nelike_lgy09#cu19.dat
Resolved Specific Ion Data Collections
- Ion
- Cu19+
- Temperature Range
- 6.893 eV → 6.893 x 104 eV
ADF04
- Filename
- nelike_lgy09#cu19.dat
- Full Path
- adf04/copaw#ne/nelike_lgy09#cu19.dat
Download data
- Spontaneous Emission: Cu+19(i) → Cu+19(j) + hv
- Electron Impact Excitation: Cu+19(i) + e → Cu+19(j) + e
| 2s2 2p6 1S0.0 | 0.0 cm-1 |
| 2s2 2p5 3s1 3P2.0 | 7780670.0 cm-1 |
| 2s2 2p5 3s1 1P1.0 | 7798460.0 cm-1 |
| 2s2 2p5 3s1 3P0.0 | 7948580.0 cm-1 |
| 2s2 2p5 3s1 3P1.0 | 7959060.0 cm-1 |
| 2s2 2p5 3p1 3S1.0 | 8077500.0 cm-1 |
| 2s2 2p5 3p1 3D2.0 | 8106150.0 cm-1 |
| 2s2 2p5 3p1 3D3.0 | 8132770.0 cm-1 |
| 2s2 2p5 3p1 1P1.0 | 8140470.0 cm-1 |
| 2s2 2p5 3p1 3P2.0 | 8160120.0 cm-1 |
| 2s2 2p5 3p1 3P0.0 | 8228980.0 cm-1 |
| 2s2 2p5 3p1 3D1.0 | 8268780.0 cm-1 |
| 2s2 2p5 3p1 3P1.0 | 8308760.0 cm-1 |
| 2s2 2p5 3p1 1D2.0 | 8314340.0 cm-1 |
| 2s2 2p5 3p1 1S0.0 | 8426680.0 cm-1 |
| 2s2 2p5 3d1 3P0.0 | 8518740.0 cm-1 |
| 2s2 2p5 3d1 3P1.0 | 8530590.0 cm-1 |
| 2s2 2p5 3d1 3P2.0 | 8552090.0 cm-1 |
| 2s2 2p5 3d1 3F4.0 | 8552680.0 cm-1 |
| 2s2 2p5 3d1 3F3.0 | 8555640.0 cm-1 |
| 2s2 2p5 3d1 1D2.0 | 8573280.0 cm-1 |
| 2s2 2p5 3d1 3D3.0 | 8587420.0 cm-1 |
| 2s2 2p5 3d1 3D1.0 | 8639710.0 cm-1 |
| 2s2 2p5 3d1 3F2.0 | 8721750.0 cm-1 |
| 2s2 2p5 3d1 3D2.0 | 8733290.0 cm-1 |
| 2s2 2p5 3d1 1F3.0 | 8740290.0 cm-1 |
| 2s2 2p5 3d1 1P1.0 | 8803840.0 cm-1 |
| 2s1 2p6 3s1 3S1.0 | 9097700.0 cm-1 |
| 2s1 2p6 3s1 1S0.0 | 9162080.0 cm-1 |
| 2s1 2p6 3p1 3P0.0 | 9412140.0 cm-1 |
| 2s1 2p6 3p1 3P1.0 | 9417460.0 cm-1 |
| 2s1 2p6 3p1 3P2.0 | 9451000.0 cm-1 |
| 2s1 2p6 3p1 1P1.0 | 9468160.0 cm-1 |
| 2s1 2p6 3d1 3D1.0 | 9850150.0 cm-1 |
| 2s1 2p6 3d1 3D2.0 | 9853700.0 cm-1 |
| 2s1 2p6 3d1 3D3.0 | 9860180.0 cm-1 |
| 2s1 2p6 3d1 1D2.0 | 9905420.0 cm-1 |
| 2s2 2p5 4s1 3P2.0 | 10509900.0 cm-1 |
| 2s2 2p5 4s1 1P1.0 | 10515100.0 cm-1 |
| 2s2 2p5 4p1 3S1.0 | 10631200.0 cm-1 |
| 2s2 2p5 4p1 3D2.0 | 10638100.0 cm-1 |
| 2s2 2p5 4p1 3D3.0 | 10648400.0 cm-1 |
