A unified description of static and dynamic properties of Fermi liquids
arXiv:cond-mat/9901100 · doi:10.1142/S0217979200000376
Abstract
In Landau's phenomenological Fermi-liquid theory (FLT), most physical quantities are derived from the knowledge of the energy variation corresponding to a change of the quasi-particle (QP) distribution function . We show that the internal energy (or, more precisely, the thermodynamic potential ), expressed as a function of the QP distribution , can be interpreted as an effective potential (in the sense of field theory), which is obtained from the free energy by a Legendre transformation. This allows to obtain explicitly (or ) starting from a microscopic Hamiltonian and to relate the Landau function to the forward-scattering two-particle vertex without considering the collective modes as in the standard diagrammatic derivation of FLT. Out-of-equilibrium properties are obtained by extending the definition of the effective potential to space- and time-dependent configurations. is then a functional of the Wigner distribution function . It contains information about both the static and dynamic properties of the Fermi liquid. In particular, it yields the quantum Boltzmann equation satisfied by . Finally, we show how can be derived (in the static case) using a finite-temperature renormalization-group approach. In agreement with previous results based on this technique, we find that the Landau function is defined by the fixed-point value of the -limit of the forward-scattering two-particle vertex.
13 pages, RevTex, no figures