We use time-resolved nonlinear pump--probe measurements to reveal features of semiconductor moir\'e materials not accessible to linear spectroscopy. With an intense, red-detuned pump pulse, we generate a high density of virtual excitons or exciton--polarons in various moir\'e minibands. A broadband probe pulse in turn measures the response of all optical resonances induced by the pump-generated excitations. We generically observe a coherent blue shift originating from contact-like exciton--exciton interactions. At charge neutrality, these measurements allow us to assess the spatial overlap between different optical excitations: in particular, we observe signatures of a bound biexciton state between two different moire exciton modes. For integer fillings ν=2 and ν=3 of the moir\'e lattice with electrons, the correlated Mott state results in a suppression of the exciton--polaron interactions, providing a nonlinear optical signature of electronic incompressibility. In stark contrast, for lower electron fillings ν < 2, the light shift of the attractive polaron resonance is electron density independent. Deeply localized moir\'e polarons are thus akin to an ensemble of non-interacting two-level atoms, subject to the single-emitter ac Stark effect. Finally, tuning the pump laser on resonance with the attractive polaron for ν < 2, we demonstrate the filling of the moir\'e lattice with localized polarons and thereby realize a nonequilibrium Bose--Fermi mixture in moir\'e flat bands.
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Evrard et al. (2024) studied this question.
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