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[Paper Review] Dataset for 'Mapping twist-tuned multi-band topology in bilayer WSe$_2$'

Benjamin A. Foutty, Carlos R. Kometter|arXiv (Cornell University)|Apr 19, 2023
Topological Materials and Phenomena12 references24 citations
TL;DR

Local electronic compressibility measurements reveal multiple topological bands and tunable Chern insulators in twisted bilayer WSe2 near a magic angle, including displacement-field driven topological transitions.

ABSTRACT

Datasets and code for the manuscript 'Mapping twist-tuned multi-band topology in bilayer WSe2.' See 'README.txt' for further details.

Motivation & Objective

  • Map topological bands and correlated ground states in twisted bilayer WSe2 at small twist angles.
  • Identify Chern insulators near a magic angle around 1.23° at zero magnetic field.
  • Explore displacement-field induced topological phase transitions at nu = -1.
  • Examine how ground states depend on local moiré wavelength by varying twist angle.
  • Establish the topological phase diagram of a generalized Kane-Mele-Hubbard model in tWSe2.

Proposed method

  • Use scanning single electron transistor (SET) microscopy to measure inverse compressibility dμ/dn and chemical potential μ(n).
  • Vary twist angle locally from 1.1° to 1.6° to map moiré wavelength effects.
  • Apply a locally controlled displacement field D_eff via the SET tip to tune topology and induce phase transitions.
  • Compare measurements with Hartree-Fock continuum-model predictions for Kane-Mele-Hubbard–like physics.
  • Study magnetic-field dependent spectra up to B ≈ 11 T to observe Hofstadter-like features.
Figure 1: Multiple topological bands and ground states in tWSe 2 . a , Schematic showing the moiré pattern in twisted WSe 2 (tWSe 2 ), in which MX and XM stacking sites (bottom illustrations) form a honeycomb lattice. b , Cartoon of lowest energy moiré bands and their occupations at the first four i
Figure 1: Multiple topological bands and ground states in tWSe 2 . a , Schematic showing the moiré pattern in twisted WSe 2 (tWSe 2 ), in which MX and XM stacking sites (bottom illustrations) form a honeycomb lattice. b , Cartoon of lowest energy moiré bands and their occupations at the first four i

Experimental results

Research questions

  • RQ1Do twisted WSe2 bilayers host multiple topological bands with nonzero Chern numbers at small twist angles?
  • RQ2How does moiré wavelength affect correlated ground states and gaps at integer fillings?
  • RQ3Can displacement-field tuning drive topological phase transitions at integer fillings such as ν = -1?
  • RQ4What is the magnetic-field dependence of the gaps and Hofstadter states in these systems?

Key findings

  • Multiple topological bands with Chern number C = +1 gaps observed at ν = -1 and ν = -3 that persist to zero magnetic field.
  • Gaps at ν = -1 and ν = -3 have total Chern number C = +1, while ν = -2 and ν = -4 have C = 0, indicating distinct topological ground states.
  • At a local twist angle around 1.23°, a series of quantum anomalous Hall (QAH) insulators is observed at zero field.
  • Displacement-field tuning via the SET tip induces a topological phase transition at ν = -1 between a QAH state and a topologically trivial layer-polarized state.
  • Twist-angle dependence shows topological gaps appear only in a narrow range (≈1.2°–1.25°), with broader angles yielding weaker or no zero-field topological states.
  • Hartree-Fock continuum-model calculations support a landscape with spin-valley polarized Chern insulators and transitions to trivial states under varying D and θ.
Figure 2: Magnetic field dependence at $\theta=1.23^{\circ}$ . a Magnetic field dependence of d $\mu$ /d $n$ up to $B=11$ T. b , Thermodynamic gaps $\Delta_{(C,s)}$ for states with intercept $s$ and slope $C$ as identified by the Diophantine equation, as a function of $B$ , for the pair of competing
Figure 2: Magnetic field dependence at $\theta=1.23^{\circ}$ . a Magnetic field dependence of d $\mu$ /d $n$ up to $B=11$ T. b , Thermodynamic gaps $\Delta_{(C,s)}$ for states with intercept $s$ and slope $C$ as identified by the Diophantine equation, as a function of $B$ , for the pair of competing

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This review was created by AI and reviewed by human editors.