| 2s2 2p5 4p1 1P1.0 | 10651100.0 cm-1 |
| 2s2 2p5 4p1 3P2.0 | 10657500.0 cm-1 |
| 2s2 2p5 4s1 3P0.0 | 10678000.0 cm-1 |
| 2s2 2p5 4s1 3P1.0 | 10680600.0 cm-1 |
| 2s2 2p5 4p1 3P0.0 | 10695600.0 cm-1 |
| 2s2 2p5 4d1 3P0.0 | 10792600.0 cm-1 |
| 2s2 2p5 4d1 3P1.0 | 10797400.0 cm-1 |
| 2s2 2p5 4p1 3D1.0 | 10803900.0 cm-1 |
| 2s2 2p5 4d1 3F4.0 | 10804200.0 cm-1 |
| 2s2 2p5 4d1 3F3.0 | 10804900.0 cm-1 |
| 2s2 2p5 4d1 3P2.0 | 10805300.0 cm-1 |
| 2s2 2p5 4d1 1D2.0 | 10811200.0 cm-1 |
| 2s2 2p5 4d1 3D3.0 | 10816300.0 cm-1 |
| 2s2 2p5 4p1 3P1.0 | 10818400.0 cm-1 |
| 2s2 2p5 4p1 1D2.0 | 10820800.0 cm-1 |
| 2s2 2p5 4p1 1S0.0 | 10839900.0 cm-1 |
| 2s2 2p5 4d1 1P1.0 | 10841800.0 cm-1 |
| 2s2 2p5 4f1 3D1.0 | 10880200.0 cm-1 |
| 2s2 2p5 4f1 1G4.0 | 10881400.0 cm-1 |
| 2s2 2p5 4f1 3D2.0 | 10882200.0 cm-1 |
| 2s2 2p5 4f1 3G5.0 | 10882600.0 cm-1 |
| 2s2 2p5 4f1 1D2.0 | 10886100.0 cm-1 |
| 2s2 2p5 4f1 3F3.0 | 10886100.0 cm-1 |
| 2s2 2p5 4f1 1F3.0 | 10886800.0 cm-1 |
| 2s2 2p5 4f1 3F4.0 | 10888500.0 cm-1 |
| 2s2 2p5 4d1 3F2.0 | 10971500.0 cm-1 |
| 2s2 2p5 4d1 3D2.0 | 10975700.0 cm-1 |
| 2s2 2p5 4d1 1F3.0 | 10978900.0 cm-1 |
| 2s2 2p5 4d1 3D1.0 | 10996300.0 cm-1 |
| 2s2 2p5 4f1 3G3.0 | 11051100.0 cm-1 |
| 2s2 2p5 4f1 3G4.0 | 11053100.0 cm-1 |
| 2s2 2p5 4f1 3F2.0 | 11053100.0 cm-1 |
| 2s2 2p5 4f1 3D3.0 | 11053900.0 cm-1 |
| 2s2 2p5 5s1 3P2.0 | 11689300.0 cm-1 |
| 2s2 2p5 5s1 1P1.0 | 11691900.0 cm-1 |
| 2s2 2p5 5p1 3S1.0 | 11747500.0 cm-1 |
| 2s2 2p5 5p1 3D2.0 | 11753300.0 cm-1 |
| 2s2 2p5 5p1 3D3.0 | 11758300.0 cm-1 |
| 2s2 2p5 5p1 1P1.0 | 11759200.0 cm-1 |
| 2s2 2p5 5p1 3P2.0 | 11762700.0 cm-1 |
| 2s2 2p5 5p1 1S0.0 | 11781200.0 cm-1 |
| 2s1 2p6 4s1 3S1.0 | 11814400.0 cm-1 |
| 2s2 2p5 5d1 3P0.0 | 11828600.0 cm-1 |
| 2s2 2p5 5d1 3P1.0 | 11831000.0 cm-1 |
| 2s1 2p6 4s1 1S0.0 | 11831900.0 cm-1 |
| 2s2 2p5 5d1 3F4.0 | 11834400.0 cm-1 |
| 2s2 2p5 5d1 3F3.0 | 11834500.0 cm-1 |
| 2s2 2p5 5d1 3P2.0 | 11834900.0 cm-1 |
| 2s2 2p5 5d1 1D2.0 | 11837400.0 cm-1 |
