This Appendix is adopted from the Ph.D. Thesis by Alston Misquitta [66].
The following procedure can be applied to construct an
auxiliary basis set for each atom in the dimer under consideration. Denoted
by is the decontracted basis set used in calculations for
given dimer. The auxiliary basis, denoted by
, is
developed as follows:
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(15) |
If G(li,αi) and
G
(lj,αj) are
two basis functions of
centered at the same point, where
li
and lj are the angular quantum numbers and
αi and αj are
the exponents, then the product is a basis function belonging to
centered at the same point and given by
G
(lk,αk)
where lk = li +
lj
and αk = αi +
αj. The resulting basis
is a (large) basis including high symmetry functions compared to the
original basis. All the products involving basis functions from
different centers are rejected.
We have found the optimal values of ϵ used in the pruning process to be between 0.3 and
0.5. This procedure typically results in an auxiliary basis that
is 2 to 3 times larger than the basis used to obtain molecular orbitals and
eigenvalues. While in general the auxiliary basis for a molecule should be
centered also on sites between pairs of atoms in addition to atomic sites,
it is our experience that the use of only atomic centers is adequate. This
is also true for the optimized auxiliary basis sets [14].