Theory of Disordered Itinerant Ferromagnets II: Metal-Insulator Transition
arXiv:cond-mat/9912478 · doi:10.1103/PhysRevB.62.966
Abstract
The theory for disordered itinerant ferromagnets developed in a previous paper is used to construct a simple effective field theory that is capable of describing the quantum phase transition from a ferromagnetic metal to a ferromagnetic insulator. It is shown that this transition is in the same universality class as the one from a paramagnetic metal to a paramagnetic insulator in the presence of an external magnetic field, and that strong corrections to scaling exist in this universality class. The experimental consequences of these results are discussed.
12pp., REVTeX, 1 ps and 2 eps figs, final version as published
References in corpus (1)
Cited by in corpus (7)
- Metallic behavior and related phenomena in two dimensions
- Ferromagnetism and Metal-Insulator Transition in the Disordered Hubbard Model
- Theory of Disordered Itinerant Ferromagnets I: Metallic Phase
- Non-perturbative saddle point for the effective action of disordered and interacting electrons in 2D
- The Parallel Magnetoconductance of Interacting Electrons in a Two Dimensional Disordered System
- Transport properties of clean and disordered superconductors in matrix field theory
- Quantum Altermagnetic Instability in Disordered Metals