Be+ 3 4 4 1756019.(2s) 1 1s(2S) (2)0( 0.5) 0. 2 2s(2S) (2)0( 0.5) 1316847. 3 2p(2P) (2)1( 2.5) 1316848. 4 3s(2S) (2)0( 0.5) 1560708. 5 3p(2P) (2)1( 2.5) 1560709. 6 3d(2D) (2)2( 4.5) 1560711. 7 4s(2S) (2)0( 0.5) 1646060. 8 4p(2P) (2)1( 2.5) 1646061. 9 4d(2D) (2)2( 4.5) 1646062. 10 4f(2F) (2)3( 6.5) 1646063. -1 4.00 3 2.00+04 5.00+04 1.00+05 2.00+05 5.00+05 1.00+06 2.00+06 5.00+06 2 1 0.00+00 3.62-02 3.57-02 3.63-02 3.64-02 3.53-02 3.51-02 3.64-02 4.00-02 5.55-02 3 1 1.60+11 1.34-01 1.36-01 1.42-01 1.49-01 1.64-01 1.88-01 2.30-01 3.18-01 2.77-01 4 1 0.00+00 1.17-02 1.06-02 9.64-03 8.65-03 7.60-03 7.19-03 7.19-03 7.76-03 1.10-02 5 1 4.28+10 2.81-02 2.73-02 2.71-02 2.73-02 2.97-02 3.39-02 4.06-02 5.40-02 4.45-02 6 1 0.00+00 1.41-02 1.27-02 1.12-02 9.33-03 7.24-03 6.20-03 5.73-03 5.86-03 8.47-03 7 1 0.00+00 4.30-03 4.04-03 3.69-03 3.32-03 2.91-03 2.71-03 2.68-03 2.86-03 4.10-03 8 1 1.75+10 8.31-03 8.28-03 8.34-03 8.77-03 1.01-02 1.18-02 1.43-02 1.90-02 1.55-02 9 1 0.00+00 5.42-03 4.97-03 4.42-03 3.88-03 3.28-03 2.94-03 2.78-03 2.85-03 4.01-03 10 1 0.00+00 1.97-03 1.59-03 1.15-03 7.84-04 4.57-04 3.01-04 2.02-04 1.29-04 6.11-05 4 2 0.00+00 2.72-01 2.84-01 2.99-01 3.22-01 3.69-01 4.17-01 4.71-01 5.38-01 6.64-01 5 2 5.75+09 6.33-01 6.30-01 6.40-01 6.91-01 9.06-01 1.24+00 1.75+00 2.65+00 1.57+00 6 2 0.00+00 7.61-01 7.75-01 7.89-01 8.31-01 9.88-01 1.19+00 1.41+00 1.68+00 2.10+00 7 2 0.00+00 5.44-02 5.46-02 5.50-02 5.74-02 6.50-02 7.38-02 8.46-02 9.93-02 1.29-01 8 2 2.48+09 1.49-01 1.46-01 1.44-01 1.51-01 1.86-01 2.42-01 3.27-01 4.78-01 2.74-01 9 2 0.00+00 1.47-01 1.40-01 1.32-01 1.28-01 1.38-01 1.55-01 1.78-01 2.08-01 2.62-01 10 2 0.00+00 1.26-01 1.18-01 1.07-01 1.02-01 1.05-01 1.13-01 1.22-01 1.30-01 1.37-01 4 3 1.62+09 4.38-01 3.94-01 3.40-01 2.80-01 2.23-01 2.11-01 2.28-01 2.90-01 1.47-01 5 3 0.00+00 1.84+00 1.73+00 1.63+00 1.54+00 1.53+00 1.61+00 1.73+00 1.89+00 2.18+00 6 3 1.66+10 5.05+00 5.22+00 5.40+00 5.81+00 7.20+00 9.17+00 1.20+01 1.66+01 7.51+00 7 3 6.60+08 1.48-01 1.27-01 1.06-01 8.55-02 6.52-02 5.65-02 5.43-02 6.04-02 2.44-02 8 3 0.00+00 4.48-01 4.10-01 3.68-01 3.35-01 3.17-01 3.23-01 3.40-01 3.68-01 4.28-01 9 3 5.28+09 8.67-01 8.98-01 9.15-01 9.71-01 1.16+00 1.43+00 1.80+00 2.39+00 9.74-01 10 3 0.00+00 5.57-01 5.08-01 4.45-01 3.96-01 3.74-01 3.92-01 4.28-01 4.80-01 5.83-01 7 4 0.00+00 7.69-01 9.22-01 1.08+00 1.30+00 1.66+00 1.94+00 2.20+00 2.47+00 2.86+00 8 4 7.85+08 1.54+00 1.60+00 1.76+00 2.18+00 3.44+00 5.07+00 7.24+00 1.07+01 4.99+00 9 4 0.00+00 1.81+00 