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Orbital-Selective Mott Transition out of Band Degeneracy Lifting

2008/08/31 by Luca de' Medici, Luca de’ Medici, S. R. Hassan +2 · 271 citations
Materials Science · Physics and Astronomy · #Condensed matter physics #Coupling (piping) #Degeneracy (biology) #Electron #Hubbard model #Iron-based superconductors research #Kinetic energy #Materials science #Mott transition #Phase transition #Physics #Physics of Superconductivity and Magnetism #Quantum mechanics #Rare-earth and actinide compounds #Superconductivity #cond-mat.str-el #cond-mat.supr-con

paper · pdf · doi:10.1103/physrevlett.102.126401

published in Physical Review Letters 102(12), 126401 (American Physical Society) · Published version

openalex publication_date 2009/03/23 · arxiv created 2009/03/24 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05

Abstract

We outline a general mechanism for orbital-selective Mott transition, the coexistence of both itinerant and localized conduction electrons, and show how it can take place in a wide range of realistic situations, even for bands of identical width and correlation, provided a crystal field splits the energy levels in manifolds with different degeneracies and the exchange coupling is large enough to reduce orbital fluctuations. The mechanism relies on the different kinetic energy in manifolds with different degeneracy. This phase has Curie-Weiss susceptibility and non-Fermi-liquid behavior, which disappear at a critical doping, all of which is reminiscent of the physics of the pnictides.

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