The recent idea of extracting effective atomic orbitals from molecular
wave functions by performing independent localization transformations
for each atom separately is generalized to the case of an arbitrary H
ermitian bilinear localization functional. The general equations are d
erived and the orthogonality relationships pertinent to the localized
molecular orbitals are proved, The ''intraatomic components'' of these
localized orbitals form an effective atomic basis, which is also auto
matically orthogonal if some conditions are fulfilled. Several differe
nt localization functionals are considered and it is shown that for th
e simplest one the orbitals obtained are natural hybrids in McWeeny's
sense and are conceptually close to (but not identical with) Weinhold'
s ''natural hybrid orbitals''. In this case one obtains for each atom
of a ''usual'' molecule as many effective AOs of appreciable importanc
e as the number of orbitals contained in the classical ''minimal basis
'' of that atom, forming therefore a-distorted but still orthogonal-ef
fective minimal basis of the atom within the molecule. The similaritie
s and differences with Weinhold's ''atomic natural orbitals'' are also
discussed. It is pointed out that by selecting a proper localization
functional, the present approach can also be used to define the effect
ive atomic orbitals in a basis-free manner, i.e. even if no atom-cente
red basis was used in calculating the wave function. A possibility of
generalization for correlated wave functions is also suggested.