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  • Fig1c.xlsx: RC spectrum of encapsulated MoS2 bilayer at low temperature
  • Fig1e.xlsx: RC spectra of excitons in BL MoS2 detected in two circular polarizations in an out-of-plane magnetic field of 8 T at T = 4 K
  • Fig2b.xlsx: Low temperature (4K) RC spectra measured as a function of the cavity-exciton detuning (∆ = Ecav−Eexc) for cavity scans across XA energy
  • Fig2c.xlsx: Low temperature (4K) RC spectra measured as a function of the cavity-exciton detuning (∆ = Ecav−Eexc) for cavity scans across hIX energy
  • Fig2d.xlsx: Waterfall plot of RC spectra measured for the cavity-exciton detunings in the vicinity of the anticrossing between hIX and the cavity mode.
  • Fig2e.xlsx: Dipolariton dispersion measured with circularly polarized detection for 8 T magnetic field
  • Fig2f.xlsx: RC spectra at 8 T at the hIX-cavity anticrossing measured with circularly polarized detection
  • Fig3a.xlsx: RC spectra measured with the NB (FWHM=28 nm) excitation for the XA at different fluences
  • Fig3b.xlsx: RC spectra measured with the NB (FWHM=28 nm) excitation for the hIX at different fluences
  • Fig3c.xlsx: RC spectra measured with the BB (FWHM=50 nm) excitation at different fluences
  • Fig3d.xlsx: The energy shift ∆E (top) and normalized integrated intensity (bottom) as a function of the exciton density for the hIX (first worksheet) and XA (second worksheet)
  • Fig4a.xlsx: Reflectance contrast dispersion spectra of the MoS2 bilayer placed in a monolithic cavity. The low fluence case (0.6 µJ cm−2)
  • Fig4b.xlsx: Reflectance contrast dispersion spectra of the MoS2 bilayer placed in a monolithic cavity. The high fluence case (58.5 µJ cm−2 )
  • Fig4c.xlsx: RC spectra measured at the anticrossing as a function of the laser fluence
  • Fig4de.xlsx: Measured UPB , LPB peak energies and normalised Rabi splitting as a function of the laser fluence and the corresponding polariton density. Rabi splittings are normalised by the Rabi splitting obtained at the lowest fluence.