Derivative Discontinuity in Many-Body Perturbation Theory and Chemical Potentials in Random Phase Approximation
Abstract
We derive analytical expressions for chemical potentials within the random phase approximation (RPA), equivalently the $GW$ energy functional evaluated using non interacting Green's functions ($G_s$). The chemical potential is obtained using two formally equivalent approaches: a direct derivative of the total energy with respect to particle number, and a functional derivative via the chain rule through $G_s$, both validated with finite difference benchmarks. We show that the functional derivativ...
Description / Details
We derive analytical expressions for chemical potentials within the random phase approximation (RPA), equivalently the energy functional evaluated using non interacting Green's functions (). The chemical potential is obtained using two formally equivalent approaches: a direct derivative of the total energy with respect to particle number, and a functional derivative via the chain rule through , both validated with finite difference benchmarks. We show that the functional derivative of the correlation energyi.e., the correlation self energyexhibits a discontinuity at integer particle numbers with finite jumps. This resolves the apparent inconsistency between accurate quasiparticle energies and the large delocalization errors observed in RPA total energies, as standard self energies neglect this nonanalytic behavior. Our results suggest that derivative discontinuities are a fundamental feature of correlation energy functionals, analogous to the known discontinuity in the exact exchange correlation energy.
Source: arXiv:2603.19112v1 - http://arxiv.org/abs/2603.19112v1 PDF: https://arxiv.org/pdf/2603.19112v1 Original Link: http://arxiv.org/abs/2603.19112v1
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Mar 20, 2026
Chemistry
Chemistry
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