Physical and unphysical regimes of self-consistent many-body perturbation theory
Kris Van Houcke, Evgeny Kozik, Riccardo Rossi, Youjin Deng, Félix Werner
SciPost Phys. 16, 133 (2024) · published 27 May 2024
- doi: 10.21468/SciPostPhys.16.5.133
- Submissions/Reports
Abstract
In the standard framework of self-consistent many-body perturbation theory, the skeleton series for the self-energy is truncated at a finite order N and plugged into the Dyson equation, which is then solved for the propagator $G_N$. We consider two examples of fermionic models, the Hubbard atom at half filling and its zero space-time dimensional simplified version. First, we show that $G_N$ converges when $N\to∞$ to a limit $G_∞\,$, which coincides with the exact physical propagator $G_{exact}$ at small enough coupling, while $G_∞ ≠ G_{exact}$ at strong coupling. This follows from the findings of [Phys. Rev. Lett. 114, 156402 (2015)] and an additional subtle mathematical mechanism elucidated here. Second, we demonstrate that it is possible to discriminate between the $G_∞=G_{exact}$ and $G_∞≠G_{exact}$ regimes thanks to a criterion which does not require the knowledge of $G_{exact}$, as proposed in [Phys. Rev. B 93, 161102 (2016)].
Cited by 1
Authors / Affiliations: mappings to Contributors and Organizations
See all Organizations.- 1 Kris Van Houcke,
- 2 Evgeny Kozik,
- 1 3 4 5 Riccardo Rossi,
- 6 Youjin Deng,
- 7 Félix Werner
- 1 Laboratoire de Physique de l’École Normale Supérieure / Physics Laboratory of the École Normale Supérieure [LPENS]
- 2 King's College London [KCL]
- 3 Sorbonne Université / Sorbonne University
- 4 École Polytechnique Fédérale de Lausanne [EPFL]
- 5 Flatiron Institute
- 6 中国科学技术大学 / University of Science and Technology of China [USTC]
- 7 Laboratoire Kastler Brossel / Kastler-Brossel Laboratory [LKB]