Time-domain signatures of distinct correlated insulators in a moiré superlattice

Eric A. Arsenault, Yiliu Li, Birui Yang, Takashi Taniguchi, Kenji Watanabe, James C. Hone, Cory R. Dean, Xiaodong Xu and X.-Y. Zhu ()
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Eric A. Arsenault: Columbia University
Yiliu Li: Columbia University
Birui Yang: Columbia University
Takashi Taniguchi: National Institute for Materials Science
Kenji Watanabe: National Institute for Materials Science
James C. Hone: Columbia University
Cory R. Dean: Columbia University
Xiaodong Xu: University of Washington
X.-Y. Zhu: Columbia University

Nature Communications, 2025, vol. 16, issue 1, 1-8

Abstract: Abstract Among expanding discoveries of quantum phases in moiré superlattices, correlated insulators stand out as both the most stable and most commonly observed. Despite the central importance of these states in moiré physics, little is known about their underlying nature. Here, we use pump-probe spectroscopy to show distinct time-domain signatures of correlated insulators at fillings of one (ν = −1) and two (ν = −2) holes per moiré unit cell in the angle-aligned WSe2/WS2 system. Following photo-doping, we find that the disordering time of the ν = −1 state is independent of excitation density (nex), as expected from the characteristic phonon response time associated with a polaronic state. In contrast, the disordering time of the ν = −2 state scales with $$1/\sqrt{{{{\boldsymbol{n}}}}_{{\mbox{ex}}}}$$ 1 / n ex , in agreement with plasmonic screening from free holons and doublons. These states display disparate reordering behavior dominated either by first order (ν = −1) or second order (ν = −2) recombination, suggesting the presence of Hubbard excitons and free carrier-like holons/doublons, respectively. Our work delineates the roles of electron–phonon (e–ph) versus electron–electron (e–e) interactions in correlated insulators on the moiré landscape and establishes non-equilibrium responses as mechanistic signatures for distinguishing and discovering quantum phases.

Date: 2025
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DOI: 10.1038/s41467-024-54886-8

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