Be+ 2 4 3 1241242.(2S) 1 1s2(1S) (1)0( 0.0) 0. 2 1s2s(3S) (3)0( 1.0) 956502. 3 1s2s(1S) (1)0( 0.0) 981178. 4 1s2p(3P) (3)1( 4.0) 983355. 5 1s2p(1P) (1)1( 1.0) 997454. 6 1s3s(3S) (3)0( 1.0) 1121184. 7 1s3s(1S) (1)0( 0.0) 1127704. 8 1s3p(3P) (3)1( 4.0) 1128300. 9 1s3d(3D) (3)2( 7.0) 1131383. 10 1s3d(1D) (1)2( 2.0) 1131462. 11 1s3p(1P) (1)1( 1.0) 1132390. 12 1s4s(3S) (3)0( 1.0) 1175295. 13 1s4s(1S) (1)0( 0.0) 1178005. 14 1s4p(3P) (3)1( 4.0) 1178173. 15 1s4d(3D) (3)2( 7.0) 1179451. 16 1s4d(1D) (1)2( 2.0) 1179495. 17 1s4f(1F) (1)3( 3.0) 1179514. 18 1s4f(3F) (3)3(10.0) 1179515. 19 1s4p(1P) (1)1( 1.0) 1179830. -1 3.00 3 1.00+04 2.00+04 5.00+04 1.00+05 2.00+05 5.00+05 1.00+06 2.00+06 2 1 0.00+00 4.99-02 4.94-02 4.01-02 3.26-02 2.62-02 1.88-02 1.41-02 9.98-03 0.00+00 3 1 0.00+00 2.68-02 2.58-02 2.41-02 2.33-02 2.28-02 2.33-02 2.50-02 2.83-02 5.37-02 4 1 0.00+00 7.35-02 7.23-02 6.93-02 6.69-02 6.27-02 5.31-02 4.33-02 3.25-02 0.00+00 5 1 1.25+11 3.51-02 3.61-02 3.97-02 4.48-02 5.35-02 7.75-02 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2.24+01 2.60+01 2.88+01 3.12+01 3.61+01 16 9 0.00+00 2.89+00 2.48+00 1.79+00 1.26+00 8.27-01 4.31-01 2.48-01 1.37-01 0.00+00 17 9 0.00+00 4.19+00 3.79+00 2.93+00 2.17+00 1.47+00 7.86-01 4.55-01 2.51-01 0.00+00 18 9 1.12+09 6.07+01 6.49+01 7.51+01 9.21+01 1.24+02 1.94+02 2.65+02 3.46+02 1.39+02 19 9 0.00+00 1.24+00 1.12+00 8.45-01 6.05-01 3.97-01 2.04-01 1.15-01 6.28-02 0.00+00 11 10 1.20+04 1.23+02 1.37+02 1.62+02 1.85+02 2.11+02 2.48+02 2.75+02 3.01+02 2.97+01 12 10 0.00+00 1.68+00 1.13+00 6.27-01 3.85-01 2.27-01 1.07-01 5.83-02 3.09-02 0.00+00 13 10 0.00+00 1.25+00 8.71-01 5.61-01 4.33-01 3.75-01 3.59-01 3.63-01 3.67-01 3.63-01 14 10 0.00+00 2.73+00 1.96+00 1.23+00 8.09-01 5.04-01 2.49-01 1.38-01 7.45-02 0.00+00 15 10 0.00+00 2.75+00 2.34+00 1.69+00 1.20+00 7.89-01 4.14-01 2.39-01 1.32-01 0.00+00 16 10 0.00+00 6.17+00 6.03+00 6.02+00 6.40+00 7.19+00 8.61+00 9.64+00 1.05+01 1.21+01 17 10 1.12+09 1.85+01 2.01+01 2.40+01 3.02+01 4.11+01 6.49+01 8.90+01 1.16+02 4.66+01 18 10 0.00+00 4.36+00 3.94+00 3.04+00 2.25+00 1.52+00 8.14-01 4.70-01 2.59-01 0.00+00 19 10 2.32+07 2.29+00 2.16+00 1.86+00 1.63+00 1.48+00 1.44+00 1.52+00 1.67+00 4.04-01 12 11 0.00+00 8.98-01 5.83-01 3.17-01 1.93-01 1.15-01 5.48-02 3.02-02 1.62-02 0.00+00 13 11 2.56+08 1.09+00 9.41-01 8.54-01 9.00-01 1.10+00 1.69+00 2.40+00 3.28+00 1.78+00 14 11 0.00+00 1.03+00 7.79-01 5.13-01 3.48-01 2.23-01 1.15-01 6.65-02 3.74-02 0.00+00 15 11 0.00+00 1.27+00 1.11+00 8.19-01 5.83-01 3.84-01 1.99-01 1.13-01 6.15-02 0.00+00 16 11 5.95+08 5.19+00 5.58+00 6.64+00 8.50+00 1.21+01 2.03+01 2.90+01 3.92+01 1.87+01 17 11 0.00+00 3.48+00 3.80+00 4.50+00 5.61+00 7.45+00 1.07+01 1.31+01 1.49+01 1.81+01 18 11 0.00+00 1.55+00 1.42+00 1.09+00 8.07-01 5.55-01 3.06-01 1.81-01 1.02-01 0.00+00 19 11 0.00+00 1.65+00 1.92+00 2.51+00 3.22+00 4.18+00 5.66+00 6.76+00 7.69+00 9.73+00 13 12 0.00+00 1.12+00 8.09-01 5.01-01 3.36-01 2.26-01 1.39-01 9.71-02 6.62-02 0.00+00 14 12 9.17+05 2.98+02 3.71+02 5.22+02 6.78+02 8.64+02 1.14+03 1.34+03 1.53+03 2.28+02 15 12 0.00+00 9.09+01 8.89+01 8.42+01 8.06+01 7.82+01 7.66+01 7.58+01 7.51+01 7.30+01 16 12 0.00+00 1.39+00 1.26+00 8.94-01 5.99-01 3.69-01 1.77-01 9.68-02 5.12-02 0.00+00 17 12 0.00+00 2.06+00 1.77+00 1.20+00 7.80-01 4.68-01 2.19-01 1.17-01 6.12-02 0.00+00 18 12 0.00+00 1.82+01 1.72+01 1.42+01 1.20+01 1.07+01 1.00+01 9.92+00 