<p>Excitons, Coulomb-driven bound states of electrons and holes, are typically composed of integer charges<sup><CitationRef CitationID="CR1">1</CitationRef>,<CitationRef CitationID="CR2">2</CitationRef></sup>. However, in bilayer systems influenced by charge fractionalization<sup><CitationRef CitationID="CR3">3</CitationRef>,<CitationRef CitationID="CR4">4</CitationRef></sup>, a more interesting form of interlayer exciton can emerge, in which pairing occurs between constituents that carry fractional charges. Despite numerous theoretical predictions for these fractional excitons<sup><CitationRef AdditionalCitationIDS="CR6 CR7 CR8 CR9 CR10 CR11 CR12 CR13 CR14 CR15" CitationID="CR5">5</CitationRef>–<CitationRef CitationID="CR16">16</CitationRef></sup>, their experimental observation has remained unexplored. Here we report transport signatures of excitonic pairing in fractional quantum Hall effect states. By probing the composition of these excitons and their impact on the underlying wavefunction, we discover two new types of quantum phases of matter. One of these can be viewed as the fractional counterpart of the exciton condensate at a total filling of 1, whereas the other involves a more unusual type of exciton that obeys non-bosonic quantum statistics, challenging the standard model of bosonic excitons.</p>

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Excitons in the fractional quantum Hall effect

  • Naiyuan J. Zhang,
  • Ron Q. Nguyen,
  • Navketan Batra,
  • Xiaoxue Liu,
  • Kenji Watanabe,
  • Takashi Taniguchi,
  • D. E. Feldman,
  • J. I. A. Li

摘要

Excitons, Coulomb-driven bound states of electrons and holes, are typically composed of integer charges1,2. However, in bilayer systems influenced by charge fractionalization3,4, a more interesting form of interlayer exciton can emerge, in which pairing occurs between constituents that carry fractional charges. Despite numerous theoretical predictions for these fractional excitons516, their experimental observation has remained unexplored. Here we report transport signatures of excitonic pairing in fractional quantum Hall effect states. By probing the composition of these excitons and their impact on the underlying wavefunction, we discover two new types of quantum phases of matter. One of these can be viewed as the fractional counterpart of the exciton condensate at a total filling of 1, whereas the other involves a more unusual type of exciton that obeys non-bosonic quantum statistics, challenging the standard model of bosonic excitons.