Self-doping instability of the Wigner-Mott insulator
arXiv:0705.3428 · doi:10.1103/PhysRevB.77.085104
Abstract
We present a theory describing the mechanism for the two-dimensional (2D) metal-insulator transition (MIT) in absence of disorder. A two-band Hubbard model is introduced, describing vacancy-interstitial pair excitations within the Wigner crystal. Kinetic energy gained by delocalizing such excitations is found to lead to an instability of the insulator to self-doping above a critical carrier concentration , mapping the problem to a density-driven Mott MIT. This mechanism provides a natural microscopic picture of several puzzling experimental features, including the large effective mass enhancement, the large resistivity drop, and the large positive magneto-resistance on the metallic side of the transition. We also present a global phase diagram for the clean 2D electron gas as a function of and parallel magnetic field , which agrees well with experimental findings in ultra clean samples.
5 pages, 2 figures
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- Metal-insulator transition in the two-dimensional fully polarized homogeneous electron gas from Hartree-Fock solutions
- Quantum critical scaling for finite temperature Mott-like metal-insulator crossover in a few layered-MoS
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- A metal-insulator transition in 2D: Established facts and open questions
- Exact solution of the 1D Hubbard model with NN and NNN interactions in the narrow-band limit
- Exact solution of the 1D Hubbard model in the atomic limit with inter-site magnetic coupling
- Polarization field in a single-valley strongly-interacting 2D electron system
- Particle-Hole Asymmetry and Pinball Liquid in a Triangular-Lattice Extended Hubbard Model within Mean-Field Approximation
- Electronic Crystal Phases in the Presence of Non-Uniform Berry Curvature and Tunable Berry Flux: The -Jellium model
- Defects in Wigner crystals: fracton-elasticity duality and vacancy proliferation