lilike_lgy10#be1.dat
Resolved Specific Ion Data Collections
- Ion
- Be1+
- Temperature Range
- 0.069 eV → 689 eV
ADF04
- Filename
- lilike_lgy10#be1.dat
- Full Path
- adf04/copaw#li/lilike_lgy10#be1.dat
Download data
- Spontaneous Emission: Be+1(i) → Be+1(j) + hv
- Electron Impact Excitation: Be+1(i) + e → Be+1(j) + e
| 2s1 2S0.5 | 0.0 cm-1 |
| 2p1 2P0.5 | 32174.0 cm-1 |
| 2p1 2P1.5 | 32179.0 cm-1 |
| 3s1 2S0.5 | 87731.0 cm-1 |
| 3p1 2P0.5 | 96084.0 cm-1 |
| 3p1 2P1.5 | 96085.0 cm-1 |
| 3d1 2D1.5 | 97442.0 cm-1 |
| 3d1 2D2.5 | 97443.0 cm-1 |
| 4s1 2S0.5 | 114871.0 cm-1 |
| 4p1 2P0.5 | 118206.0 cm-1 |
| 4p1 2P1.5 | 118207.0 cm-1 |
| 4d1 2D1.5 | 118787.0 cm-1 |
| 4d1 2D2.5 | 118787.0 cm-1 |
| 4f1 2F2.5 | 118797.0 cm-1 |
| 4f1 2F3.5 | 118797.0 cm-1 |
| 5s1 2S0.5 | 126712.0 cm-1 |
| 5p1 2P0.5 | 128369.0 cm-1 |
| 5p1 2P1.5 | 128369.0 cm-1 |
| 5d1 2D1.5 | 128668.0 cm-1 |
| 5d1 2D2.5 | 128668.0 cm-1 |
| 5f1 2F2.5 | 128673.0 cm-1 |
| 5f1 2F3.5 | 128673.0 cm-1 |
| 5g1 2G3.5 | 128673.0 cm-1 |
| 5g1 2G4.5 | 128673.0 cm-1 |
| 1s1 2s2 2S0.5 | 935812.0 cm-1 |
| 1s1 2s1 2p1 4P0.5 | 952984.0 cm-1 |
| 1s1 2s1 2p1 4P1.5 | 952986.0 cm-1 |
| 1s1 2s1 2p1 4P2.5 | 952990.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 971229.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 971233.0 cm-1 |
| 1s1 2s1 2p1 2P0.5 | 996947.0 cm-1 |
| 1s1 2s1 2p1 2P1.5 | 996949.0 cm-1 |
| 1s1 2p2 4P0.5 | 998148.0 cm-1 |
| 1s1 2p2 4P1.5 | 998150.0 cm-1 |
| 1s1 2p2 4P2.5 | 998154.0 cm-1 |
| 1s1 2p2 2P0.5 | 1009480.0 cm-1 |
| 1s1 2p2 2P1.5 | 1009480.0 cm-1 |
| 1s1 2p2 2D1.5 | 1009770.0 cm-1 |
| 1s1 2p2 2D2.5 | 1009780.0 cm-1 |
| 1s1 2p2 2S0.5 | 1040700.0 cm-1 |
| 1s1 2s1 3s1 4S1.5 | 1051500.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 1061490.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 1064730.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 1064740.0 cm-1 |
| 1s1 2s1 3p1 4P0.5 | 1066430.0 cm-1 |
| 1s1 2s1 3p1 4P1.5 | 1066430.0 cm-1 |
| 1s1 2s1 3p1 4P2.5 | 1066430.0 cm-1 |
| 1s1 2s1 3d1 4D0.5 | 1070500.0 cm-1 |
| 1s1 2s1 3d1 4D1.5 | 1070500.0 cm-1 |
| 1s1 2s1 3d1 4D2.5 | 1070500.0 cm-1 |
| 1s1 2s1 3d1 4D3.5 | 1070500.0 cm-1 |
| 1s1 2s1 3s1 2S0.5 | 1072330.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 1074910.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 1074910.0 cm-1 |
| 1s1 2s1 3p1 2P0.5 | 1081220.0 cm-1 |
| 1s1 2s1 3p1 2P1.5 | 1081220.0 cm-1 |
| 1s1 2s1 3d1 2D1.5 | 1087610.0 cm-1 |
| 1s1 2s1 3d1 2D2.5 | 1087610.0 cm-1 |
| 1s1 2s1 4s1 4S1.5 | 1089870.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 1091590.0 cm-1 |
| 1s1 2s1 4p1 4P0.5 | 1093100.0 cm-1 |
| 1s1 2s1 4p1 4P1.5 | 1093100.0 cm-1 |
| 1s1 2s1 4p1 4P2.5 | 1093100.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 1093240.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 1093240.0 cm-1 |
| 1s1 2p1 3s1 4P0.5 | 1095010.0 cm-1 |
