Resolved Specific Ion Data Collections

Temperature Range
0.086 eV → 8.617 eV


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  • Spontaneous Emission: Li+0(i) → Li+0(j) + hv
  • Electron Impact Excitation: Li+0(i) + e → Li+0(j) + e
2s(2s) 2S0.5 0.0 cm-1
2p(2p) 2P2.5 14850.0 cm-1
3s(2s) 2S0.5 26890.0 cm-1
3p(2p) 2P2.5 30626.0 cm-1
3d(2d) 2D4.5 30893.0 cm-1
4s(2s) 2S0.5 34643.0 cm-1
4p(2p) 2P2.5 36112.0 cm-1
4d(2d) 2D4.5 36228.0 cm-1
4f(2f) 2F6.5 36229.0 cm-1

        For more information see: D. C. Griffin, D. M. Mitnik, J. Colgan,    
        and M. S. Pindzola, Phys. Rev. A 64 032718 (2001)                    
        From a 55-state R-matrix with pseudo-state (RMPS) calculation        
        The 1s and 2s orbitals were determined from a Hartree-Fock (HF)      
        calculation on 1s22s.  The 2p, 3s, 3p, 3d, 4s, 4p, 4d, and 4f        
        orbitals were determined from a frozen-core HF calculation on        
        1s2nl.  In addition, we generated 1s2nl pseudo states for:           
        ns with n=6 to 15, np with n=6 to 14, nd with n=6 to 13, nf with     
        n=6 to 12, and ng with n=6 to 12 using Laguerre orbitals.  These     
        were used to represent the target continuum as well as the highly    
        excited Rydberg states.                                              
        For the RMPS calculation with exchange, all partial LSPI partial     
        waves from L = 0 to L = 9 were included.  This was then extended     
        to higher L values by adding to it the results of a no-exchange      
        9-state R-matrix calculation from L=10 to L=60 with top up.  The
        size of the continuum basis for these calculations was 36 and the
        size of the R-matrix box was 77.3 au.                                            

        Donald C. Griffin                 December, 2 2001           

                 Changed format of first line from "Li  0" to "Li+ 0"
                 Allan Whiteford, August 17 2006



  • Don Griffin
  • James Colgan
  • Allan Whiteford
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