When Could Abelian Fractional Topological Insulators Exist in Twisted MoTe$_2$ (and Other Systems)

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Hauptverfasser: Kwan, Yves H., Wagner, Glenn, Yu, Jiabin, Dagnino, Andrea Kouta, Jiang, Yi, Xu, Xiaodong, Bernevig, B. Andrei, Neupert, Titus, Regnault, Nicolas
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Veröffentlicht: 2024
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author Kwan, Yves H.
Wagner, Glenn
Yu, Jiabin
Dagnino, Andrea Kouta
Jiang, Yi
Xu, Xiaodong
Bernevig, B. Andrei
Neupert, Titus
Regnault, Nicolas
author_facet Kwan, Yves H.
Wagner, Glenn
Yu, Jiabin
Dagnino, Andrea Kouta
Jiang, Yi
Xu, Xiaodong
Bernevig, B. Andrei
Neupert, Titus
Regnault, Nicolas
contents Using comprehensive exact diagonalization calculations on $θ\approx 3.7 ^{\circ}$ twisted bilayer MoTe$_2$ ($t$MoTe$_2$), as well as idealized Landau level models also relevant for lower $θ$, we extract general principles for engineering fractional topological insulators (FTIs) in realistic situations. First, in a Landau level setup at $ν=1/3+1/3$, we investigate what features of the interaction destroy an FTI. For both pseudopotential interactions and realistic screened Coulomb interactions, we find that sufficient suppression of the short-range repulsion is needed for stabilizing an FTI. We then study $θ\approx 3.7 ^{\circ}$ $t$MoTe$_2$ with realistic band-mixing and anisotropic non-local dielectric screening. Our finite-size calculations only find an FTI phase at $ν=-4/3$ in the presence of a significant additional short-range attraction $g$ that acts to counter the Coulomb repulsion at short distances. We discuss how further finite-size drifts, dielectric engineering, Landau level character, and band-mixing effects may reduce the required value of $g$ closer towards the experimentally relevant conditions of $t$MoTe$_2$. Projective calculations into the $n=1$ Landau level, which resembles the second valence band of $θ\simeq 2.1^\circ$ $t$MoTe$_2$, do not yield FTIs for any $g$, suggesting that FTIs at low-angle $t$MoTe$_2$ for $ν=-8/3$ and $-10/3$ may be unlikely. While our study highlights the challenges, at least for the fillings considered, to obtaining an FTI with transport plateaus, even in large-angle $t$MoTe$_2$ where fractional Chern insulators are experimentally established, we also provide potential sample-engineering routes to improve the stability of FTI phases.
format Preprint
id arxiv_https___arxiv_org_abs_2407_02560
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle When Could Abelian Fractional Topological Insulators Exist in Twisted MoTe$_2$ (and Other Systems)
Kwan, Yves H.
Wagner, Glenn
Yu, Jiabin
Dagnino, Andrea Kouta
Jiang, Yi
Xu, Xiaodong
Bernevig, B. Andrei
Neupert, Titus
Regnault, Nicolas
Strongly Correlated Electrons
Mesoscale and Nanoscale Physics
Using comprehensive exact diagonalization calculations on $θ\approx 3.7 ^{\circ}$ twisted bilayer MoTe$_2$ ($t$MoTe$_2$), as well as idealized Landau level models also relevant for lower $θ$, we extract general principles for engineering fractional topological insulators (FTIs) in realistic situations. First, in a Landau level setup at $ν=1/3+1/3$, we investigate what features of the interaction destroy an FTI. For both pseudopotential interactions and realistic screened Coulomb interactions, we find that sufficient suppression of the short-range repulsion is needed for stabilizing an FTI. We then study $θ\approx 3.7 ^{\circ}$ $t$MoTe$_2$ with realistic band-mixing and anisotropic non-local dielectric screening. Our finite-size calculations only find an FTI phase at $ν=-4/3$ in the presence of a significant additional short-range attraction $g$ that acts to counter the Coulomb repulsion at short distances. We discuss how further finite-size drifts, dielectric engineering, Landau level character, and band-mixing effects may reduce the required value of $g$ closer towards the experimentally relevant conditions of $t$MoTe$_2$. Projective calculations into the $n=1$ Landau level, which resembles the second valence band of $θ\simeq 2.1^\circ$ $t$MoTe$_2$, do not yield FTIs for any $g$, suggesting that FTIs at low-angle $t$MoTe$_2$ for $ν=-8/3$ and $-10/3$ may be unlikely. While our study highlights the challenges, at least for the fillings considered, to obtaining an FTI with transport plateaus, even in large-angle $t$MoTe$_2$ where fractional Chern insulators are experimentally established, we also provide potential sample-engineering routes to improve the stability of FTI phases.
title When Could Abelian Fractional Topological Insulators Exist in Twisted MoTe$_2$ (and Other Systems)
topic Strongly Correlated Electrons
Mesoscale and Nanoscale Physics
url https://arxiv.org/abs/2407.02560