| 1s1 2p1 3s1 4P1.5 | 1095010.0 cm-1 |
| 1s1 2p1 3s1 4P2.5 | 1095020.0 cm-1 |
| 1s1 2s1 4f1 4F1.5 | 1095250.0 cm-1 |
| 1s1 2s1 4f1 4F2.5 | 1095250.0 cm-1 |
| 1s1 2s1 4f1 4F3.5 | 1095250.0 cm-1 |
| 1s1 2s1 4f1 4F4.5 | 1095250.0 cm-1 |
| 1s1 2s1 4d1 4D0.5 | 1095430.0 cm-1 |
| 1s1 2s1 4d1 4D1.5 | 1095430.0 cm-1 |
| 1s1 2s1 4d1 4D2.5 | 1095430.0 cm-1 |
| 1s1 2s1 4d1 4D3.5 | 1095430.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 1095610.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 1095610.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 1095980.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 1095980.0 cm-1 |
| 1s1 2p1 3p1 4D0.5 | 1096550.0 cm-1 |
| 1s1 2p1 3p1 4D1.5 | 1096550.0 cm-1 |
| 1s1 2p1 3p1 4D2.5 | 1096550.0 cm-1 |
| 1s1 2p1 3p1 4D3.5 | 1096560.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 1097130.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 1097130.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 1100170.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 1100170.0 cm-1 |
| 1s1 2p1 3p1 4S1.5 | 1100390.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 1102920.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 1102930.0 cm-1 |
| 1s1 2p1 3s1 2P1.5 | 1104160.0 cm-1 |
| 1s1 2p1 3s1 2P0.5 | 1104170.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 1104330.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 1104330.0 cm-1 |
| 1s1 2p1 3d1 4F1.5 | 1104940.0 cm-1 |
| 1s1 2p1 3d1 4F2.5 | 1104940.0 cm-1 |
| 1s1 2p1 3d1 4F3.5 | 1104940.0 cm-1 |
| 1s1 2p1 3d1 4F4.5 | 1104940.0 cm-1 |
| 1s1 2s1 4s1 2S0.5 | 1105620.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 1106960.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 1106960.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 1107560.0 cm-1 |
| 1s1 2p1 3d1 4D0.5 | 1108600.0 cm-1 |
| 1s1 2p1 3d1 4D1.5 | 1108600.0 cm-1 |
| 1s1 2p1 3d1 4D2.5 | 1108600.0 cm-1 |
| 1s1 2p1 3d1 4D3.5 | 1108600.0 cm-1 |
| 1s1 2p1 3p1 4P0.5 | 1109010.0 cm-1 |
| 1s1 2p1 3p1 4P1.5 | 1109010.0 cm-1 |
| 1s1 2p1 3p1 4P2.5 | 1109010.0 cm-1 |
| 1s1 2s1 4p1 2P0.5 | 1109820.0 cm-1 |
| 1s1 2s1 4p1 2P1.5 | 1109820.0 cm-1 |
| 1s1 2p1 3d1 4P2.5 | 1110560.0 cm-1 |
| 1s1 2p1 3d1 4P1.5 | 1110560.0 cm-1 |
| 1s1 2p1 3d1 4P0.5 | 1110560.0 cm-1 |
| 1s1 2s1 4d1 2D1.5 | 1111640.0 cm-1 |
| 1s1 2s1 4d1 2D2.5 | 1111640.0 cm-1 |
| 1s1 2s1 4f1 2F2.5 | 1112480.0 cm-1 |
| 1s1 2s1 4f1 2F3.5 | 1112480.0 cm-1 |
| 1s1 2p1 3p1 2P0.5 | 1114020.0 cm-1 |
| 1s1 2p1 3p1 2P1.5 | 1114030.0 cm-1 |
| 1s1 2p1 3d1 2D1.5 | 1114170.0 cm-1 |
| 1s1 2p1 3d1 2D2.5 | 1114180.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 1114570.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 1114570.0 cm-1 |
| 1s1 2p1 3p1 2D2.5 | 1114640.0 cm-1 |
| 1s1 2p1 3p1 2D1.5 | 1114640.0 cm-1 |
| 1s1 2p1 3d1 2F3.5 | 1120170.0 cm-1 |
| 1s1 2p1 3d1 2F2.5 | 1120180.0 cm-1 |
| 1s1 2p1 3p1 2S0.5 | 1120790.0 cm-1 |
