Be+ 0 4 1 75193.(2S) 1 1s22s2(1S) (1)0( 0.0) 0. 2 1s22s2p(3P) (3)1( 4.0) 21980. 3 1s22s2p(1P) (1)1( 1.0) 42565. 4 1s22s3s(3S) (3)0( 1.0) 52081. 5 1s22s3s(1S) (1)0( 0.0) 54677. 6 1s22p2(1D) (1)2( 2.0) 56882. 7 1s22s3p(3P) (3)1( 4.0) 58908. 8 1s22p2(3P) (3)1( 4.0) 59696. 9 1s22s3p(1P) (1)1( 1.0) 60187. 10 1s22s3d(3D) (3)2( 7.0) 62054. 11 1s22s3d(1D) (1)2( 2.0) 64428. 12 1s22s4s(3S) (3)0( 1.0) 64506. 13 1s22s4s(1S) (1)0( 0.0) 65245. 14 1s22s4p(3P) (3)1( 4.0) 66812. 15 1s22s4p(1P) (1)1( 1.0) 67035. 16 1s22s4d(3D) (3)2( 7.0) 67942. 17 1s22s4f(3F) (3)3(10.0) 68241. 18 1s22s4f(1F) (1)3( 3.0) 68242. 19 1s22s4d(1D) (1)2( 2.0) 68781. -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 0.00+00 1.40+00 2.14+00 3.13+00 3.56+00 3.56+00 2.88+00 2.13+00 1.44+00 0.00+00 3 1 5.51+08 6.79-02 1.53-01 3.95-01 8.65-01 1.85+00 4.43+00 7.80+00 1.26+01 1.41+01 4 1 0.00+00 2.55-02 8.59-02 1.84-01 2.13-01 2.01-01 1.56-01 1.15-01 7.84-02 0.00+00 5 1 0.00+00 1.59-02 4.49-02 9.44-02 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0.00+00 9.92-01 2.10+00 4.21+00 6.59+00 1.05+01 1.96+01 2.87+01 3.79+01 6.00+01 16 9 0.00+00 1.05+00 1.58+00 1.98+00 1.90+00 1.58+00 1.02+00 6.58-01 3.92-01 0.00+00 17 9 0.00+00 4.10-01 8.03-01 1.37+00 1.61+00 1.55+00 1.15+00 7.83-01 4.85-01 0.00+00 18 9 0.00+00 1.72+00 3.50+00 7.20+00 1.16+01 1.86+01 3.32+01 4.70+01 5.97+01 7.78+01 19 9 2.69+05 5.39-01 1.15+00 2.37+00 3.50+00 4.86+00 6.70+00 7.77+00 8.56+00 1.39+00 11 10 0.00+00 1.35+00 3.76+00 7.38+00 8.53+00 7.89+00 5.61+00 3.86+00 2.48+00 0.00+00 12 10 0.00+00 4.29+00 9.75+00 1.68+01 1.99+01 2.25+01 2.89+01 3.78+01 4.80+01 6.98+01 13 10 0.00+00 5.40-01 9.76-01 1.30+00 1.21+00 9.72-01 6.24-01 4.00-01 2.37-01 0.00+00 14 10 1.91+06 9.98+00 1.78+01 2.86+01 3.74+01 5.12+01 8.66+01 1.32+02 1.92+02 1.05+02 15 10 0.00+00 9.36-01 1.57+00 2.31+00 2.45+00 2.17+00 1.48+00 9.62-01 5.73-01 0.00+00 16 10 0.00+00 1.12+01 1.97+01 3.43+01 4.95+01 7.33+01 1.20+02 1.61+02 1.99+02 2.74+02 17 10 1.52+07 5.86+00 1.33+01 3.41+01 7.05+01 1.51+02 4.20+02 8.19+02 1.37+03 8.85+02 18 10 0.00+00 1.74+00 2.87+00 4.06+00 4.30+00 3.90+00 2.78+00 1.88+00 1.16+00 0.00+00 19 10 0.00+00 6.79-01 1.32+00 2.16+00 2.39+00 2.19+00 1.54+00 1.04+00 6.55-01 0.00+00 12 11 0.00+00 4.27-01 1.43+00 2.60+00 2.56+00 1.99+00 1.17+00 7.03-01 3.97-01 0.00+00 13 11 0.00+00 1.44+00 2.97+00 5.02+00 6.85+00 1.01+01 1.80+01 2.67+01 3.58+01 5.70+01 14 11 0.00+00 3.21+00 5.11+00 6.18+00 5.53+00 4.26+00 2.54+00 1.55+00 8.85-01 0.00+00 15 11 1.64+06 4.02+00 1.01+01 2.66+01 5.17+01 9.72+01 2.04+02 3.25+02 4.67+02 1.83+02 16 11 0.00+00 4.86+00 7.38+00 9.13+00 8.45+00 6.65+00 4.05+00 2.53+00 1.50+00 0.00+00 17 11 0.00+00 2.01+00 3.82+00 6.06+00 6.65+00 6.09+00 4.30+00 2.87+00 1.74+00 0.00+00 18 11 7.28+06 6.16+00 1.52+01 3.89+01 7.94+01 1.70+02 4.42+02 8.00+02 1.25+03 6.05+02 19 11 0.00+00 2.50+00 6.44+00 1.50+01 2.38+01 3.70+01 6.36+01 8.81+01 1.12+02 1.62+02 13 12 0.00+00 5.64-01 8.73-01 1.04+00 9.28-01 7.34-01 5.03-01 3.71-01 2.64-01 0.00+00 14 12 1.92+06 1.49+01 3.17+01 7.27+01 1.55+02 3.48+02 8.89+02 1.55+03 2.34+03 9.26+02 15 12 0.00+00 2.18-01 4.74-01 8.28-01 9.18-01 8.40-01 5.95-01 4.01-01 2.48-01 0.00+00 16 12 0.00+00 1.33+01 2.12+01 4.01+01 6.87+01 1.14+02 1.95+02 2.61+02 3.14+02 3.35+02 17 12 0.00+00 9.14+00 1.58+01 2.83+01 3.81+01 4.85+01 6.46+01 7.73+01 8.75+01 9.10+01 18 12 0.00+00 1.65+00 2.43+00 2.87+00 2.57+00 1.96+00 1.15+00 6.98-01 3.96-01 0.00+00 19 12 0.00+00 3.96-01 7.03-01 1.01+00 1.03+00 8.85-01 5.82-01 3.70-01 2.17-01 0.00+00 14 13 0.00+00 1.17+00 1.60+00 1.71+00 1.47+00 1.12+00 6.93-01 