Effective Soft-Mode Theory of Strongly Interacting Fermions
arXiv:1112.5916 · doi:10.1103/PhysRevB.85.125126
Abstract
An effective field theory for clean electron systems is developed in analogy to the generalized nonlinear sigma-model for disordered interacting electrons. The physical goal is to separate the soft or massless electronic degrees of freedom from the massive ones and integrate out the latter to obtain a field theory in terms of the soft degrees of freedom only. The resulting theory is not perturbative with respect to the electron-electron interaction. It is controlled by means of a systematic loop expansion and allows for a renormalization-group analysis in a natural way. It is applicable to universal phenomena within phases, and to transitions between phases, with order parameters in arbitrary angular-momentum channels, and in the spin-singlet, spin-triplet, particle-hole, and particle-particle channels. Applications include ferromagnetic and ferrimagnetic ordering, non-s-wave ferromagnetic order (magnetic nematics), Fermi-liquid to non-Fermi-liquid transitions, and universal phenomena within a Fermi-liquid phase.
28pp, 5 figs; version corrects typos and other minor mistakes, adds references
References in corpus (4)
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- Soft modes in Fermi liquids at arbitrary temperatures
- Fluctuating Quantum Kinetic Theory
- Soft Modes and Nonanalyticities in a Clean Dirac Metal
- An emerging global picture of heavy fermion physics
- Magnetic Quantum Phase Transitions in a Clean Dirac Metal
- The quantum ferromagnetic transition in a clean Kondo lattice is discontinuous
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- Scaling Theory of a Compressibility-Driven Metal-Insulator Transition in a Two-Dimensional Electron Fluid
- Quantum Correlations in Metals that Grow in Time and Space
- Anomalous Density-of-States Fluctuations in Two-Dimensional Clean Metals
- Work probability distribution for a ferromagnet with long-ranged and short-ranged correlations