9.95+00 1.01+01 19 12 0.00+00 7.01-01 6.69-01 4.97-01 3.44-01 2.20-01 1.12-01 6.45-02 3.61-02 0.00+00 14 13 0.00+00 1.87+00 1.34+00 8.07-01 5.10-01 3.06-01 1.47-01 8.20-02 4.48-02 0.00+00 15 13 0.00+00 1.42+00 1.27+00 9.01-01 6.03-01 3.70-01 1.77-01 9.64-02 5.08-02 0.00+00 16 13 0.00+00 2.46+01 2.45+01 2.40+01 2.37+01 2.37+01 2.40+01 2.41+01 2.42+01 2.38+01 17 13 0.00+00 4.75+00 4.48+00 3.76+00 3.29+00 3.04+00 2.96+00 2.98+00 3.00+00 3.03+00 18 13 0.00+00 2.25+00 1.93+00 1.30+00 8.43-01 5.03-01 2.33-01 1.24-01 6.47-02 0.00+00 19 13 2.43+05 1.45+02 1.76+02 2.36+02 2.94+02 3.62+02 4.59+02 5.31+02 5.98+02 7.88+01 15 14 8.27+04 9.33+02 1.11+03 1.43+03 1.74+03 2.09+03 2.59+03 2.95+03 3.29+03 3.92+02 16 14 0.00+00 4.20+00 3.80+00 2.70+00 1.81+00 1.12+00 5.44-01 3.01-01 1.62-01 0.00+00 17 14 0.00+00 6.36+00 5.36+00 3.60+00 2.36+00 1.44+00 6.81-01 3.68-01 1.93-01 0.00+00 18 14 0.00+00 1.08+02 1.05+02 9.43+01 8.69+01 8.22+01 7.93+01 7.80+01 7.67+01 7.28+01 19 14 0.00+00 2.57+00 2.38+00 1.77+00 1.27+00 8.68-01 5.18-01 3.48-01 2.29-01 0.00+00 16 15 0.00+00 9.57+00 8.67+00 6.26+00 4.31+00 2.79+00 1.50+00 9.32-01 5.71-01 0.00+00 17 15 0.00+00 1.24+01 1.08+01 7.38+00 4.86+00 2.95+00 1.40+00 7.61-01 4.01-01 0.00+00 18 15 6.28+00 2.15+03 2.51+03 3.01+03 3.39+03 3.77+03 4.25+03 4.58+03 4.89+03 3.37+02 19 15 0.00+00 3.51+00 3.29+00 2.41+00 1.64+00 1.03+00 5.01-01 2.78-01 1.49-01 0.00+00 17 16 1.63-01 8.68+02 1.03+03 1.23+03 1.38+03 1.51+03 1.68+03 1.80+03 1.90+03 1.12+02 18 16 0.00+00 1.38+01 1.18+01 7.95+00 5.19+00 3.14+00 1.48+00 8.01-01 4.21-01 0.00+00 19 16 2.40+03 4.91+02 5.82+02 7.29+02 8.55+02 9.86+02 1.16+03 1.28+03 1.39+03 1.26+02 18 17 0.00+00 2.80+01 2.47+01 1.76+01 1.20+01 7.66+00 3.95+00 2.33+00 1.35+00 0.00+00 19 17 0.00+00 2.89+01 2.89+01 2.71+01 2.57+01 2.49+01 2.43+01 2.40+01 2.36+01 2.23+01 19 18 0.00+00 5.42+00 4.71+00 3.27+00 2.18+00 1.34+00 6.37-01 3.44-01 1.80-01 0.00+00 -1 -1 -1 C------------------------------------------------------------------------------- C C From a 103 term R-matrix with pseudo states (RMPS) calculation. C The close-coupling expansion included the 21 spectroscopic terms C arising from the configurations 1s2, 1s2l, 1s3l, 1s4l, 2s2, and C 3s2. In addition it, included the 84 pseudo-state terms arising C from the configurations 1s5l with l = 0 to 4, and 1snl with n = 6 C to 11 and l = 0 to 5. The spectrospic orbitals (1s - 4f) were C determined from local potentials using Slater-type orbitals. 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 C Laguerre orbitals were adjusted to obtain a good distribution of C pseudo states above and below the ionization limit. In STG3 of C the R-Matrix calculation, the term energies were adjusted to the C experimental 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 45 and the size of the R-matrix "box" was 25.9 au. In the resonance C region of the calculation, we used an energy mesh spacing of C 1.0e-03 Ryd; above all thresholds of the 1s5l configurations, we C employed an energy-mesh spacing of 5.0e-02 Ryd up to a total C energy of 18.4 Ryd. The radiative rates were determined from C an LS-coupling configuration-interaction expansion that employed C all 103 terms included in the close-coupling expansion for the C RMPS calculation. 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-------------------------------------------------------------------------------