed the k-matrices to intermediate coupling. For the higher partial waves, we performed a no-exchange calculation in LS coupling, with the long-range multipoles included, for all LSPI partial waves from L = 10 to 60; transformed the K-matrices to intermediate-coupling; and topped up. This allowed us to add the partial-wave contributions from J = 11.5 to 58.5. The size of the continuum basis for these calculations was set to 25. The radiative rates for the dipole-allowed transitions were determined from our 45-level CI calculation in the Breit-Pauli approximation. The number of mesh points used in the asymptotic part of the problem was 10031 and the maximum energy was 81 Ry. Donald C. Griffin May 18, 2000 ------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------