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Emergence of composite many-body exciton states in WS2 and MoSe2 monolayers

J. Choi1,2, J. Li1,3, D. Van Tuan4, H. Dery4,5, and S. A. Crooker1

  • 1National High Magnetic Field Laboratory, Los Alamos, New Mexico 87545, USA
  • 2Advanced Instrumentation Institute, Korea Research Institute of Standards and Science, Daejeon 34113, Korea
  • 3Wuhan National High Magnetic Field Center and School of Physics, Huazhong University of Science and Technology, Hubei 430074, China
  • 4Department of Electrical and Computer Engineering, University of Rochester, Rochester, New York 14627, USA
  • 5Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA

Phys. Rev. B 109, L041304 – Published 30 January, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L041304

Abstract

When doped with a high density of mobile charge carriers, monolayer transition-metal dichalcogenide (TMD) semiconductors can host new types of composite many-particle exciton states that do not exist in conventional semiconductors. Such multiparticle bound states arise when a photoexcited electron-hole pair couples not to just a single Fermi sea that is quantum-mechanically distinguishable (as in the case of conventional charged excitons or trions), but rather couples simultaneously to multiple Fermi seas, each having distinct spin and valley quantum numbers. Composite six-particle “hexciton” states were recently identified in electron-doped WSe2 monolayers, but under suitable conditions they should also form in all other members of the monolayer TMD family. Here we present spectroscopic evidence demonstrating the emergence of many-body hexcitons in charge-tunable WS2 monolayers (at the A-exciton) and MoSe2 monolayers (at the B-exciton). The roles of distinguishability and carrier screening on the stability of hexcitons are discussed.

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