C + 3 6 4 520159.(1S) 1 1s22s(2S) (2)0( 0.5) 0. 2 1s22p(2P) (2)1( 2.5) 65034. 3 1s23s(2S) (2)0( 0.5) 302024. 4 1s23p(2P) (2)1( 2.5) 319365. 5 1s23d(2D) (2)2( 4.5) 323873. 6 1s24s(2S) (2)0( 0.5) 400346. 7 1s24p(2P) (2)1( 2.5) 407367. 8 1s24d(2D) (2)2( 4.5) 409265. 9 1s24f(2F) (2)3( 6.5) 409321. -1 4.00 3 1.60+04 3.20+04 8.00+04 1.60+05 3.20+05 8.00+05 1.60+06 3.20+06 2 1 2.75+08 8.60+00 8.83+00 9.44+00 1.02+01 1.14+01 1.37+01 1.59+01 1.86+01 3 1 0.00+00 5.66-01 4.94-01 4.07-01 3.68-01 3.54-01 3.60-01 3.77-01 3.96-01 4 1 4.52+09 3.32-01 2.95-01 2.57-01 2.39-01 2.44-01 3.13-01 4.31-01 6.15-01 5 1 0.00+00 4.59-01 4.64-01 4.76-01 4.92-01 5.38-01 6.63-01 7.93-01 9.17-01 6 1 0.00+00 1.02-01 8.52-02 6.99-02 6.42-02 6.28-02 6.53-02 6.92-02 7.34-02 7 1 2.22+09 9.73-02 9.15-02 8.06-02 7.45-02 7.40-02 8.77-02 1.14-01 1.55-01 8 1 0.00+00 9.00-02 9.32-02 9.13-02 9.16-02 9.76-02 1.17-01 1.40-01 1.63-01 9 1 0.00+00 7.36-02 7.35-02 6.64-02 6.13-02 5.90-02 5.95-02 6.09-02 6.19-02 3 2 4.21+09 1.86+00 1.39+00 8.57-01 6.03-01 4.67-01 4.36-01 5.08-01 6.47-01 4 2 0.00+00 2.67+00 2.26+00 1.87+00 1.66+00 1.53+00 1.51+00 1.58+00 1.67+00 5 2 1.75+10 4.13+00 4.23+00 4.41+00 4.70+00 5.40+00 7.27+00 9.58+00 1.27+01 6 2 1.56+09 3.21-01 2.35-01 1.58-01 1.20-01 9.68-02 8.36-02 8.67-02 9.98-02 7 2 0.00+00 6.02-01 5.29-01 4.34-01 3.76-01 3.35-01 3.12-01 3.15-01 3.26-01 8 2 5.86+09 7.16-01 7.52-01 7.71-01 8.16-01 9.25-01 1.22+00 1.58+00 2.04+00 9 2 0.00+00 4.64-01 4.64-01 4.14-01 3.74-01 3.52-01 3.54-01 3.74-01 3.99-01 4 3 3.24+07 4.91+01 5.11+01 5.84+01 6.78+01 8.05+01 1.01+02 1.19+02 1.38+02 5 3 0.00+00 7.78+00 7.81+00 7.56+00 7.16+00 6.86+00 6.71+00 6.71+00 6.71+00 6 3 0.00+00 2.18+00 1.84+00 1.60+00 1.57+00 1.63+00 1.79+00 1.93+00 2.05+00 7 3 4.96+08 8.23-01 7.53-01 6.85-01 7.06-01 8.47-01 1.29+00 1.85+00 2.59+00 8 3 0.00+00 1.23+00 1.29+00 1.38+00 1.53+00 1.77+00 2.14+00 2.41+00 2.62+00 9 3 0.00+00 1.75+00 1.82+00 1.87+00 1.95+00 2.06+00 2.19+00 2.25+00 2.28+00 5 4 4.76+05 1.22+02 1.28+02 1.41+02 1.58+02 1.84+02 2.23+02 2.53+02 2.83+02 6 4 1.07+09 4.41+00 3.03+00 2.01+00 1.78+00 1.98+00 2.84+00 3.88+00 5.21+00 7 4 0.00+00 5.20+00 4.92+00 4.81+00 5.02+00 5.53+00 6.53+00 7.37+00 8.12+00 8 4 1.75+09 6.72+00 7.05+00 7.78+00 9.22+00 1.20+01 1.81+01 2.48+01 3.30+01 9 4 0.00+00 6.85+00 7.42+00 8.28+00 9.44+00 1.11+01 1.37+01 1.56+01 1.71+01 6 5 0.00+00 8.06+00 5.03+00 2.60+00 1.63+00 1.12+00 8.18-01 7.32-01 6.97-01 7 5 1.27+08 6.97+00 5.46+00 3.93+00 3.11+00 2.58+00 2.32+00 2.40+00 2.65+00 8 5 0.00+00 1.01+01 1.02+01 9.61+00 9.36+00 9.55+00 1.04+01 1.12+01 1.20+01 9 5 3.53+09 3.31+01 3.55+01 4.04+01 4.81+01 6.08+01 8.56+01 1.11+02 1.40+02 7 6 7.29+06 1.36+02 1.53+02 1.89+02 2.33+02 2.91+02 3.79+02 4.49+02 5.18+02 8 6 0.00+00 3.23+01 3.19+01 3.07+01 3.00+01 2.98+01 2.96+01 2.93+01 2.89+01 9 6 0.00+00 7.51+00 7.06+00 5.91+00 5.10+00 4.56+00 4.18+00 4.05+00 3.97+00 8 7 1.51+05 3.09+02 3.59+02 4.77+02 6.16+02 7.80+02 9.93+02 1.14+03 1.28+03 9 7 0.00+00 4.59+01 4.41+01 4.01+01 3.73+01 3.52+01 3.30+01 3.17+01 3.07+01 9 8 2.32+00 6.98+02 8.72+02 1.13+03 1.34+03 1.53+03 1.76+03 1.90+03 2.02+03 -1 -1 -1 C------------------------------------------------------------------------------- C C See: Griffin D C, Badnell N R, and Pindzola M S 2000 J. Phys. B C 33, 1013 for a more complete description. C C From a 41-state RMPS calculation that included the 9 spectroscopic C terms of the configurations 1s22s, 1s22p, 1s23s, 1s23p, 1s23d, 1s24s, C 1s24p, 1s24d, 1s24f; and the 32 pseudo states 1s2nl for n = 5 to 12 C and l = 0 to 3 in the close-coupling expansion. C C The 1s and 2s orbitals were generated from a single-configuration C Hartree-Fock (SCHF) calculation on 1s22s, while the 2p through 4f C orbitals were generated from a SCHF calculation on the terms C 1s2nl with the 1s orbital frozen. The pseudo states were generated C from an non-orthogonal Laguerre basis; these states were then C orthogonalized with respect to the Hartree-Fock orbitals and each C other. C C For the L = 0 to 12 even and odd parity LSPI partial waves, we C performed an R-Matrix calculation with exchange. For the higher C partial waves we performed a no-exchange R-Matrix calculation for C L = 13 to 60 with the long-range perturbations turned on and with C topup. However, because of numerical problems for high partial waves C that affected only the 2-4, 2-7, and 2-9 transitions, the NX run for C these three transitions was from L = 13 to L = 30, again with long- C range perturbations turned on and with topup. The continuum basis for C these calculations was set to 40 and the radius of the R-matrix box C was 20.76 a.u. C C Donald C. Griffin May 18, 2000 C-------------------------------------------------------------------------------