| 2s2 2p5 5d1 3D3.0 | 11840000.0 cm-1 |
| 2s2 2p5 5d1 1P1.0 | 11851500.0 cm-1 |
| 2s2 2p5 5s1 3P0.0 | 11856700.0 cm-1 |
| 2s2 2p5 5s1 3P1.0 | 11859700.0 cm-1 |
| 2s2 2p5 5f1 3D1.0 | 11870900.0 cm-1 |
| 2s2 2p5 5f1 3D2.0 | 11872200.0 cm-1 |
| 2s2 2p5 5f1 1G4.0 | 11872700.0 cm-1 |
| 2s2 2p5 5f1 3G5.0 | 11873400.0 cm-1 |
| 2s2 2p5 5f1 3D3.0 | 11874500.0 cm-1 |
| 2s2 2p5 5f1 1D2.0 | 11875000.0 cm-1 |
| 2s2 2p5 5f1 1F3.0 | 11875100.0 cm-1 |
| 2s2 2p5 5g1 3F2.0 | 11876100.0 cm-1 |
| 2s2 2p5 5f1 3F4.0 | 11876100.0 cm-1 |
| 2s2 2p5 5g1 3F3.0 | 11876400.0 cm-1 |
| 2s2 2p5 5g1 1H5.0 | 11877700.0 cm-1 |
| 2s2 2p5 5g1 3G3.0 | 11878100.0 cm-1 |
| 2s2 2p5 5g1 3H6.0 | 11878400.0 cm-1 |
| 2s2 2p5 5g1 1G4.0 | 11878500.0 cm-1 |
| 2s2 2p5 5g1 3G4.0 | 11878900.0 cm-1 |
| 2s2 2p5 5g1 3G5.0 | 11879600.0 cm-1 |
| 2s2 2p5 5p1 3D1.0 | 11920500.0 cm-1 |
| 2s2 2p5 5p1 1D2.0 | 11928400.0 cm-1 |
| 2s2 2p5 5p1 3P1.0 | 11928400.0 cm-1 |
| 2s2 2p5 5p1 3P0.0 | 11935300.0 cm-1 |
| 2s1 2p6 4p1 3P0.0 | 11939900.0 cm-1 |
| 2s1 2p6 4p1 3P1.0 | 11940500.0 cm-1 |
| 2s1 2p6 4p1 3P2.0 | 11952300.0 cm-1 |
| 2s1 2p6 4p1 1P1.0 | 11958300.0 cm-1 |
| 2s2 2p5 5d1 3F2.0 | 12002000.0 cm-1 |
| 2s2 2p5 5d1 3D2.0 | 12004300.0 cm-1 |
| 2s2 2p5 5d1 1F3.0 | 12005600.0 cm-1 |
| 2s2 2p5 5d1 3D1.0 | 12013200.0 cm-1 |
| 2s2 2p5 5f1 3G3.0 | 12041400.0 cm-1 |
| 2s2 2p5 5f1 3F3.0 | 12041800.0 cm-1 |
| 2s2 2p5 5f1 3F2.0 | 12042000.0 cm-1 |
| 2s2 2p5 5f1 3G4.0 | 12042600.0 cm-1 |
| 2s2 2p5 5g1 1F3.0 | 12045200.0 cm-1 |
| 2s2 2p5 5g1 3F4.0 | 12045700.0 cm-1 |
| 2s2 2p5 5g1 3H4.0 | 12046400.0 cm-1 |
| 2s2 2p5 5g1 3H5.0 | 12047000.0 cm-1 |
| 2s1 2p6 4d1 3D1.0 | 12102900.0 cm-1 |
| 2s1 2p6 4d1 3D2.0 | 12104500.0 cm-1 |
| 2s1 2p6 4d1 3D3.0 | 12107400.0 cm-1 |
| 2s1 2p6 4d1 1D2.0 | 12122200.0 cm-1 |
| 2s1 2p6 4f1 3F2.0 | 12181400.0 cm-1 |
| 2s1 2p6 4f1 3F3.0 | 12182300.0 cm-1 |
| 2s1 2p6 4f1 3F4.0 | 12183700.0 cm-1 |
| 2s1 2p6 4f1 1F3.0 | 12184500.0 cm-1 |
| 2s2 2p5 6s1 3P2.0 | 12312900.0 cm-1 |
| 2s2 2p5 6s1 1P1.0 | 12314200.0 cm-1 |
