4.8 Article

Experimental measurement of the intrinsic excitonic wave function

Journal

SCIENCE ADVANCES
Volume 7, Issue 17, Pages -

Publisher

AMER ASSOC ADVANCEMENT SCIENCE
DOI: 10.1126/sciadv.abg0192

Keywords

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Funding

  1. JSPS Kakenhi [JP17K04995]
  2. Kick-start fund KICKS, Okinawa Institute of Science and Technology Graduate University
  3. Femtosecond Spectroscopy Unit of the Okinawa Institute of Science and Technology Graduate University
  4. NSF through the University of Washington Materials Research Science and Engineering Center [DMR-1719797]
  5. AMOS program, Chemical Sciences, Geosciences, and Biosciences Division, Basic Energy Sciences, U.S. Department of Energy [DE-AC02-76-SF00515]
  6. Micron Foundation
  7. GLAM postdoctoral fellowship at Stanford
  8. state of Washington through the University of Washington Clean Energy Institute
  9. NSF [ACI-1053575]
  10. NSF through the Center for Dynamics and Control of Materials: an NSF MRSEC [DMR-1720595]

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This study directly images the excitonic wave function in reciprocal space, revealing the distribution of electrons within excitons. The experimental results confirm the inverted energy-momentum dispersion relationship of the photoemitted electron, consistent with theoretical predictions.
An exciton, a two-body composite quasiparticle formed of an electron and hole, is a fundamental optical excitation in condensed matter systems. Since its discovery nearly a century ago, a measurement of the excitonic wave function has remained beyond experimental reach. Here, we directly image the excitonic wave function in reciprocal space by measuring the momentum distribution of electrons photoemitted from excitons in monolayer tungsten diselenide. By transforming to real space, we obtain a visual of the distribution of the electron around the hole in an exciton. Further, by also resolving the energy coordinate, we confirm the elusive theoretical prediction that the photoemitted electron exhibits an inverted energy-momentum dispersion relationship reflecting the valence band where the partner hole remains, rather than that of conduction band states of the electron.

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