lilike_lgy10#b2.dat
Resolved Specific Ion Data Collections
- Ion
- B2+
- Temperature Range
- 0.155 eV → 1551 eV
ADF04
- Filename
- lilike_lgy10#b2.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#b2.dat
Download data
- Spontaneous Emission: B+2(i) → B+2(j) + hv
- Electron Impact Excitation: B+2(i) + e → B+2(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 48827.0 cm-1 |
| 2p1 2P1.5 | 48859.0 cm-1 |
| 3s1 2S0.5 | 179606.0 cm-1 |
| 3p1 2P0.5 | 192487.0 cm-1 |
| 3p1 2P1.5 | 192496.0 cm-1 |
| 3d1 2D1.5 | 195352.0 cm-1 |
| 3d1 2D2.5 | 195354.0 cm-1 |
| 4s1 2S0.5 | 236985.0 cm-1 |
| 4p1 2P0.5 | 242172.0 cm-1 |
| 4p1 2P1.5 | 242176.0 cm-1 |
| 4d1 2D1.5 | 243385.0 cm-1 |
| 4d1 2D2.5 | 243386.0 cm-1 |
| 4f1 2F2.5 | 243414.0 cm-1 |
| 4f1 2F3.5 | 243415.0 cm-1 |
| 5s1 2S0.5 | 262408.0 cm-1 |
| 5p1 2P0.5 | 264998.0 cm-1 |
| 5p1 2P1.5 | 265000.0 cm-1 |
| 5d1 2D1.5 | 265620.0 cm-1 |
| 5d1 2D2.5 | 265620.0 cm-1 |
| 5f1 2F2.5 | 265636.0 cm-1 |
| 5f1 2F3.5 | 265637.0 cm-1 |
| 5g1 2G3.5 | 265637.0 cm-1 |
| 5g1 2G4.5 | 265637.0 cm-1 |
| 1s1 2s2 2S0.5 | 1566640.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 1586890.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 1586900.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 1586920.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 1617960.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 1617980.0 cm-1 |
| 1s1 2p2 4P0.5 | 1647530.0 cm-1 |
| 1s1 2p2 4P1.5 | 1647540.0 cm-1 |
| 1s1 2p2 4P2.5 | 1647560.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 1649510.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 1649510.0 cm-1 |
| 1s1 2p2 2D1.5 | 1667700.0 cm-1 |
| 1s1 2p2 2D2.5 | 1667700.0 cm-1 |
| 1s1 2p2 2P0.5 | 1669550.0 cm-1 |
| 1s1 2p2 2P1.5 | 1669570.0 cm-1 |
| 1s1 2p2 2S0.5 | 1710690.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 1781580.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 1795820.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 1800380.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 1800380.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 1802260.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 1802260.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 1802260.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 1809420.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 1809420.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 1809420.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 1809420.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 1813180.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 1815950.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 1815950.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 1826090.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 1826100.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 1834950.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 1834960.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 1834980.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 1836840.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 1836840.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 1839820.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 1839830.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 1839990.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 1840000.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 1840010.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 1840020.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 1844980.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 1845610.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 1845640.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 1848470.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 1848480.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 1848480.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 1848500.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 1851400.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 1851410.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 1851420.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 1851420.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 1851870.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 1851890.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 1854770.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 1855140.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 1855160.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 1855270.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 1855350.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 1855360.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 1855360.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 1857510.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 1857510.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 1857510.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 1857520.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 1858350.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 1858360.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 1858360.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 1860090.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 1861640.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 1861650.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 1862940.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 1862950.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 1862950.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 1863550.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 1863550.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 1863550.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 1863550.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 1865160.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 1865160.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 1865600.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 1865600.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 1866370.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 1866380.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 1866860.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 1866860.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 1867350.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 1867350.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 1867350.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 1867350.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 1868390.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 1868400.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 1869110.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 1869120.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 1876050.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 1876080.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 1876080.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 1879140.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 1879140.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 1882540.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 1887230.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 1887230.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 1889640.