April 7 - 11, 2025
Seattle, Washington
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2025 MRS Spring Meeting & Exhibit
QT03.01.02

Displacement Field-Controlled Fractional Chern Insulators and Charge Density Waves in a Graphene/hBN Moire Superlattice

When and Where

Apr 8, 2025
11:00am - 11:30am
Summit, Level 4, Room 441

Presenter(s)

Co-Author(s)

Raymond Ashoori1,Samuel Aronson1,Tonghang Han1,Zhengguang Lu1,Kenji Watanabe2,Takashi Taniguchi2,Long Ju1

Massachusetts Institute of Technology1,National Institute for Materials Science2

Abstract

Raymond Ashoori1,Samuel Aronson1,Tonghang Han1,Zhengguang Lu1,Kenji Watanabe2,Takashi Taniguchi2,Long Ju1

Massachusetts Institute of Technology1,National Institute for Materials Science2
The fractional quantum Hall effect is arguably the most well-studied manifestation of the interplay between electronic correlations and non-trivial topology in condensed matter physics. Recent experiments on bilayer MoTe2 and rhombohedral multilayer graphene realized the long-sought fractional quantum anomalous Hall effect (FQAHE) at zero magnetic field. The past year has seen a flurry of experimental and theoretical efforts towards understanding this exotic phenomenon. In bilayer MoTe2, the prerequisite flat Chern bands can be understood at the single-particle level. However, in rhombohedral graphene, electronic correlations themselves produce the topological minibands required for the FQAHE, making this a challenging system to address theoretically. The aim of this work is to explore previously unexplored parameter regimes to pin down the conditions for the observation of topological states as well as to look for new many-body electronic phases.

We focus on five-layer rhombohedral graphene aligned to a layer of hexagonal boron nitride. Due to the lattice mismatch between the two materials, the rhombohedral graphene develops a long-period moiré superlattice potential. The FQAHE appears when electrons are pushed away from the superlattice by an electric field; the majority of studies so far have focused on this moiré-distant limit. In contrast, our work examines the opposite limit, in which the moiré potential is significantly stronger. By tuning the electric and magnetic fields, we can modify the topology and charge order of the correlated phases, revealing a rich phase diagram of delicate symmetry-broken states. Crucially, we observe fractional Chern insulators extending to nearly zero magnetic field with topology that is qualitatively different than in the moiré-distant case, along with a Wigner solid and a series of charge density waves. These are phases that, while seen individually in other moiré platforms, now all occur within close proximity to each other in a single system. Consequently, our work opens the door to further studies of topological phases and their competition via tuning of moiré potential strength in rhombohedral graphene multilayers.

Keywords

Hall effect

Symposium Organizers

Jairo Velasco Jr., University of California, Santa Cruz
Giulia Pacchioni, Springer Nature
Matthew Yankowitz, University of Washington
Long Ju, Massachusetts Institute of Technology

Symposium Support

Gold
Gordon and Betty Moore Foundation

Silver
Bluefors

Bronze
QUANTUM DESIGN
Scienta Omicron, Inc.
Thouless Institute for Quantum Matter

Session Chairs

Long Ju
Giulia Pacchioni

In this Session