lilike_lgy10#n4.dat
Resolved Specific Ion Data Collections
- Ion
- N4+
- Temperature Range
- 0.431 eV → 4308 eV
ADF04
- Filename
- lilike_lgy10#n4.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#n4.dat
Download data
- Spontaneous Emission: N+4(i) → N+4(j) + hv
- Electron Impact Excitation: N+4(i) + e → N+4(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 81177.0 cm-1 |
| 2p1 2P1.5 | 81428.0 cm-1 |
| 3s1 2S0.5 | 455464.0 cm-1 |
| 3p1 2P0.5 | 477276.0 cm-1 |
| 3p1 2P1.5 | 477350.0 cm-1 |
| 3d1 2D1.5 | 483635.0 cm-1 |
| 3d1 2D2.5 | 483657.0 cm-1 |
| 4s1 2S0.5 | 605550.0 cm-1 |
| 4p1 2P0.5 | 614412.0 cm-1 |
| 4p1 2P1.5 | 614443.0 cm-1 |
| 4d1 2D1.5 | 617080.0 cm-1 |
| 4d1 2D2.5 | 617090.0 cm-1 |
| 4f1 2F2.5 | 617177.0 cm-1 |
| 4f1 2F3.5 | 617182.0 cm-1 |
| 5s1 2S0.5 | 673043.0 cm-1 |
| 5p1 2P0.5 | 677491.0 cm-1 |
| 5p1 2P1.5 | 677507.0 cm-1 |
| 5d1 2D1.5 | 678853.0 cm-1 |
| 5d1 2D2.5 | 678858.0 cm-1 |
| 5f1 2F2.5 | 678907.0 cm-1 |
| 5f1 2F3.5 | 678910.0 cm-1 |
| 5g1 2G3.5 | 678910.0 cm-1 |
| 5g1 2G4.5 | 678912.0 cm-1 |
| 1s1 2s2 2S0.5 | 3325930.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 3352410.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 3352500.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 3352660.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 3409340.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 3409460.0 cm-1 |
| 1s1 2p2 4P0.5 | 3443990.0 cm-1 |
| 1s1 2p2 4P1.5 | 3444080.0 cm-1 |
| 1s1 2p2 4P2.5 | 3444240.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 3450710.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 3450780.0 cm-1 |
| 1s1 2p2 2D1.5 | 3481260.0 cm-1 |
| 1s1 2p2 2D2.5 | 3481260.0 cm-1 |
| 1s1 2p2 2P0.5 | 3488350.0 cm-1 |
| 1s1 2p2 2P1.5 | 3488540.0 cm-1 |
| 1s1 2p2 2S0.5 | 3546690.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 3829710.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 3852050.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 3859860.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 3859870.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 3861210.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 3861230.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 3861260.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 3874980.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 3874980.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 3875000.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 3875010.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 3883090.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 3885920.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 3885920.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 3903300.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 3903350.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 3904380.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 3904460.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 3904600.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 3915440.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 3915500.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 3915590.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 3915720.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 3916330.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 3916350.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 3923100.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 3923130.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 3924240.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 3925760.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 3925970.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 3930630.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 3930680.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 3930760.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 3930850.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 3933960.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 3933980.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 3935590.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 3935640.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 3935720.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 3937700.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 3937900.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 3939840.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 3939890.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 3943770.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 3943790.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 3943820.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 3943860.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 3945200.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 3945400.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 3948220.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 3948390.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 3948440.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 3948470.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 3959900.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 3960010.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 3960610.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 3960620.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 3960630.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 3960720.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 3968720.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 3968750.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 3973700.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 3973750.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 3975310.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 3984310.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 3984360.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 4004070.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 4011440.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 4014240.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 4014250.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 4014260.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 4017040.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 4017050.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 4019530.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 4019540.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 4019540.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 4019540.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 4023070.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 4023070.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 4024660.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 4024660.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 4024660.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 4024660.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 4026850.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 4026850.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 4050880.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 4059130.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 4059140.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 4065470.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 4065480.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 4066480.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 4066560.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 4066700.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 4069840.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 4069850.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 4072420.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 4072580.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 4072990.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 4073040.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 4073120.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 4073220.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 4074110.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 4074170.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 4075770.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 4076790.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 4076840.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 4076910.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 4078360.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 4078410.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 4078480.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 4078570.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 4078720.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 4078760.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 4079910.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 4080060.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 4081060.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 4081070.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 4081100.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 4081140.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 4081930.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 4081960.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 4082160.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 4082170.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 4082180.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 4082210.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 4082760.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 4082820.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 4082860.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 4083880.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 4083930.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 4083990.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 4084070.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 4085040.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 4085170.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 4085360.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 4085510.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 4086040.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 4086100.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 4086150.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 4086170.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 4086420.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 4087260.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 4087350.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 4087710.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 4087810.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 4095540.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 4095540.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 4103110.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 4103120.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 4103250.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 4103280.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 4107470.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 4107480.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 4107760.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 4108700.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 4108730.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 4109180.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 4109180.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 4111450.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 4111450.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 4112220.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 4112240.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 4113650.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 4113660.0 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 = 1.27433 2S = 1.00560 2P = 0.88541 3S = 0.99501 3P = 0.88145 3D = 0.80706 4S = 0.99365 4P = 0.88123 4D = 0.80795 4F = 0.87641 5S = 0.99490 5P = 0.88244 5D = 0.81094 5F = 0.78572 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 96.9868 Rydbergs (1319.602401 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00217696 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (2.17696 eV) was used from the last threshold up to 4.496683 Z**2 Rydbergs (978.91 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (2.17696 eV) was used from first threshold up to 4.496683 Z**2 Rydbergs (978.91 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 = 1.27685 2S = 1.00828 2P = 0.89033 3S = 0.99779 3P = 0.88302 3D = 0.81162 4S = 0.99694 4P = 0.88415 4D = 0.81755 4F = 0.89765 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. 46 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 105.1952 Rydbergs (1431.285891 eV) A fine energy mesh of 0.000020 Z**2 Rydbergs (0.00435392 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (2.17696 eV) was used from the last threshold up to 4.496683 Z**2 Rydbergs (978.91 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (2.17696 eV) was used from first threshold up to 4.496683 Z**2 Rydbergs (978.91 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 0.733235 3 0.735592 4 4.156531 5 4.353721 6 4.354417 7 4.414217 8 4.414417 9 5.525457 10 5.605577 11 5.605876 12 5.630868 13 5.630951 14 5.632171 15 5.632214 16 6.140903 17 6.181128 18 6.181275 19 6.193998 20 6.194043 21 6.194706 22 6.194706 23 6.194814 24 6.194814 28 30.47341 33 31.28863 41 34.78625 51 35.18521 59 35.36955 79 35.61341 87 35.74928 91 35.78874 107 35.61860 Produced by: Guiyun Liang Date: 30/08/10 ------------------------------------------------------------------------