lilike_lgy10#cl14.dat
Resolved Specific Ion Data Collections
- Ion
- Cl14+
- Temperature Range
- 3.878 eV → 3.878 x 104 eV
ADF04
- Filename
- lilike_lgy10#cl14.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#cl14.dat
Download data
- Spontaneous Emission: Cl+14(i) → Cl+14(j) + hv
- Electron Impact Excitation: Cl+14(i) + e → Cl+14(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 241423.0 cm-1 |
| 2p1 2P1.5 | 261016.0 cm-1 |
| 3s1 2S0.5 | 3682680.0 cm-1 |
| 3p1 2P0.5 | 3749300.0 cm-1 |
| 3p1 2P1.5 | 3755040.0 cm-1 |
| 3d1 2D1.5 | 3780270.0 cm-1 |
| 3d1 2D2.5 | 3782100.0 cm-1 |
| 4s1 2S0.5 | 4941990.0 cm-1 |
| 4p1 2P0.5 | 4969380.0 cm-1 |
| 4p1 2P1.5 | 4971770.0 cm-1 |
| 4d1 2D1.5 | 4982250.0 cm-1 |
| 4d1 2D2.5 | 4983020.0 cm-1 |
| 4f1 2F2.5 | 4983540.0 cm-1 |
| 4f1 2F3.5 | 4983930.0 cm-1 |
| 5s1 2S0.5 | 5518270.0 cm-1 |
| 5p1 2P0.5 | 5532110.0 cm-1 |
| 5p1 2P1.5 | 5533320.0 cm-1 |
| 5d1 2D1.5 | 5538640.0 cm-1 |
| 5d1 2D2.5 | 5539040.0 cm-1 |
| 5f1 2F2.5 | 5539330.0 cm-1 |
| 5f1 2F3.5 | 5539530.0 cm-1 |
| 5g1 2G3.5 | 5539530.0 cm-1 |
| 5g1 2G4.5 | 5539650.0 cm-1 |
| 1s1 2s2 2S0.5 | 22079800.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 22140500.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 22147100.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 22158900.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 22330500.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 22339800.0 cm-1 |
| 1s1 2p2 4P0.5 | 22400700.0 cm-1 |
| 1s1 2p2 4P1.5 | 22407900.0 cm-1 |
| 1s1 2p2 4P2.5 | 22418700.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 22422800.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 22427400.0 cm-1 |
| 1s1 2p2 2D1.5 | 22532300.0 cm-1 |
| 1s1 2p2 2D2.5 | 22535000.0 cm-1 |
| 1s1 2p2 2P0.5 | 22560400.0 cm-1 |
| 1s1 2p2 2P1.5 | 22576400.0 cm-1 |
| 1s1 2p2 2S0.5 | 22705600.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 25870600.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 25933800.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 25955600.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 25956600.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 25960300.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 25963900.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 25964200.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 26007700.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 26008300.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 26009400.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 26010900.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 26034100.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 26042300.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 26042300.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 26057000.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 26062800.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 26074200.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 26090500.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 26095100.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 26098800.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 26103300.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 26111200.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 26118900.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 26119600.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 26121300.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 26132200.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 26138800.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 26147200.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 26149300.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 26150100.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 26154200.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 26155200.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 26159600.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 26160400.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 26161400.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 26164200.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 26168700.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 26169000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 26169700.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 26175300.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 26189200.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 26192900.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 26193200.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 26194800.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 26196200.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 26196200.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 26202000.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 26204600.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 26212400.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 26214900.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 26216300.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 26218800.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 26219300.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 26245400.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 26253800.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 26254200.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 26254900.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 26255700.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 26261200.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 26293300.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 26295100.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 26300200.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 26309600.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 26313400.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 26332800.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 26336700.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 27192900.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 27213600.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 27223500.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 27224100.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 27225300.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 27233300.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 27233800.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 27245500.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 27245600.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 27245900.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 27246300.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 27256300.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 27256500.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 27261900.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 27262000.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 27262200.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 27262400.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 27265600.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 27265700.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 27341300.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 27350100.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 27355200.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 27363400.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 27367300.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 27367800.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 27369800.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 27373300.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 27376100.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 27379000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 27381000.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 27383500.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 27387000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 27388100.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 27389600.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 27390800.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 27391000.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 27391000.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 27391600.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 27394300.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 27397400.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 27397500.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 27399300.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 27399700.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 27400900.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 27401800.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 27404400.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 27405200.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 27406100.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 27406500.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 27406700.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 27407800.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 27409100.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 27409400.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 27410700.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 27411000.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 27411400.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 27411400.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 27412200.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 27415900.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 27416200.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 27417100.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 27418900.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 27421200.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 27421300.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 27422200.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 27425200.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 27425500.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 27425700.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 27427900.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 27428100.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 27428600.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 27429500.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 27430200.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 27430900.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 27431500.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 27431900.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 27433000.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 27435300.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 27435400.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 27470400.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 27470500.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 27493200.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 27493200.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 27494000.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 27495600.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 27507200.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 27511100.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 27511800.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 27513500.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 27515200.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 27517800.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 27518200.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 27523500.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 27524900.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 27524900.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 27525100.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 27529500.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 27530000.0 cm-1 |
Contributors
- Guiyun Liang
- Nigel Badnell
L+14 17 15 6717792.( ) ------------------------------------------------------------------------ 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 = 1.28113 2S = 1.03933 2P = 0.93783 3S = 1.02650 3P = 0.93079 3D = 0.86475 4S = 1.02509 4P = 0.93044 4D = 0.86662 4F = 1.00570 5S = 1.02722 5P = 0.93204 5D = 0.87059 5F = 0.84887 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 780.0165 Rydbergs (10612.904499 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.010667104 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (26.66776 eV) was used from the last threshold up to 3.123247 Z**2 Rydbergs (8329 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (26.66776 eV) was used from first threshold up to 3.123247 Z**2 Rydbergs (8329 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 = 1.28586 2S = 1.04139 2P = 0.94045 3S = 1.02886 3P = 0.93172 3D = 0.87059 4S = 1.02877 4P = 0.93299 4D = 0.87546 4F = 0.99869 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. 45 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 0 Rydbergs (0.000000 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.02666776 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (26.66776 eV) was used from the last threshold up to 3.123247 Z**2 Rydbergs (8329 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (26.66776 eV) was used from first threshold up to 3.123247 Z**2 Rydbergs (8329 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 2.19305 3 2.37346 4 33.55650 5 34.16158 6 34.21170 7 34.44225 8 34.45683 9 45.03026 10 45.27813 11 45.30455 12 45.39477 13 45.39841 14 45.41026 15 45.41117 Produced by: Guiyun Liang Date: 25/11/10 ------------------------------------------------------------------------