Li+ 0 3 1 43488.(1S) 1 2s(2S) (2)0( 0.5) 0. 2 2p(2P) (2)1( 2.5) 14850. 3 3s(2S) (2)0( 0.5) 26890. 4 3p(2P) (2)1( 2.5) 30626. 5 3d(2D) (2)2( 4.5) 30893. 6 4s(2S) (2)0( 0.5) 34643. 7 4p(2P) (2)1( 2.5) 36112. 8 4d(2D) (2)2( 4.5) 36228. 9 4f(2F) (2)3( 6.5) 36229. -1 1.00 3 1.00+03 2.00+03 5.00+03 1.00+04 2.00+04 5.00+04 1.00+05 2.00+05 2 1 3.75+07 2.25+00 3.73+00 7.29+00 1.18+01 1.90+01 3.58+01 5.58+01 8.13+01 4.53+01 3 1 0.00+00 1.09+00 1.33+00 1.42+00 1.32+00 1.25+00 1.36+00 1.70+00 2.21+00 4.63+00 4 1 7.08+05 1.04+00 1.17+00 1.24+00 1.20+00 1.15+00 1.15+00 1.22+00 1.32+00 9.74-02 5 1 0.00+00 4.99-01 6.90-01 9.76-01 1.27+00 1.69+00 2.55+00 3.48+00 4.50+00 7.38+00 6 1 0.00+00 3.06-01 3.44-01 3.34-01 3.05-01 2.83-01 2.96-01 3.57-01 4.57-01 9.20-01 7 1 1.02+06 2.99-01 3.37-01 3.47-01 3.46-01 3.38-01 3.29-01 3.37-01 3.58-01 8.56-02 8 1 0.00+00 2.56-01 3.05-01 3.55-01 4.11-01 5.04-01 7.04-01 9.22-01 1.17+00 2.06+00 9 1 0.00+00 2.22-01 2.56-01 2.79-01 2.92-01 3.05-01 3.32-01 3.59-01 3.72-01 2.15-01 3 2 3.28+07 3.56+00 4.49+00 5.44+00 6.13+00 7.58+00 1.28+01 2.08+01 3.22+01 2.47+01 4 2 0.00+00 8.05+00 8.97+00 9.71+00 1.02+01 1.11+01 1.38+01 1.70+01 2.06+01 3.34+01 5 2 6.74+07 3.62+00 5.45+00 8.83+00 1.27+01 1.97+01 4.03+01 7.09+01 1.16+02 1.07+02 6 2 1.01+07 2.06+00 2.09+00 1.80+00 1.53+00 1.35+00 1.47+00 1.94+00 2.70+00 1.71+00 7 2 0.00+00 2.24+00 2.64+00 2.75+00 2.75+00 2.81+00 3.12+00 3.66+00 4.40+00 6.53+00 8 2 2.25+07 2.17+00 2.46+00 2.81+00 3.29+00 4.27+00 7.25+00 1.16+01 1.79+01 1.51+01 9 2 0.00+00 1.89+00 2.26+00 2.62+00 2.98+00 3.53+00 4.82+00 6.20+00 7.44+00 7.87+00 4 3 3.82+06 1.17+01 1.34+01 2.32+01 5.03+01 1.12+02 2.72+02 4.59+02 6.80+02 2.89+02 5 3 0.00+00 6.81+00 1.26+01 2.42+01 3.40+01 4.32+01 5.47+01 6.44+01 7.42+01 9.73+01 6 3 0.00+00 3.43+00 4.09+00 4.04+00 3.64+00 3.69+00 5.70+00 8.84+00 1.28+01 2.72+01 7 3 1.49+02 1.99+00 2.43+00 3.00+00 3.71+00 4.95+00 7.18+00 8.81+00 1.01+01 7.50-04 8 3 0.00+00 2.66+00 3.22+00 3.63+00 4.04+00 5.02+00 7.73+00 1.04+01 1.23+01 1.10+01 9 3 0.00+00 3.69+00 5.01+00 6.78+00 8.34+00 1.06+01 1.52+01 1.89+01 2.14+01 2.08+01 5 4 1.59+03 3.04+02 5.59+02 1.06+03 1.54+03 2.08+03 2.82+03 3.41+03 3.98+03 5.47+02 6 4 7.34+06 6.43+00 8.37+00 1.22+01 1.94+01 3.59+01 8.70+01 1.57+02 2.50+02 1.49+02 7 4 0.00+00 1.07+01 1.40+01 1.75+01 2.30+01 3.50+01 6.12+01 8.38+01 1.05+02 1.57+02 8 4 6.85+06 1.05+01 1.39+01 1.88+01 2.50+01 3.99+01 9.80+01 1.91+02 