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    First-order quantum Hall to Wigner crystal phase transition on a triangular lattice: An infinite density matrix renormalization group study

    Gleb Fedorovich1,2,*, Clemens Kuhlenkamp1, Atac Imamoglu1, and Ivan Amelio1,3,4

    • 1Institute of Quantum Electronics ETH Zurich, CH-8093 Zurich, Switzerland
    • 2Department of Physics and Astronomy, Ghent University, Krijgslaan 281, 9000 Gent, Belgium
    • 3Center for Nonlinear Phenomena and Complex Systems, Université Libre de Bruxelles, CP 231, Campus Plaine, B-1050 Brussels, Belgium
    • 4International Solvay Institutes, Brussels, Belgium

    • *Contact author: gleb.fedorovich@ugent.be

    Phys. Rev. B 111, 235141 – Published 23 June, 2025

    DOI: https://doi.org/10.1103/66gf-h6nn

    Abstract

    In this work we study a system of interacting fermions on a triangular lattice in the presence of an external magnetic field. We assume electrons are spin polarized and fix a density of one third, with one unit of magnetic flux per particle. The infinite density matrix renormalization group algorithm is used to compute the ground state of this generalized Fermi-Hubbard model. Increasing the strength of the nearest-neighbor repulsion, we find a first-order transition between an integer quantum Hall phase and a crystalline, generalized Wigner crystal state. The first-order nature of the phase transition is consistent with a Ginzburg-Landau argument. We expect our results to be relevant for moiré heterostructures of two-dimensional materials.

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