Convexity of the self-energy functional in the variational cluster approximation
Andriy H. Nevidomskyy, David S\'en\'echal, A.-M.S. Tremblay

TL;DR
This paper addresses the non-convexity issue in the variational cluster approximation for the Hubbard model by proposing two methods to construct convex self-energy functionals, enabling more efficient solution algorithms.
Contribution
It introduces two approaches to create convex self-energy functionals in VCA, improving the stability and efficiency of finding physical solutions.
Findings
Convexity can hinder the detection of instabilities in certain channels.
A phenomenological functional enforces convexity on selected variables.
The new functional allows second-order phase transitions, facilitating better numerical analysis.
Abstract
In the variational cluster approximation (VCA) (or variational cluster perturbation theory), widely used to study the Hubbard model, a fundamental problem that renders variational solutions difficult in practice is its known lack of convexity at stationary points, i.e. the physical solutions can be saddle points rather than extrema of the self-energy functional. Here we suggest two different approaches to construct a convex functional of the self-energy. In the first approach, one can show analytically that in the approximation where the irreducible particle-hole vertex depends only on center of mass coordinates, the functional is convex away from phase transitions in the corresponding channel. Numerical tests on a tractable version of that functional show that convexity can be a nuisance when looking for instabilities both in the pairing and particle-hole channels. Therefore, an…
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