Establishing a non-Fermi liquid theory for disordered metals near two dimensions
arXiv:cond-mat/0106446 · doi:10.1103/PhysRevB.66.075317
Abstract
We consider the finkelstein action describing a system of spin polarized or spinless electrons near two dimensions, in the presence of disorder as well as the Coulomb interactions.We extend the renormalization group analysis of our previous work and evaluate the metal-insulator transition of the electron gas to second order in an (d-2) expansion. We obtain the complete scaling behavior of physical observables like the conductivity and the specific heat with varying frequency, temperature and/or electron density.
arXiv comment19 pages, 3 tables and one figure
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- The effects of macroscopic inhomogeneities on the magneto transport properties of the electron gas in two dimensions
- Quantum critical behaviour of the plateau-insulator transition in the quantum Hall regime
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- New Insights into the Plateau-Insulator Transition in the Quantum Hall Regime
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- Disordered electron liquid in double quantum well heterostructures: Renormalization group analysis and dephasing rate
- Comment on ``Topological Oscillations of the Magnetoconductance in Disordered GaAs Layers''
- Super universality of the quantum Hall effect and the "large picture" of the angle
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- Beta-functions of non-linear -models for disordered and interacting electron systems
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- Emergence of quasi-metallic state in disordered 2D electron gas due to strong interactions
- Quantum phase coherence in non-Markovian and reaction-diffusive transport