jj#b1.dat
        Resolved Specific Ion Data Collections
        
        
                - Ion
 - B1+
 
                                                - Temperature Range
 - 0.345 eV  → 68.93 eV
                                                                         
        ADF04
        
                - Filename
 - jj#b1.dat
 
                - Full Path
 - adf04/copmm#5/jj#b1.dat
 
        
        Download data
 
        
                        
                
                - Spontaneous Emission: B+1(i) → B+1(j) + hv
 - Electron Impact Excitation: B+1(i) + e → B+1(j) + e
                 
                 
                | 1s2-2s2 1S0.0 |             0.0 cm-1 | 
| 1s2 2s1 2p1 3P0.0 |         37184.1 cm-1 | 
| 1s2 2s1 2p1 3P1.0 |         37191.8 cm-1 | 
| 1s2 2s1 2p1 3P2.0 |         37207.1 cm-1 | 
| 1s2 2s1 2p1 1P1.0 |         70425.8 cm-1 | 
| 1s2 2p2 3P0.0 |         98568.9 cm-1 | 
| 1s2 2p2 3P1.0 |         98576.6 cm-1 | 
| 1s2 2p2 3P2.0 |         98592.0 cm-1 | 
| 1s2 2p2 1D2.0 |        104869.0 cm-1 | 
| 1s2 2p2 1S0.0 |        126638.0 cm-1 | 
| 1s2 2s1 3s1 3S1.0 |        129920.0 cm-1 | 
| 1s2 2s1 3s1 1S0.0 |        136511.0 cm-1 | 
| 1s2 2s1 3p1 3P0.0 |        144341.0 cm-1 | 
| 1s2 2s1 3p1 3P1.0 |        144343.0 cm-1 | 
| 1s2 2s1 3p1 3P2.0 |        144346.0 cm-1 | 
| 1s2 2s1 3p1 1P1.0 |        144810.0 cm-1 | 
| 1s2 2s1 3d1 3D1.0 |        150887.0 cm-1 | 
| 1s2 2s1 3d1 3D2.0 |        150887.0 cm-1 | 
| 1s2 2s1 3d1 3D3.0 |        150888.0 cm-1 | 
| 1s2 2s1 3d1 1D2.0 |        155135.0 cm-1 | 
| 1s2 2s1 4s1 3S1.0 |        167679.0 cm-1 | 
| 1s2 2s1 4s1 1S0.0 |        169246.0 cm-1 | 
| 1s2 2s1 4p1 1P1.0 |        171802.0 cm-1 | 
| 1s2 2s1 4p1 3P0.0 |        172672.0 cm-1 | 
| 1s2 2s1 4p1 3P1.0 |        172672.0 cm-1 | 
| 1s2 2s1 4p1 3P2.0 |        172673.0 cm-1 | 
| 1s2 2s1 4d1 3D1.0 |        175203.0 cm-1 | 
| 1s2 2s1 4d1 3D2.0 |        175203.0 cm-1 | 
| 1s2 2s1 4d1 3D3.0 |        175203.0 cm-1 | 
| 1s2 2s1 4f1 3F2.0 |        176018.0 cm-1 | 
| 1s2 2s1 4f1 3F3.0 |        176018.0 cm-1 | 
| 1s2 2s1 4f1 3F4.0 |        176018.0 cm-1 | 
| 1s2 2s1 4f1 1F3.0 |        176025.0 cm-1 | 
| 1s2 2s1 4d1 1D2.0 |        176842.0 cm-1 | 
| 1s2 2p1 3s1 3P0.0 |        181403.0 cm-1 | 
| 1s2 2p1 3s1 3P1.0 |        181413.0 cm-1 | 
| 1s2 2p1 3s1 3P2.0 |        181433.0 cm-1 | 
| 1s2 2p1 3p1 1P1.0 |        188846.0 cm-1 | 
| 1s2 2p1 3s1 1P1.0 |        189095.0 cm-1 | 
| 1s2 2p1 3p1 3D1.0 |        190345.0 cm-1 | 
| 1s2 2p1 3p1 3D2.0 |        190356.0 cm-1 | 
| 1s2 2p1 3p1 3D3.0 |        190374.0 cm-1 | 
| 1s2 2p1 3p1 3S1.0 |        192431.0 cm-1 | 
| 1s2 2p1 3p1 3P0.0 |        196908.0 cm-1 | 
| 1s2 2p1 3p1 3P1.0 |        196914.0 cm-1 | 
| 1s2 2p1 3p1 3P2.0 |        196925.0 cm-1 | 
| 1s2 2p1 3d1 1D2.0 |        197740.0 cm-1 | 
| 1s2 2p1 3d1 3F2.0 |        198583.0 cm-1 | 
| 1s2 2p1 3d1 3F3.0 |        198593.0 cm-1 | 
| 1s2 2p1 3d1 3F4.0 |        198607.0 cm-1 | 
| 1s2 2p1 3d1 3D1.0 |        199739.0 cm-1 | 
| 1s2 2p1 3d1 3D2.0 |        199742.0 cm-1 | 
| 1s2 2p1 3d1 3D3.0 |        199748.0 cm-1 | 
| 1s2 2p1 3p1 1D2.0 |        200053.0 cm-1 | 
| 1s2 2p1 3d1 3P2.0 |        201693.0 cm-1 | 
| 1s2 2p1 3d1 3P1.0 |        201702.0 cm-1 | 
| 1s2 2p1 3d1 3P0.0 |        201707.0 cm-1 | 
| 1s2 2p1 3d1 1F3.0 |        204043.0 cm-1 | 
| 1s2 2p1 3d1 1P1.0 |        205251.0 cm-1 | 
| 1s2 2p1 3p1 1S0.0 |        208319.0 cm-1 | 
         
