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Coexistence of insulating phases in confined fermionic chains with a Wannier-Stark potential

N. Aucar Boidi1,*, K. Hallberg1,2,†, Amnon Aharony3,‡, and Ora Entin-Wohlman3,§

  • 1Centro Atómico Bariloche, Instituto Balseiro, 8400 Bariloche, Argentina
  • 2Instituto de Nanociencia y Nanotecnología CNEA-CONICET, 8400 Bariloche, Argentina
  • 3School of Physics and Astronomy, Tel Aviv University, Tel Aviv 6997801, Israel

  • *nairaucar@gmail.com
  • †karenhallberg@gmail.com
  • ‡aaharonyaa@gmail.com
  • §orawohlman@gmail.com

Phys. Rev. B 109, L041404 – Published 12 January, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L041404

Abstract

We study fermions on a finite chain, interacting repulsively when residing on the same and on nearest-neighbor sites, and subjected to a Wannier-Stark linearly varying potential. Using the density matrix renormalization-group numerical technique to solve this generalized extended Hubbard model, the ground state exhibits a staircase of (quasi) plateaus in the average local site density along the chain, decreasing from being doubly filled to empty as the potential increases. These “plateaus” represent locked-in commensurate phases of charge density waves together with band and Mott insulators. These phases are separated by incompressible regions with incommensurate fillings. These results differ from the many-body localization proposed for this model earlier. It is suggested that experimental variations of the slope of the potential and the range of the repulsive interactions will produce such a coexistence of phases which have been individually expected theoretically and observed experimentally for uniform systems.

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