Exact integral equation for the renormalized Fermi surface
arXiv:cond-mat/0208517 · doi:10.1088/0953-8984/15/27/309
Abstract
The true Fermi surface of a fermionic many-body system can be viewed as a fixed point manifold of the renormalization group (RG). Within the framework of the exact functional RG we show that the fixed point condition implies an exact integral equation for the counterterm which is needed for a self-consistent calculation of the Fermi surface. In the simplest approximation, our integral equation reduces to the self-consistent Hartree-Fock equation for the counterterm.
5 pages, 1 figure
Cited by in corpus (11)
- Functional renormalization group approach to correlated fermion systems
- Collective fields in the functional renormalization group for fermions, Ward identities, and the exact solution of the Tomonaga-Luttinger model
- Self-energy and critical temperature of weakly interacting bosons
- Renormalization group approach to interacting fermion systems in the two-particle-irreducible formalism
- Critical behavior of weakly interacting bosons: A functional renormalization group approach
- Dynamic structure factor of Luttinger liquids with quadratic energy dispersion and long-range interactions
- Fermi surface renormalization and confinement in two coupled metallic chains
- Self-energy corrections to anisotropic Fermi surfaces
- Confined coherence in quasi-one-dimensional metals
- Deformation of anisotropic Fermi surfaces due to electron-electron interactions
- Electronic instabilities of a Hubbard model approached as a large array of coupled chains: competition between d-wave superconductivity and pseudogap phase