4.8 Article

Signatures of Wigner crystal of electrons in a monolayer semiconductor

Journal

NATURE
Volume 595, Issue 7865, Pages 53-+

Publisher

NATURE PORTFOLIO
DOI: 10.1038/s41586-021-03590-4

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The signature of a Wigner crystal in a monolayer transition metal dichalcogenide is observed through optical spectroscopy, demonstrating electron charge order in a system with high electron effective mass and reduced dielectric screening even without moire potential or an external magnetic field. The findings show that charge-tunable transition metal dichalcogenide monolayers open up new territory for many-body physics where interaction energy dominates over kinetic energy.
The signature of a Wigner crystal-the analogue of a solid phase for electrons-is observed via the optical reflection spectrum in a monolayer transition metal dichalcogenide. When the Coulomb repulsion between electrons dominates over their kinetic energy, electrons in two-dimensional systems are predicted to spontaneously break continuous-translation symmetry and form a quantum crystal(1). Efforts to observe(2-12) this elusive state of matter, termed a Wigner crystal, in two-dimensional extended systems have primarily focused on conductivity measurements on electrons confined to a single Landau level at high magnetic fields. Here we use optical spectroscopy to demonstrate that electrons in a monolayer semiconductor with density lower than 3 x 10(11) per centimetre squared form a Wigner crystal. The combination of a high electron effective mass and reduced dielectric screening enables us to observe electronic charge order even in the absence of a moire potential or an external magnetic field. The interactions between a resonantly injected exciton and electrons arranged in a periodic lattice modify the exciton bandstructure so that an umklapp resonance arises in the optical reflection spectrum, heralding the presence of charge order(13). Our findings demonstrate that charge-tunable transition metal dichalcogenide monolayers(14) enable the investigation of previously uncharted territory for many-body physics where interaction energy dominates over kinetic energy.

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