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 1889640.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 1892940.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 1892940.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 1899870.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 1899880.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 1899900.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 1902820.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 1902840.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 1903850.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 1903860.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 1903870.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 1903880.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 1904250.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 1904260.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 1905250.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 1906150.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 1906160.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 1906160.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 1906560.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 1906560.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 1906570.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 1906580.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 1906610.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 1906620.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 1907520.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 1907540.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 1907880.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 1907880.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 1907890.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 1907890.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 1908330.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 1908330.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 1908460.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 1908470.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 1908470.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 1908470.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 1908880.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 1908880.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 1908890.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 1909520.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 1909530.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 1909540.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 1909550.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 1910180.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 1910200.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 1910530.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 1910550.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 1910890.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 1910900.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 1910900.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 1910900.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 1911490.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 1911710.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 1911720.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 1912220.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 1912240.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 1913640.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 1913640.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 1918380.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 1918380.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 1918450.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 1918450.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 1920340.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 1920340.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 1921260.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 1921260.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 1921310.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 1921310.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 1921400.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 1922600.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 1922600.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 1923430.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 1923430.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 1924120.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 1924120.0 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 = 1.26855 2S = 0.97899 2P = 0.84268 3S = 0.96958 3P = 0.83983 3D = 0.75956 4S = 0.96833 4P = 0.83995 4D = 0.76070 4F = 0.84971 5S = 0.96925 5P = 0.84156 5D = 0.76285 5F = 0.73398 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. 65 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 37.1306 Rydbergs (505.198944 eV) A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00054424 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.54424 eV) was used from the last threshold up to 6.969535 Z**2 Rydbergs (379.31 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.54424 eV) was used from first threshold up to 6.969535 Z**2 Rydbergs (379.31 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: 15/10/10 ------------------------------------------------------------------------ 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 = 1.26941 2S = 0.98145 2P = 0.84871 3S = 0.97191 3P = 0.84175 3D = 0.76433 4S = 0.97153 4P = 0.84272 4D = 0.76957 4F = 0.89579 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 38.2646 Rydbergs (520.628148 eV) A fine energy mesh of 0.000060 Z**2 Rydbergs (0.00326544 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.54424 eV) was used from the last threshold up to 6.969535 Z**2 Rydbergs (379.31 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.54424 eV) was used from first threshold up to 6.969535 Z**2 Rydbergs (379.31 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 0.4406742 3 0.4409849 4 1.6421223 5 1.7583025 6 1.7583938 7 1.7867112 8 1.7867378 9 2.1660677 10 2.2128267 11 2.2128642 12 2.2247841 13 2.2247953 14 2.2253077 15 2.2253133 16 2.3980886 17 2.4214349 18 2.4214542 19 2.4275374 20 2.4275432 21 2.4278208 22 2.4278237 23 2.4278604 24 2.4278604 25 14.1655 26 14.314638 29 14.6358 31 14.850050 34 14.8450 36 15.01039 38 15.08167 40 15.364 41 16.070608 42 16.193 43 16.226 45 16.219273 48 16.306368 52 16.406 53 16.358 55 16.491 57 16.45633 58 16.456234 59 16.456579 60 16.608 62 16.551380 64 16.544113 68 16.57856 69 16.568 71 16.614368 75 16.637841 77 16.661 79 16.6293 82 16.669373 83 16.669745 84 16.71166 85 16.601940 88 16.673687 92 16.696837 95 16.667 98 16.76693 101 16.792945 105 16.8135 109 16.778 111 16.7772 113 16.822700 119 16.8514 133 17.045583 138 17.07928 142 17.104 144 17.085007 145 17.099794 148 17.107908 154 17.104 156 17.129482 160 17.133974 162 17.134111 166 17.140446 169 17.148636 173 17.149284 177 17.148788 188 17.2769 192 17.302 Produced by: Guiyun Liang Date: 11/10/10 ------------------------------------------------------------------------