click here). Pseudopotentials a) are adjusted to orbital energies and densities of a suitable atomic reference state, while pseudopotentials b) are generated using total valence energies of a multitude of atomic states.
Library keywords in case a) are ECP1 and ECP2;
ECP2 is used when more than
one pseudopotential is available for a given atom and then denotes the ECP
with the smaller core definition. (For Cu, e.g., ECP1
refers to an Ar-like
18-core, while ECP2
simulates a Ne-like 10
one with the
and
electrons promoted to the valence shell). For accurate calculations
including electron correlation, promotion of all core orbitals with main
quantum number equal to any of the valence orbitals is recommended.
Library keywords in case b) are of the form ECP;
is the number
of core electrons which are replaced by the pseudopotential,
denotes
the reference system used for generating the pseudopotential (
:
single-valence-electron ion;
: neutral atom), and
stands for the
theoretical level of the reference data (
: Hartree-Fock,
:
quasi-relativistic;
: relativistic).
For one- or two-valence electron atoms
,
is a good choice, while
otherwise
,
(or
)
is recommended. (For light atoms, or for the discussion
of relativistic effects, the corresponding
pseudopotentials may be
useful.) Additionally, spin-orbit (SO) potentials and core-polarization potentials (CPP)
are available, to be used in connection with case b) ECPs, but these are not
currently contained in the library, so explicit input is necessary here (cf. below).
In both cases, a) and b), the same keywords refer to the pseudopotential and the corresponding basis set, with a prefix MBS-...in case a).
P.J. Knowles and H.-J. Werner