Observation of exciton polariton condensation in a perovskite lattice at room temperature
Exciton polaritons, with extremely low effective mass1, are regarded as promising candidates to realize Bose–Einstein condensation in lattices for quantum simulations2 towards room-temperature operations3–8. Along with the condensation, an efficient exciton polariton quantum simulator9 would require...
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Main Authors: | , , , , , , |
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Other Authors: | |
Format: | Article |
Language: | English |
Published: |
2020
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Subjects: | |
Online Access: | https://hdl.handle.net/10356/138202 https://doi.org/10.21979/N9/EZLMHJ |
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Institution: | Nanyang Technological University |
Language: | English |
Summary: | Exciton polaritons, with extremely low effective mass1, are regarded as promising candidates to realize Bose–Einstein condensation in lattices for quantum simulations2 towards room-temperature operations3–8. Along with the condensation, an efficient exciton polariton quantum simulator9 would require a strong lattice with robust polariton trapping as well as strong intersite coupling to allow coherent quantum motion of polaritons within the lattice. A strong lattice can be characterized with a larger forbidden bandgap opening and a larger lattice bandwidth compared with the linewidth. However, exciton polaritons in such strong lattices have only been shown to condense at cryogenic temperatures3–8. Here, we report the observation of non-equilibrium exciton polariton condensation in a one-dimensional strong lead halide perovskite lattice at room temperature. Modulated by deep periodic potentials, the strong lead halide perovskite lattice exhibits a large forbidden bandgap opening up to 13.3 meV and a lattice band up to 8.5 meV wide, which are at least 10 times larger than previous systems. Above a critical density, we observe polariton condensation into py orbital states with long-range spatial coherence at room temperature. Our result opens the route to the implementation of polariton condensates in quantum simulators at room temperature. |
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