| 2s2 2p5 6p1 3S1.0 | 12347600.0 cm-1 |
| 2s2 2p5 6p1 3D2.0 | 12349000.0 cm-1 |
| 2s2 2p5 6p1 3D3.0 | 12351700.0 cm-1 |
| 2s2 2p5 6p1 1P1.0 | 12352500.0 cm-1 |
| 2s2 2p5 6p1 3P2.0 | 12354000.0 cm-1 |
| 2s2 2p5 6p1 1S0.0 | 12365000.0 cm-1 |
| 2s2 2p5 6d1 3P0.0 | 12391300.0 cm-1 |
| 2s2 2p5 6d1 3P1.0 | 12392600.0 cm-1 |
| 2s2 2p5 6d1 3F4.0 | 12394200.0 cm-1 |
| 2s2 2p5 6d1 3F3.0 | 12394400.0 cm-1 |
| 2s2 2p5 6d1 3D2.0 | 12394700.0 cm-1 |
| 2s2 2p5 6d1 1D2.0 | 12396000.0 cm-1 |
| 2s2 2p5 6d1 3D3.0 | 12397400.0 cm-1 |
| 2s2 2p5 6d1 1P1.0 | 12405000.0 cm-1 |
| 2s2 2p5 6s1 3P0.0 | 12479900.0 cm-1 |
| 2s2 2p5 6s1 3P1.0 | 12480600.0 cm-1 |
| 2s2 2p5 6p1 3D1.0 | 12515400.0 cm-1 |
| 2s2 2p5 6p1 3P1.0 | 12519100.0 cm-1 |
| 2s2 2p5 6p1 1D2.0 | 12519800.0 cm-1 |
| 2s2 2p5 6p1 3P0.0 | 12522600.0 cm-1 |
| 2s2 2p5 6d1 3F2.0 | 12560900.0 cm-1 |
| 2s2 2p5 6d1 3P2.0 | 12562000.0 cm-1 |
| 2s2 2p5 6d1 1F3.0 | 12562900.0 cm-1 |
| 2s2 2p5 6d1 3D1.0 | 12566700.0 cm-1 |
| 2s2 2p5 7s1 3P2.0 | 12677100.0 cm-1 |
| 2s2 2p5 7s1 1P1.0 | 12677900.0 cm-1 |
| 2s2 2p5 7p1 3S1.0 | 12698600.0 cm-1 |
| 2s2 2p5 7p1 3D2.0 | 12699500.0 cm-1 |
| 2s2 2p5 7p1 3D3.0 | 12701100.0 cm-1 |
| 2s2 2p5 7p1 1P1.0 | 12701600.0 cm-1 |
| 2s2 2p5 7p1 3P2.0 | 12702500.0 cm-1 |
| 2s2 2p5 7p1 1S0.0 | 12709400.0 cm-1 |
| 2s2 2p5 7d1 3P0.0 | 12725700.0 cm-1 |
| 2s2 2p5 7d1 3P1.0 | 12726500.0 cm-1 |
| 2s2 2p5 7d1 3F4.0 | 12727400.0 cm-1 |
| 2s2 2p5 7d1 3F3.0 | 12727500.0 cm-1 |
| 2s2 2p5 7d1 3D2.0 | 12727700.0 cm-1 |
| 2s2 2p5 7d1 1D2.0 | 12728500.0 cm-1 |
| 2s2 2p5 7d1 3D3.0 | 12729300.0 cm-1 |
| 2s2 2p5 7d1 1P1.0 | 12734200.0 cm-1 |
| 2s2 2p5 7s1 3P0.0 | 12844100.0 cm-1 |
| 2s2 2p5 7s1 3P1.0 | 12844500.0 cm-1 |
| 2s2 2p5 7p1 3D1.0 | 12866100.0 cm-1 |
| 2s2 2p5 7p1 3P1.0 | 12868300.0 cm-1 |
| 2s2 2p5 7p1 1D2.0 | 12868800.0 cm-1 |
| 2s2 2p5 7p1 3P0.0 | 12870400.0 cm-1 |
| 2s2 2p5 7d1 3F2.0 | 12894200.0 cm-1 |
| 2s2 2p5 7d1 3P2.0 | 12894900.0 cm-1 |
| 2s2 2p5 7d1 1F3.0 | 12895500.0 cm-1 |