| 1s1 2p1 3d1 2P0.5 | 1121970.0 cm-1 |
| 1s1 2p1 3d1 2P1.5 | 1121970.0 cm-1 |
| 1s1 2p1 4s1 4P0.5 | 1126700.0 cm-1 |
| 1s1 2p1 4s1 4P1.5 | 1126700.0 cm-1 |
| 1s1 2p1 4s1 4P2.5 | 1126700.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 1128380.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 1128390.0 cm-1 |
| 1s1 2p1 4p1 4D0.5 | 1129420.0 cm-1 |
| 1s1 2p1 4p1 4D1.5 | 1129420.0 cm-1 |
| 1s1 2p1 4p1 4D2.5 | 1129420.0 cm-1 |
| 1s1 2p1 4p1 4D3.5 | 1129420.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 1129570.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 1129570.0 cm-1 |
| 1s1 2p1 4p1 4S1.5 | 1130220.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 1130810.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 1130810.0 cm-1 |
| 1s1 2p1 4d1 4F1.5 | 1130850.0 cm-1 |
| 1s1 2p1 4d1 4F2.5 | 1130850.0 cm-1 |
| 1s1 2p1 4d1 4F3.5 | 1130850.0 cm-1 |
| 1s1 2p1 4d1 4F4.5 | 1130850.0 cm-1 |
| 1s1 2p1 4p1 4P0.5 | 1130940.0 cm-1 |
| 1s1 2p1 4p1 4P1.5 | 1130940.0 cm-1 |
| 1s1 2p1 4p1 4P2.5 | 1130950.0 cm-1 |
| 1s1 2p1 4d1 4D0.5 | 1131550.0 cm-1 |
| 1s1 2p1 4d1 4D1.5 | 1131550.0 cm-1 |
| 1s1 2p1 4d1 4D2.5 | 1131550.0 cm-1 |
| 1s1 2p1 4d1 4D3.5 | 1131550.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 1131580.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 1131590.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 1131810.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 1131810.0 cm-1 |
| 1s1 2p1 4f1 4F1.5 | 1131900.0 cm-1 |
| 1s1 2p1 4f1 4F2.5 | 1131900.0 cm-1 |
| 1s1 2p1 4f1 4F3.5 | 1131900.0 cm-1 |
| 1s1 2p1 4f1 4F4.5 | 1131900.0 cm-1 |
| 1s1 2p1 4d1 4P2.5 | 1132190.0 cm-1 |
| 1s1 2p1 4d1 4P1.5 | 1132200.0 cm-1 |
| 1s1 2p1 4d1 4P0.5 | 1132200.0 cm-1 |
| 1s1 2p1 4f1 4G2.5 | 1132610.0 cm-1 |
| 1s1 2p1 4f1 4G3.5 | 1132610.0 cm-1 |
| 1s1 2p1 4f1 4G4.5 | 1132610.0 cm-1 |
| 1s1 2p1 4f1 4G5.5 | 1132620.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 1133040.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 1133040.0 cm-1 |
| 1s1 2p1 4s1 2P0.5 | 1133350.0 cm-1 |
| 1s1 2p1 4s1 2P1.5 | 1133350.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 1133360.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 1133360.0 cm-1 |
| 1s1 2p1 4f1 4D3.5 | 1133540.0 cm-1 |
| 1s1 2p1 4f1 4D2.5 | 1133540.0 cm-1 |
| 1s1 2p1 4f1 4D1.5 | 1133540.0 cm-1 |
| 1s1 2p1 4f1 4D0.5 | 1133540.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 1134100.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 1134110.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 1134150.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 1134960.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 1134960.0 cm-1 |
| 1s1 2p1 4p1 2P0.5 | 1136860.0 cm-1 |
| 1s1 2p1 4p1 2P1.5 | 1136860.0 cm-1 |
| 1s1 2p1 4p1 2D2.5 | 1136900.0 cm-1 |
| 1s1 2p1 4p1 2D1.5 | 1136900.0 cm-1 |
| 1s1 2p1 4d1 2D1.5 | 1137650.0 cm-1 |
