ANDERSON LOCALIZATION VS. MOTT–HUBBARD METAL–INSULATOR TRANSITION IN DISORDERED, INTERACTING LATTICE FERMION SYSTEMS

DOI10.1142/S0217979210064575zbMath1195.82029arXiv1002.3696OpenAlexW2095834335MaRDI QIDQ4929661

Dieter Vollhardt, Krzysztof Byczuk, Walter Hofstetter

Publication date: 23 September 2010

Published in: International Journal of Modern Physics B (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/1002.3696

Mathematics Subject Classification ID

Disordered systems (random Ising models, random Schrödinger operators, etc.) in equilibrium statistical mechanics (82B44) Phase transitions (general) in equilibrium statistical mechanics (82B26) Lattice systems (Ising, dimer, Potts, etc.) and systems on graphs arising in equilibrium statistical mechanics (82B20) Statistical mechanics of metals (82D35)

Related Items (2)

Dynamical mean-field theory for correlated electrons ⋮ Non-local corrections to the typical medium theory of Anderson localization

Cites Work

• Supersymmetry in Disorder and Chaos

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