| 2s2 2p5 7d1 3D1.0 | 12897800.0 cm-1 |
| 2s1 2p6 5s1 3S1.0 | 12989400.0 cm-1 |
| 2s1 2p6 5s1 1S0.0 | 12997700.0 cm-1 |
| 2s1 2p6 5p1 3P0.0 | 13052100.0 cm-1 |
| 2s1 2p6 5p1 3P1.0 | 13052900.0 cm-1 |
| 2s1 2p6 5p1 3P2.0 | 13058800.0 cm-1 |
| 2s1 2p6 5p1 1P1.0 | 13061200.0 cm-1 |
| 2s1 2p6 5d1 3D1.0 | 13131700.0 cm-1 |
| 2s1 2p6 5d1 3D2.0 | 13132400.0 cm-1 |
| 2s1 2p6 5d1 3D3.0 | 13133600.0 cm-1 |
| 2s1 2p6 5d1 1D2.0 | 13140900.0 cm-1 |
| 2s1 2p6 5f1 3F2.0 | 13170400.0 cm-1 |
| 2s1 2p6 5f1 3F3.0 | 13170600.0 cm-1 |
| 2s1 2p6 5f1 3F4.0 | 13171200.0 cm-1 |
| 2s1 2p6 5f1 1F3.0 | 13172200.0 cm-1 |
| 2s1 2p6 5g1 3G3.0 | 13175100.0 cm-1 |
| 2s1 2p6 5g1 3G4.0 | 13175100.0 cm-1 |
| 2s1 2p6 5g1 3G5.0 | 13175600.0 cm-1 |
| 2s1 2p6 5g1 1G4.0 | 13175600.0 cm-1 |
U+19 29 20 12437070.( ) ------------------------------------------------------------------------ Result of ICFT R-matrix calculation +++++++++++++++++++++++++++++++++++ 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 = 1.00000 2S = 1.39467 2P = 1.09579 3S = 1.30170 3P = 1.10729 3D = 1.06765 4S = 1.000 4P = 1.000 4D = 1.000 4F = 1.000 5S = 1.000 5P = 1.000 5D = 1.000 5F = 1.000 5G = 1.000 6S = 1.000 6P = 1.000 6D = 1.000 7S = 1.000 7P = 1.000 7D = 1.000 An exchange calculation was performed up to J=11.5 A non-exchange calculation was then performed up to J=39.5 Followed by a top-up calculation to J -> infinity. 60 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 469.6206 Rydbergs (6389.657884 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.04911766 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (9.823532 eV) was used from the last threshold up to 0.941820 Z**2 Rydbergs (4626 eV) in the excitation calculation. A coarse energy mesh of 0.002000 Z**2 Rydbergs (9.823532 eV) was used from first threshold up to 0.941820 Z**2 Rydbergs (4626 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: 09/11/09 ------------------------------------------------------------------------