lilike_lgy10#p12.dat
Resolved Specific Ion Data Collections
- Ion
- P12+
- Temperature Range
- 2.912 eV → 2.912 x 104 eV
ADF04
- Filename
- lilike_lgy10#p12.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#p12.dat
Download data
- Spontaneous Emission: P+12(i) → P+12(j) + hv
- Electron Impact Excitation: P+12(i) + e → P+12(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 209010.0 cm-1 |
| 2p1 2P1.5 | 220120.0 cm-1 |
| 3s1 2S0.5 | 2789090.0 cm-1 |
| 3p1 2P0.5 | 2846630.0 cm-1 |
| 3p1 2P1.5 | 2849890.0 cm-1 |
| 3d1 2D1.5 | 2871230.0 cm-1 |
| 3d1 2D2.5 | 2872260.0 cm-1 |
| 4s1 2S0.5 | 3739970.0 cm-1 |
| 4p1 2P0.5 | 3763600.0 cm-1 |
| 4p1 2P1.5 | 3764970.0 cm-1 |
| 4d1 2D1.5 | 3773830.0 cm-1 |
| 4d1 2D2.5 | 3774260.0 cm-1 |
| 4f1 2F2.5 | 3774700.0 cm-1 |
| 4f1 2F3.5 | 3774910.0 cm-1 |
| 5s1 2S0.5 | 4174510.0 cm-1 |
| 5p1 2P0.5 | 4186450.0 cm-1 |
| 5p1 2P1.5 | 4187140.0 cm-1 |
| 5d1 2D1.5 | 4191640.0 cm-1 |
| 5d1 2D2.5 | 4191860.0 cm-1 |
| 5f1 2F2.5 | 4192110.0 cm-1 |
| 5f1 2F3.5 | 4192220.0 cm-1 |
| 5g1 2G3.5 | 4192220.0 cm-1 |
| 5g1 2G4.5 | 4192290.0 cm-1 |
| 1s1 2s2 2S0.5 | 16994900.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 17048500.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 17052300.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 17058900.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 17210800.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 17215900.0 cm-1 |
| 1s1 2p2 4P0.5 | 17271500.0 cm-1 |
| 1s1 2p2 4P1.5 | 17275500.0 cm-1 |
| 1s1 2p2 4P2.5 | 17281800.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 17291500.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 17294300.0 cm-1 |
| 1s1 2p2 2D1.5 | 17382000.0 cm-1 |
| 1s1 2p2 2D2.5 | 17383100.0 cm-1 |
| 1s1 2p2 2P0.5 | 17407500.0 cm-1 |
| 1s1 2p2 2P1.5 | 17416200.0 cm-1 |
| 1s1 2p2 2S0.5 | 17533200.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 19880500.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 19935300.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 19954500.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 19955200.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 19957200.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 19959600.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 19959900.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 19997900.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 19998200.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 19998900.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 19999700.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 20021600.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 20027400.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 20027400.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 20043600.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 20047000.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 20053300.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 20070300.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 20072800.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 20079500.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 20082000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 20086500.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 20092100.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 20092600.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 20092600.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 20108200.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 20109400.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 20116800.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 20121800.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 20121900.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 20124300.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 20124700.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 20127700.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 20127800.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 20130000.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 20131500.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 20132300.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 20135100.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 20135700.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 20143400.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 20151300.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 20157100.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 20157600.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 20158600.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 20159100.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 20159500.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 20162400.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 20167200.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 20171900.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 20173600.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 20174600.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 20175400.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 20179100.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 20201800.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 20206600.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 20209400.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 20209800.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 20210100.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 20213400.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 20241000.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 20242100.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 20248800.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 20255300.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 20257500.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 20276400.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 20278600.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 20886700.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 20904500.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 20913200.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 20913500.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 20914100.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 20921100.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 20921400.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 20931300.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 20931400.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 20931600.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 20931800.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 20940600.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 20940700.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 20945300.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 20945400.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 20945500.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 20945600.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 20948500.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 20948600.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 21014700.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 21024100.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 21027200.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 21033700.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 21034000.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 21035900.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 21041100.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 21043200.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 21045600.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 21046600.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 21049800.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 21050400.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 21052200.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 21052300.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 21054000.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 21055500.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 21056700.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 21057000.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 21058400.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 21059600.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 21059800.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 21060600.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 21063600.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 21064800.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 21064900.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 21065400.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 21068200.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 21068600.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 21068600.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 21069900.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 21070200.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 21070900.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 21071500.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 21072300.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 21072600.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 21073700.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 21073900.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 21074300.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 21074900.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 21075000.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 21078100.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 21078200.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 21079100.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 21079500.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 21080200.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 21081500.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 21082900.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 21083500.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 21084600.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 21084900.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 21085500.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 21086400.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 21087300.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 21087400.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 21088000.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 21088300.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 21088900.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 21089300.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 21091300.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 21091800.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 21123000.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 21123100.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 21142500.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 21142600.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 21142900.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 21144000.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 21154600.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 21157300.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 21157800.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 21159600.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 21160500.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 21162800.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 21163000.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 21168400.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 21168900.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 21168900.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 21169300.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 21173200.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 21173500.0 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 = 1.28056 2S = 1.03623 2P = 0.93338 3S = 1.02393 3P = 0.92664 3D = 0.85968 4S = 1.02267 4P = 0.92629 4D = 0.86165 4F = 0.99434 5S = 1.02410 5P = 0.92792 5D = 0.86559 5F = 0.84554 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. 63 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 645.9965 Rydbergs (8789.428379 eV) A fine energy mesh of 0.000004 Z**2 Rydbergs (0.007837056 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (19.59264 eV) was used from the last threshold up to 3.263981 Z**2 Rydbergs (6395 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (19.59264 eV) was used from first threshold up to 3.263981 Z**2 Rydbergs (6395 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: 14/10/10 ------------------------------------------------------------------------ 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 = 1.28510 2S = 1.03837 2P = 0.93622 3S = 1.02631 3P = 0.92840 3D = 0.86341 4S = 1.02619 4P = 0.92890 4D = 0.86877 4F = 0.99694 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 (0.01959264 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (19.59264 eV) was used from the last threshold up to 3.263981 Z**2 Rydbergs (6395 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (19.59264 eV) was used from first threshold up to 3.263981 Z**2 Rydbergs (6395 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 1.89729 3 1.9996 4 25.4120 5 25.9354 6 25.9657 7 26.1583 8 26.1673 9 34.0818 10 34.2912 11 34.3051 12 34.387 13 34.391 14 34.3934 15 34.3947 19 38.203 20 38.203 25 154.654 26 155.139 27 155.166 28 155.234 29 156.616 30 156.670 31 157.166 32 157.211 33 157.262 34 157.297 35 157.324 36 158.133 37 158.143 38 158.365 39 158.462 40 159.458 Produced by: Guiyun Liang Date: 25/11/10 ------------------------------------------------------------------------