3.24+02 2.56+02 9 4 0.00+00 1.20+01 1.67+01 2.56+01 3.59+01 5.52+01 1.06+02 1.59+02 2.11+02 2.97+02 6 5 0.00+00 1.13+01 1.42+01 1.64+01 1.75+01 1.90+01 2.21+01 2.53+01 2.78+01 2.67+01 7 5 4.92+05 1.29+01 1.59+01 1.81+01 1.95+01 2.17+01 2.58+01 3.02+01 3.61+01 1.37+01 8 5 0.00+00 1.80+01 2.34+01 3.09+01 4.02+01 5.79+01 9.57+01 1.28+02 1.56+02 2.17+02 9 5 1.38+07 2.73+01 3.73+01 5.71+01 9.07+01 1.68+02 4.33+02 8.20+02 1.34+03 8.37+02 7 6 7.95+05 1.34+01 2.36+01 7.56+01 2.07+02 4.93+02 1.20+03 1.99+03 2.87+03 9.91+02 8 6 0.00+00 1.41+01 2.84+01 6.74+01 1.09+02 1.56+02 2.29+02 2.83+02 3.25+02 3.88+02 9 6 0.00+00 2.02+01 2.88+01 3.74+01 4.09+01 4.42+01 5.18+01 5.93+01 6.56+01 7.05+01 8 7 5.57+02 8.52+02 1.70+03 3.89+03 6.24+03 8.88+03 1.25+04 1.53+04 1.80+04 2.32+03 9 7 0.00+00 3.19+02 4.14+02 4.93+02 5.07+02 4.97+02 4.81+02 4.77+02 4.74+02 4.29+02 9 8 1.04-02 1.43+04 1.74+04 2.16+04 2.47+04 2.76+04 3.11+04 3.36+04 3.59+04 2.02+03 -1 -1 -1 C------------------------------------------------------------------------------- C C C For more information see: D. C. Griffin, D. M. Mitnik, J. Colgan, C and M. S. Pindzola, Phys. Rev. A 64 032718 (2001) C C From a 55-state R-matrix with pseudo-state (RMPS) calculation C C The 1s and 2s orbitals were determined from a Hartree-Fock (HF) C calculation on 1s22s. The 2p, 3s, 3p, 3d, 4s, 4p, 4d, and 4f C orbitals were determined from a frozen-core HF calculation on C 1s2nl. In addition, we generated 1s2nl pseudo states for: C ns with n=6 to 15, np with n=6 to 14, nd with n=6 to 13, nf with C n=6 to 12, and ng with n=6 to 12 using Laguerre orbitals. These C were used to represent the target continuum as well as the highly C excited Rydberg states. C C C For the RMPS calculation with exchange, all partial LSPI partial C waves from L = 0 to L = 9 were included. This was then extended C to higher L values by adding to it the results of a no-exchange C RMPS calculation from L=10 to L=60 with top up. The size of the C continuum basis for these calculations was 36 and the size of the C R-matrix box was 77.3 au. C C The numbers in the last column of the above table are the theoretical C values for the reduced effective collision strengths in the infinite C temperature limit as defined in Burgess and Tully Astron. Astrophys. C 254 436 (1992) C C Donald C. Griffin November 21 2003 C-------------------------------------------------------------------------------