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Thickness and twist angle tunable moiré excitons in InSe/GaSe heterostructures

ORAL

Abstract

Moiré quantum systems have emerged as a materials framework displaying highly tunable electronic, optical and topological properties with an exquisite level of control. To date, the moiré physics has been constrained mainly by two factors i) the dimensionality, defined by the stacking of monolayers, and ii) the twist angle φ, which unveils novel phases only at quite precise values (e.g. superconductivity, orbital magnetism, correlated insulator states). Here, we overcome these practical limitations through a new class of heterostructures composed of γ-InSe on ε-GaSe that reveal strong evidence for the moiré potential even in thick stacked layers and at arbitrary values of φ. We detect a pronounced interlayer exciton composed of several superimposed emissions that are uniformly spaced in energy ΔE with pronounced φ-dependence. In the interfacial area, similar behavior is displayed also by the intralayer exciton of GaSe. This strong correlation between φ and ΔE implies the localization of excitations at the moiré potential minima. But in contrast to transition metal dichalcogenides (TMDs), the moiré potential modulates the multi-component interlayer exciton over the entire range of φ due to their direct band-gap at the center of their Brillouin zone. γ-InSe/ε-GaSe interfaces offer an unprecedented level of moiré exciton tunability not yet achieved in any other van der Waals heterostructure. Our results demonstrate clear pathways for quantum optoelectronics while offering opportunities to study electronic correlations over a broad range of moiré periodicities and layer thicknesses.

Presenters

  • Wenkai Zheng

    National High Magnetic Field Laboratory

Authors

  • Wenkai Zheng

    National High Magnetic Field Laboratory

  • Li Xiang

    Florida State University, Iowa State University

  • Felipe Alexander de A Quesada

    Stanford University, Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory; Department of Materials Science and Engineering, Stanford University

  • Mathias Augustin

    Institute for Condensed Matter Physics and Complex Systems, School of Physics and Astronomy,The University of Edinburgh

  • Zhengguang Lu

    National High Magnetic Field Laboratory

  • Aditya Sood

    Stanford Univ

  • Fengcheng Wu

    Wuhan University, School of Physics and Technology, Wuhan University

  • Dmitry L Shcherbakov

    The Ohio State University, Ohio State Univ - Columbus

  • Shahriar Memaran

    National High Magnetic Field Laboratory

  • Ryan Baumbach

    National High Magnetic Field Laboratory, NHFML; Florida State University, NHMFL; Florida State University

  • Justin B Felder

    Department of Chemistry and Biochemistry, The University of Texas at Dallas

  • Gregory T McCandless

    University of Texas at Dallas, University of Texas - Dallas, Department of Chemistry and Biochemistry, The University of Texas at Dallas

  • Julia Y Chan

    University of Texas at Dallas, Department of Chemistry and Biochemistry, The University of Texas at Dallas

  • Song Liu

    Columbia University, Columbia University, US, Tim Taylor Department of Chemical Engineering, Kansas State University

  • James H Edgar

    Tim Taylor Department of Chemical Engineering, Kansas State University, Kansas State University

  • Chun Ning Lau

    Ohio State Univ - Columbus, The Ohio State University

  • Elton Santos

    Higgs Centre for Theoretical Physics, Institute for Condensed Matter Physics and Complex Systems, School of Physics and Astronomy,The University of Edinburgh

  • Aaron M Lindenberg

    Stanford Univ

  • Dmitry Smirnov

    National High Magnetic Field Laboratory

  • Luis Balicas

    National High Magnetic Field Laboratory