From a simplified
version of the mathematical structure of the
strong coupling limit of the exact exchange-correlation functional,
we construct an approximation for the electronic repulsion energy
at physical coupling strength, which is fully nonlocal. This functional
is self-interaction free and yields energy densities within the definition
of the electrostatic potential of the exchange-correlation hole that
are locally accurate and have the correct asymptotic behavior. The
model is able to capture strong correlation effects that arise from
chemical bond dissociation, without relying on error cancellation.
These features, which are usually missed by standard density functional
theory (DFT) functionals, are captured by the highly nonlocal structure,
which goes beyond the “Jacob’s ladder” framework
for functional construction, by using integrals of the density as
the key ingredient. Possible routes for obtaining the full exchange-correlation
functional by recovering the missing kinetic component of the correlation
energy are also implemented and discussed.