1.94+00 2.13+00 2.51+00 3.31+00 4.02+00 4.65+00 5.23+00 5.84+00 10 4 0.00+00 1.95+00 1.95+00 1.94+00 2.02+00 2.25+00 2.46+00 2.64+00 2.80+00 2.98+00 7 5 4.70+08 1.13+00 1.02+00 9.17-01 8.65-01 9.69-01 1.21+00 1.59+00 2.25+00 9.95-01 8 5 0.00+00 3.79+00 4.15+00 4.54+00 5.16+00 6.28+00 7.21+00 8.08+00 8.96+00 1.02+01 9 5 1.80+09 8.37+00 8.82+00 9.68+00 1.17+01 1.74+01 2.44+01 3.34+01 4.74+01 1.91+01 10 5 0.00+00 7.13+00 7.38+00 7.76+00 8.79+00 1.13+01 1.37+01 1.58+01 1.78+01 1.98+01 7 6 0.00+00 9.60-01 8.06-01 6.36-01 5.01-01 3.99-01 3.65-01 3.51-01 3.44-01 3.40-01 8 6 8.90+07 4.08+00 3.51+00 2.88+00 2.34+00 1.92+00 1.83+00 1.91+00 2.19+00 5.65-01 9 6 0.00+00 9.63+00 9.45+00 9.16+00 9.26+00 1.01+01 1.09+01 1.17+01 1.25+01 1.36+01 10 6 3.53+09 3.28+01 3.52+01 3.87+01 4.59+01 6.45+01 8.64+01 1.14+02 1.54+02 5.23+01 -1 -1 -1 C------------------------------------------------------------------------------- C C From a 57 term R-matrix with pseudo states (RMPS) calculation. C The close-coupling expansion included the 9 spectroscopic terms C arising from the configurations 1s, 2l, 3l, and 4l. In addition it, C included the 48 pseudo-state terms arising from the configurations C 5l with l = 0 to 4 and nl with n = 6 to 12 and l = 0 to 5. The C pseudo orbitals were generated from a set of non-orthogonal C Laguerre orbitals that were then orthogonalized to the spectroscopic C orbitals and to each other. The screening parameters for the Laguerre C orbitals were adjusted to obtain a good distribution of pseudo states C above and below the ionization limit. In STG3 of the R-Matrix C calculation, the term energies were adjusted to the experimental C values. C C For all LSPI partial waves from L=0 to 11, we performed an RMPS C calculation with exchange. For the LSPI partial waves from L=12 C to 50, we performed a no-exchange RMPS calculation. These partial C waves were then topped up. The size of the continuum basis was C 51 and the size of the R-matrix "box" was 21.4 au. In the resonance C region of the calculation, we used an energy mesh spacing of C 5.0e-04 Ryd; above all thresholds of the 5l configurations, we C employed an energy-mesh spacing of 1.4e-02 Ryd up to a total C energy of 30 Ryd. C C Note we do not include data for transitions between degenerate levels C for hydrogenic systems 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 NAME: C Ballance and D Griffin DATE: July 22, 2003 C-------------------------------------------------------------------------------