Zero-temperature limit and statistical quasiparticles in many-body perturbation theory
arXiv:1804.03040 · doi:10.1103/PhysRevC.99.065811
Abstract
The order-by-order renormalization of the self-consistent mean-field potential in many-body perturbation theory for normal Fermi systems is investigated in detail. Building on previous work mainly by Balian and de Dominicis, as a key result we derive a thermodynamic perturbation series that manifests the consistency of the adiabatic zero-temperature formalism with perturbative statistical mechanics---for both isotropic and anisotropic systems---and satisfies at each order and for all temperatures the thermodynamic relations associated with Fermiliquid theory. These properties are proved to all orders.
minor improvements, matches published version; 29 pages, 8 figures
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- Nuclear equation of state for arbitrary proton fraction and temperature based on chiral effective field theory and a Gaussian process emulator
- Neutron matter at finite temperature based on chiral effective field theory interactions
- Effective field theory for dilute Fermi systems at fourth order
- From weak to strong: constrained extrapolation of perturbation series with applications to dilute Fermi systems
- Constrained extrapolation problem and order-dependent mappings