        
        
        
        
 
 
 
        
 
------------------------------------------------------------------------------ 1 1S2-2S2 1 1S 1S/ 2 1S2 2S1 2P1 1 2S 2S/ 1 2P 3P/ 3 1S2 2S1 2P1 1 2S 2S/ 1 2P 3P/ 4 1S2 2S1 2P1 1 2S 2S/ 1 2P 3P/ 5 1S2 2S1 2P1 1 2S 2S/ 1 2P 1P/ 6 1S2 2P2 1 3P 3P/ 7 1S2 2P2 1 3P 3P/ 8 1S2 2P2 1 3P 3P/ 9 1S2 2P2 2 1D 1D/ 10 1S2 2P2 3 1S 1S/ 11 1S2 2S1 3S1 1 2S 2S/ 1 2S 3S/ 12 1S2 2S1 3S1 1 2S 2S/ 1 2S 1S/ 13 1S2 2S1 3P1 1 2S 2S/ 1 2P 3P/ 14 1S2 2S1 3P1 1 2S 2S/ 1 2P 3P/ 15 1S2 2S1 3P1 1 2S 2S/ 1 2P 3P/ 16 1S2 2S1 3P1 1 2S 2S/ 1 2P 1P/ 17 1S2 2S1 3D1 1 2S 2S/ 1 2D 3D/ 18 1S2 2S1 3D1 1 2S 2S/ 1 2D 3D/ 19 1S2 2S1 3D1 1 2S 2S/ 1 2D 3D/ 20 1S2 2S1 3D1 1 2S 2S/ 1 2D 1D/ 21 1S2 2S1 4S1 1 2S 2S/ 1 2S 3S/ 22 1S2 2S1 4S1 1 2S 2S/ 1 2S 1S/ 23 1S2 2S1 4P1 1 2S 2S/ 1 2P 1P/ 24 1S2 2S1 4P1 1 2S 2S/ 1 2P 3P/ 25 1S2 2S1 4P1 1 2S 2S/ 1 2P 3P/ 26 1S2 2S1 4P1 1 2S 2S/ 1 2P 3P/ 27 1S2 2S1 4D1 1 2S 2S/ 1 2D 3D/ 28 1S2 2S1 4D1 1 2S 2S/ 1 2D 3D/ 29 1S2 2S1 4D1 1 2S 2S/ 1 2D 3D/ 30 1S2 2S1 4F1 1 2S 2S/ 1 2F 3F/ 31 1S2 2S1 4F1 1 2S 2S/ 1 2F 3F/ 32 1S2 2S1 4F1 1 2S 2S/ 1 2F 3F/ 33 1S2 2S1 4F1 1 2S 2S/ 1 2F 1F/ 34 1S2 2S1 4D1 1 2S 2S/ 1 2D 1D/ 35 1S2 2P1 3S1 1 2P 2P/ 1 2S 3P/ 36 1S2 2P1 3S1 1 2P 2P/ 1 2S 3P/ 37 1S2 2P1 3S1 1 2P 2P/ 1 2S 3P/ 38 1S2 2P1 3P1 1 2P 2P/ 1 2P 1P/ 39 1S2 2P1 3S1 1 2P 2P/ 1 2S 1P/ 40 1S2 2P1 3P1 1 2P 2P/ 1 2P 3D/ 41 1S2 2P1 3P1 1 2P 2P/ 1 2P 3D/ 42 1S2 2P1 3P1 1 2P 2P/ 1 2P 3D/ 43 1S2 2P1 3P1 1 2P 2P/ 1 2P 3S/ 44 1S2 2P1 3P1 1 2P 2P/ 1 2P 3P/ 45 1S2 2P1 3P1 1 2P 2P/ 1 2P 3P/ 46 1S2 2P1 3P1 1 2P 2P/ 1 2P 3P/ 47 1S2 2P1 3D1 1 2P 2P/ 1 2D 1D/ 48 1S2 2P1 3D1 1 2P 2P/ 1 2D 3F/ 49 1S2 2P1 3D1 1 2P 2P/ 1 2D 3F/ 50 1S2 2P1 3D1 1 2P 2P/ 1 2D 3F/ 51 1S2 2P1 3D1 1 2P 2P/ 1 2D 3D/ 52 1S2 2P1 3D1 1 2P 2P/ 1 2D 3D/ 53 1S2 2P1 3D1 1 2P 2P/ 1 2D 3D/ 54 1S2 2P1 3P1 1 2P 2P/ 1 2P 1D/ 55 1S2 2P1 3D1 1 2P 2P/ 1 2D 3P/ 56 1S2 2P1 3D1 1 2P 2P/ 1 2D 3P/ 57 1S2 2P1 3D1 1 2P 2P/ 1 2D 3P/ 58 1S2 2P1 3D1 1 2P 2P/ 1 2D 1F/ 59 1S2 2P1 3D1 1 2P 2P/ 1 2D 1P/ 60 1S2 2P1 3P1 1 2P 2P/ 1 2P 1S/ ------------------------------------------------------------------------------ Generated from Cowan Atomic Structure Program M O'Mullane 11:07 22/10/1992 SCF method used : HR Scale factors for Slater Parameters : 75 99 75 75 80 Optically allowed transitions : yes Optically forbidden transitions M1 : parity 1 Optically forbidden transitions E2 : parity 1 Born Collision-Strength - print : 9 - forbidden : 0 -> 2 - allowed : 1 -> 1 - included : 7,all Parity 1 Parity 2 Allowed 281 0 575 initially 281 0 575 reduced ------------------------------------------------------------------------------ Minor re-organisation to produce a conformant adf04 dataset. Numerical data has not changed. Martin O'Mullane 04-08-2009 ----------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------