Correlated fractional Dirac materials

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-dimensiona...

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Main Authors: Bitan Roy, Vladimir Juričić
Format: Article
Language:English
Published: American Physical Society 2023-07-01
Series:Physical Review Research
Online Access:http://doi.org/10.1103/PhysRevResearch.5.L032002
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author Bitan Roy
Vladimir Juričić
author_facet Bitan Roy
Vladimir Juričić
author_sort Bitan Roy
collection DOAJ
description 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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spelling doaj.art-ca8ad0cfe6a443e1aecb11cb62a08e332024-04-12T17:32:20ZengAmerican Physical SocietyPhysical Review Research2643-15642023-07-0153L03200210.1103/PhysRevResearch.5.L032002Correlated fractional Dirac materialsBitan RoyVladimir JuričićFractional 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.http://doi.org/10.1103/PhysRevResearch.5.L032002
spellingShingle Bitan Roy
Vladimir Juričić
Correlated fractional Dirac materials
Physical Review Research
title Correlated fractional Dirac materials
title_full Correlated fractional Dirac materials
title_fullStr Correlated fractional Dirac materials
title_full_unstemmed Correlated fractional Dirac materials
title_short Correlated fractional Dirac materials
title_sort correlated fractional dirac materials
url http://doi.org/10.1103/PhysRevResearch.5.L032002
work_keys_str_mv AT bitanroy correlatedfractionaldiracmaterials
AT vladimirjuricic correlatedfractionaldiracmaterials