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  • Letter
  • Open Access

Correlated fractional Dirac materials

Bitan Roy1,* and Vladimir Juričić2,3,†

  • 1Department of Physics, Lehigh University, Bethlehem, Pennsylvania 18015, USA
  • 2Departamento de Física, Universidad Técnica Federico Santa María, Casilla 110, Valparaíso, Chile
  • 3Nordita, KTH Royal Institute of Technology and Stockholm University, Hannes Alfvéns väg 12, 106 91 Stockholm, Sweden

  • *bitan.roy@lehigh.edu
  • †vladimir.juricic@su.se

Phys. Rev. Research 5, L032002 – Published 10 July, 2023

DOI: https://doi.org/10.1103/PhysRevResearch.5.L032002

Abstract

Fractional Dirac materials (FDMs) feature a fractional energy-momentum relation E(k)∼|k|α, where α(<1) is a real noninteger number, in contrast to that in conventional Dirac materials with α=1. Here we analyze the effects of short- and long-range Coulomb repulsions in two- and three-dimensional FDMs. Only a strong short-range interaction causes nucleation of a correlated insulator that takes place through a quantum critical point. The universality class of the associated quantum phase transition is determined by the correlation length exponent ν−1=d−α and dynamic scaling exponent z=α, set by the band curvature. On the other hand, the fractional dispersion is protected against long-range interaction due to its nonanalytic structure. Rather, a linear Dirac dispersion gets generated under coarse graining, and the associated Fermi velocity increases logarithmically in the infrared regime, thereby yielding a two-fluid system. Altogether, correlated FDMs unfold a rich landscape accommodating unconventional emergent many-body phenomena.

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