Bosonization of Fermi liquids in a weak magnetic field
Daniel G. Barci, Eduardo Fradkin, Leonardo Ribeiro

TL;DR
This paper extends two-dimensional bosonization techniques to Fermi liquids in a weak magnetic field, enabling non-perturbative analysis of quantum oscillations and collective modes in strongly correlated electronic systems.
Contribution
It introduces a covariant Schwinger algebra for particle-hole fluctuations and develops a bosonization formalism for Fermi liquids under a weak magnetic field, including interactions.
Findings
Derivation of a covariant Schwinger algebra for particle-hole fluctuations.
Reproduction of de Haas-van Alphen oscillations and Lifshitz-Kosevich theory.
Oscillatory corrections to Landau zero sound mode due to interactions.
Abstract
Novel controlled non-perturbative techniques are a must in the study of strongly correlated systems, especially near quantum criticality. One of these techniques, bosonization, has been extensively used to understand one-dimensional, as well as higher dimensional electronic systems at finite density. In this paper, we generalize the theory of two-dimensional bosonization of Fermi liquids, in the presence of a homogeneous weak magnetic field perpendicular to the plane. Here, we extend the formalism of bosonization to treat free spinless fermions at finite density in a uniform magnetic field. We show that particle-hole fluctuations of a Fermi surface satisfy a {\em covariant Schwinger algebra}, allowing to express a fermionic theory with forward scattering interactions as a quadratic bosonic theory representing the quantum fluctuations of the Fermi surface. By means of a coherent-state…
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