All extrapolations in W2 theory are normally done on components of the *total atomization energy*, not of the *total energy*. (Some reliance on cancellation between atom and molecule is relied upon.) For the benefit of people who would like to report "W2 total energies", we here put W2 values for the total energies of the atoms. SCF limit CCSD-SCF (T) frozen core core corr. E(W2) scalar rel. spin-orbit E(W2) val.limit val.limit limit nonrel. H(2S) -0.500022 0.000000 0.000000 -0.500022 0.000000 -0.500022 -0.000007 0.000000 -0.500028 B(2P) -24.529141 -0.071323 -0.001687 -24.602151 -0.044682 -24.646833 -0.006795 -0.000046 -24.653674 C(3P) -37.688735 -0.098181 -0.002685 -37.789601 -0.048308 -37.837909 -0.015050 -0.000135 -37.853094 N(4S) -54.401056 -0.126121 -0.003194 -54.530371 -0.051852 -54.582223 -0.029379 0.000000 -54.611602 O(3P) -74.812681 -0.188512 -0.004282 -75.005475 -0.054737 -75.060212 -0.052387 -0.000355 -75.112954 F(2P) -99.411966 -0.252012 -0.005386 -99.669364 -0.057573 -99.726938 -0.087173 -0.000614 -99.814725 Al(2P) -241.876883 -0.056632 -0.001562 -241.935077 -0.272005 -242.207082 -0.435782 -0.000340 -242.643205 Si(3P) -288.854531 -0.082216 -0.003258 -288.940004 -0.288872 -289.228876 -0.602539 -0.000682 -289.832097 P(4S) -340.718740 -0.108115 -0.004998 -340.831853 -0.300512 -341.132365 -0.814307 0.000000 -341.946673 S(3P) -397.507228 -0.161199 -0.006677 -397.675104 -0.307406 -397.982510 -1.078965 -0.000892 -399.062367 Cl(2P) -459.483910 -0.213836 -0.008326 -459.706072 -0.316593 -460.022664 -1.405037 -0.001340 -461.429041 For comparison, here are limits with best basis from electron affinities paper: G. de Oliveira, J. M. L. Martin, F. De Proft, and P. Geerlings, Phys. Rev. A, in press. ACV5Z 1st row best [a] best [a] AVQZ best [b] best best [c] best [c] best SCF limit CCSD(T)-SCF CCSDT- FCI-CCSDT valence (2s,2p)core (1s)core nonrelativ. limit CCSD(T) corr.only energy H(2S) -0.500000 0.000000 0.000000 0.000000 -0.500000 0.000000 -0.500000 B(2P) -24.529137 -0.072918 -0.000413 0.000007 -24.602462 -0.051632 -24.654094 C(3P) -37.688692 -0.100690 -0.000491 -0.000018 -37.789891 -0.055328 -37.845219 N(4S) -54.400932 -0.129001 -0.000421 0.000010 -54.530344 -0.059151 -54.589495 O(3P) -74.812392 -0.192368 -0.000354 0.000018 -75.005096 -0.062518 -75.067614 F(2P) -99.411405 -0.256940 -0.000189 -0.000059 -99.668593 -0.065784 -99.734378 Al(2P) -241.876880 -0.058220 -0.000461 0.000003 -241.935558 -0.322868 -0.074003 -242.332428 Si(3P) -288.854522 -0.085568 -0.000708 -0.000078 -288.940876 -0.315580 -0.072670 -289.329127 P(4S) -340.718740 -0.112615 -0.000758 -0.000124 -340.832237 -0.331245 -0.076841 -341.240323 S(3P) -397.507217 -0.168245 -0.000799 -0.000162 -397.676422 -0.338780 -0.077982 -398.093184 Cl(2P) -459.483896 -0.222719 -0.000682 -0.000201 -459.707497 -0.344386 -0.078633 -460.130516 [a] AVnZ (n=4,5,6) for H, B, C, N, O, F; n=3,4,5 for Al and Si; dAVnZ (n=3,4,5) for P, S, Cl [b] AVQZ for B and Al; AVTZ for C and Si; AVDZ for rest [c] extrapolated from MTavqz and MTav5z basis sets for 2nd row; from ACVQZ and ACV5Z basis sets for 1st row Note that limits for core correlation are much less reliable than those for valence correlation, since the basis set increments involved are much larger. (Most of this of course cancels between atom and molecule, which is why you can get away with using a basis set like MTsmall for inner-shell correlation.) Last updated July 21, 1999 by comartin@wicc.weizmann.ac.il