Dynamical Breakup of the Fermi Surface in a doped Mott Insulator
arXiv:cond-mat/0411696 · doi:10.1103/PhysRevLett.95.106402
Abstract
The evolution from an anomalous metallic phase to a Mott insulator within the two-dimensional Hubbard model is investigated by means of the Cellular Dynamical Mean-Field Theory. We show that the density-driven Mott metal-insulator transition is approached in a non-uniform way in different regions of the momentum space. This gives rise to a breakup of the Fermi surface and to the formation of hot and cold regions, whose position depends on the hole or electron like nature of the carriers in the system.
arXiv comment5 pages, 5 figures
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