The on-shell self-energy of the uniform electron gas in its weak-correlation limit

Abstract

The ring-diagram partial summation (or RPA) for the ground-state energy of the uniform electron gas (with the density parameter $r_s$) in its weak-correlation limit $r_s\to 0 $ is revisited. It is studied, which treatment of the self-energy $Σ(k,ω)$ is in agreement with the Hugenholtz-van Hove (Luttinger-Ward) theorem $μ-μ_0= Σ(k_{\rm F},μ)$ and which is not. The correlation part of the lhs h as the RPA asymptotics $a\ln r_s +a'+O(r_s)$ [in atomic units]. The use of renormalized RPA diagrams for the rhs yields the similar expression $a\ln r_s+a''+O(r_s)$ with the sum rule $a'= a''$ resulting from three sum rules for the components of $a'$ and $a''$. This includes in the second order of exchange the sum rule $μ_{2{\rm x}}=Σ_{2{\rm x}}$ [P. Ziesche, Ann. Phys. (Leipzig), 2006].