4.43-01 2.66-01 0.00+00 15 13 1.01+06 3.48+00 1.17+01 4.06+01 9.05+01 1.87+02 4.24+02 6.94+02 1.01+03 3.46+02 16 13 0.00+00 1.78+00 2.51+00 2.79+00 2.45+00 1.89+00 1.13+00 6.83-01 3.88-01 0.00+00 17 13 0.00+00 4.21-01 8.29-01 1.29+00 1.36+00 1.21+00 8.28-01 5.37-01 3.17-01 0.00+00 18 13 0.00+00 1.84+00 3.16+00 5.13+00 6.95+00 9.77+00 1.60+01 2.20+01 2.75+01 3.23+01 19 13 0.00+00 1.15+00 3.75+00 1.15+01 2.16+01 3.63+01 6.20+01 8.18+01 9.61+01 9.14+01 15 14 0.00+00 1.72+00 3.08+00 4.21+00 4.04+00 3.27+00 2.10+00 1.41+00 9.25-01 0.00+00 16 14 4.13+05 8.21+01 1.64+02 5.05+02 1.15+03 2.32+03 4.87+03 7.49+03 1.03+04 2.83+03 17 14 0.00+00 8.36+01 1.58+02 2.83+02 3.73+02 4.60+02 5.86+02 6.79+02 7.43+02 7.70+02 18 14 0.00+00 5.89+00 9.27+00 1.10+01 9.56+00 7.00+00 3.93+00 2.33+00 1.31+00 0.00+00 19 14 0.00+00 1.33+00 2.63+00 4.19+00 4.26+00 3.47+00 2.11+00 1.30+00 7.56-01 0.00+00 16 15 0.00+00 2.92+00 4.75+00 5.79+00 5.26+00 4.12+00 2.48+00 1.53+00 8.83-01 0.00+00 17 15 0.00+00 1.57+00 3.21+00 4.96+00 5.04+00 4.23+00 2.74+00 1.74+00 1.02+00 0.00+00 18 15 0.00+00 8.62+00 1.57+01 2.84+01 4.14+01 6.15+01 1.06+02 1.48+02 1.87+02 2.45+02 19 15 1.41+06 6.87+00 2.12+01 8.05+01 1.92+02 4.14+02 9.79+02 1.64+03 2.41+03 8.69+02 17 16 5.97+03 1.04+03 1.94+03 3.85+03 5.89+03 8.41+03 1.24+04 1.59+04 1.93+04 3.07+03 18 16 0.00+00 3.81+00 8.48+00 1.37+01 1.38+01 1.12+01 6.79+00 4.18+00 2.41+00 0.00+00 19 16 0.00+00 2.02+00 3.95+00 6.35+00 6.80+00 5.92+00 3.92+00 2.58+00 1.63+00 0.00+00 18 17 0.00+00 2.51+00 6.76+00 1.30+01 1.47+01 1.34+01 9.40+00 6.43+00 4.12+00 0.00+00 19 17 0.00+00 1.64+00 3.84+00 6.65+00 7.15+00 6.25+00 4.19+00 2.72+00 1.62+00 0.00+00 19 18 3.46+04 1.19+02 2.51+02 5.51+02 8.98+02 1.37+03 2.18+03 2.90+03 3.65+03 7.28+02 -1 -1 -1 C------------------------------------------------------------------------------- C C From a 280 term R-matrix with pseudo states (RMPS) calculation. C The close-coupling expansion included the 54 spectroscopic terms C arising from the configurations 2s2, 2s2p, 2p2, 2s3l, 2s4l, C 2p3l, 2p4l. In addition it, included the 226 pseudo-state C terms arising from the configurations 2snl with n = 5 to 11 and C l = 0 to 4, and 2pnl with n = 5 to 10 and l = 0 to 4. The C spectrospic orbitals (1s - 4f) were determined from local C potentials using Slater-type orbitals. The pseudo orbitals C were generated from a set of non-orthogonal Laguerre orbitals C that were then orthogonalized to the spectroscopic orbitals and C to each other. The screening parameters for the Laguerre orbitals C 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 20, we performed a no-exchange RMPS calculation. This was then C supplemented with a no-exchange 29-term R-matrix calculation C (all 19 terms listed here plus the ten 2s5l terms) for which C the configuration-interaction expansion of the target employed C all 280 terms included in the close-coupling expansion of the C RMPS calculation. These partial waves were then topped up. C The size of the continuum basis was 45 and the size of the C R-matrix "box" was 71.7 au. In the resonance region of the C calculation, we used an energy mesh spacing of 3.5e-04 Ryd; C above all thresholds of the 2s5l configurations, we C employed an energy-mesh spacing of 9.7e-3 Ryd up to a total C energy of 2.5 Ryd. The radiative rates were determined from C an LS-coupling configuration-interaction expansion that employed C all 280 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 & D Griffin DATE: July 22, 2003 C-------------------------------------------------------------------------------