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Abstract
Selective breaking of degenerate energy levels is a well-known tool for coherent manipulation of spin states. Though most simply achieved with magnetic fields, polarization-sensitive optical methods provide high-speed alternatives. Exploiting the optical selection rules of transition metal dichalcogenide monolayers, the optical Stark effect allows for ultrafast manipulation of valley-coherent excitons. Compared to excitons in these materials, microcavity exciton-polaritons offer a promising alternative for valley manipulation, with longer lifetimes, enhanced valley coherence, and operation across wider temperature ranges. Here, we show valley-selective control of polariton energies in WS2 using the optical Stark effect, extending coherent valley manipulation to the hybrid light-matter regime. Ultrafast pump-probe measurements reveal polariton spectra with strong polarization contrast originating from valley-selective energy shifts. This demonstration of valley degeneracy breaking at picosecond timescales establishes a method for coherent control of valley phenomena in exciton-polaritons.
Microcavity exciton-polaritons in atomically thin semiconductors are a promising platform for valley manipulation. Here, the authors show valley-selective control of polariton energies in monolayer WS2 using the optical Stark effect, thereby extending coherent valley manipulation to a hybrid light-matter regime
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1 Northwestern University, Applied Physics Program, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)
2 Northwestern University, Department of Physics and Astronomy, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)
3 Northwestern University, Department of Chemistry and the Materials Research Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)
4 Northwestern University, Department of Materials Science and Engineering and the Materials Research Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, International Institute of Nanotechnology, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)
5 Northwestern University, Department of Chemistry and the Materials Research Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, Department of Materials Science and Engineering and the Materials Research Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)
6 Northwestern University, Department of Materials Science and Engineering and the Materials Research Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, International Institute of Nanotechnology, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, NUANCE Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)
7 Northwestern University, Applied Physics Program, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, Department of Chemistry and the Materials Research Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, Department of Materials Science and Engineering and the Materials Research Center, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, Department of Electrical and Computer Engineering, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)
8 Northwestern University, Applied Physics Program, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507); Northwestern University, Department of Physics and Astronomy, Evanston, USA (GRID:grid.16753.36) (ISNI:0000 0001 2299 3507)