Treatment of electron-electron correlations in electronic structure calculations

A methodology is introduced for the systematic treatment of electron-electron correlations in solids and other interacting quantum $N$-particle systems. The method is developed within the framework of electronic structure theory (band theory) but, in contrast to conventional approaches, which are based on the single-particle picture, it is formulated within a many-particle picture in which $n$ particles in $d$-dimensional phase space are treated as a single particle in a phase space of $\mathrm{nd}$ dimensions. In this phase space, interparticle interactions appear as external potentials allowing the treatment of the system of particles through the use of single-particle methods, while at the same time allowing a systematic, direct, and nonperturbative treatment of interparticle interactions. The method makes use of the invariance of the Hamiltonian describing an interacting-particle system under partitioning into subsystems of $n$ particles. This treatment leads to exact results in the limit $n\to N$. Based on such partitioning, we propose a generalization of density functional theory and an appropriately defined local density approximation to treat the interactions between the $n$-particle units in a system of $N>~n$ particles. This approach yields $n$-particle correlated densities and $n$-particle states which can be used in an analysis of the electronic properties of materials, such as total energy, phase stability, electronic transport, and others. We use the formal construct of multiple-scattering theory to develop the method for the calculation of the two-particle electronic structure of a solid and the corresponding total energy of the ground state. We also illustrate some of the properties of the method in terms of a Hubbard model Hamiltonian on a linear ring. Various features of the method and further possible applications are presented in a discussion section.