  A novel dielectric scheme is proposed for strongly coupled electron liquids
that handles quantum mechanical effects beyond the random phase approximation
level and treats electronic correlations within the integral equation theory of
classical liquids. The self-consistent scheme features a complicated dynamic
local field correction functional and its formulation is guided by ab initio
path integral Monte Carlo simulations. Remarkably, our scheme is capable to
provide unprecedently accurate results for the static structure factor with the
exception of the Wigner crystallization vicinity, despite the absence of
adjustable or empirical parameters.