| 1s1 2p1 4d1 2D2.5 | 1137650.0 cm-1 |
| 1s1 2p1 4f1 2F2.5 | 1138190.0 cm-1 |
| 1s1 2p1 4f1 2F3.5 | 1138190.0 cm-1 |
| 1s1 2p1 4d1 2F3.5 | 1138530.0 cm-1 |
| 1s1 2p1 4d1 2F2.5 | 1138530.0 cm-1 |
| 1s1 2p1 4f1 2G4.5 | 1139090.0 cm-1 |
| 1s1 2p1 4f1 2G3.5 | 1139090.0 cm-1 |
| 1s1 2p1 4p1 2S0.5 | 1139390.0 cm-1 |
| 1s1 2p1 4d1 2P0.5 | 1140120.0 cm-1 |
| 1s1 2p1 4d1 2P1.5 | 1140120.0 cm-1 |
| 1s1 2p1 4f1 2D1.5 | 1140180.0 cm-1 |
| 1s1 2p1 4f1 2D2.5 | 1140180.0 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 = 1.26220 2S = 0.95294 2P = 0.79908 3S = 0.94457 3P = 0.79766 3D = 0.71121 4S = 0.94335 4P = 0.79778 4D = 0.71267 4F = 0.89615 5S = 0.94398 5P = 0.79888 5D = 0.71498 5F = 0.69709 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. 70 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 19.3283 Rydbergs (262.980850 eV) A fine energy mesh of 0.000050 Z**2 Rydbergs (0.0006803 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.13606 eV) was used from the last threshold up to 13.384536 Z**2 Rydbergs (182.11 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.13606 eV) was used from first threshold up to 13.384536 Z**2 Rydbergs (182.11 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 = 1.26184 2S = 0.95482 2P = 0.80563 3S = 0.94614 3P = 0.79939 3D = 0.71712 4S = 0.94575 4P = 0.80031 4D = 0.72253 4F = 0.89290 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. 47 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 17.8404 Rydbergs (242.736482 eV) A fine energy mesh of 0.000500 Z**2 Rydbergs (0.006803 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.13606 eV) was used from the last threshold up to 13.384536 Z**2 Rydbergs (182.11 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.13606 eV) was used from first threshold up to 13.384536 Z**2 Rydbergs (182.11 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 0.29095612 3 0.29101605 4 0.80402837 5 0.87933042 6 0.87934799 7 0.8935390 8 0.8935438 9 1.0521894 10 1.0822254 11 1.0822328 12 1.0882460 13 1.0882482 14 1.0884774 15 1.0884786 16 1.1603630 17 1.1752759 18 1.1752798 19 1.1783606 20 1.1783617 21 1.1784856 22 1.1784863 23 1.1785003 24 1.1785003 25 8.40188 26 8.516638 29 8.72782 31 8.89214 33 8.908528 36 9.04988 38 8.99758 40 9.246627 41 9.4102320 42 9.468065 44 9.519096 45 9.510621 48 9.5674684 52 9.644850 53 9.601110 55 9.701349 57 9.782452 59 9.724878 61 9.753291 62 9.765684 66 9.6967225 69 9.7778863 73 9.791765 80 9.758759 81 9.753619 87 9.781541 89 9.788703 90 9.806145 94 9.817262 96 9.8269763 103 9.848974 104 9.8369911 108 9.7925450 116 9.820725 120 9.922787 122 9.955228 126 9.905473 128 9.956504 133 9.990139 138 10.01138 142 10.01391 144 10.02376 145 10.03597 151 10.02501 154 10.04312 160 10.04527 162 10.045407 179 10.05251 Produced by: Guiyun Liang Date: 05/11/10 ------------------------------------------------------------------------