“…The microscope was equipped with a 50 × objective (PL FLUOTAR L 50x/0.55, Leica, Wetzlar, Germany) and a dichroic mirror (Semrock, Brightline FF389-Di01, Rochester, NY, USA), allowing the analysis of a field of view of 205 × 250 μm 2 , with a spatial sampling pitch of 0.2 μm. The hyperspectral camera was composed of a common path birefringent interferometer (the Translating-Wedge-Based Identical Pulses eNcoding System (TWINS) [49,50]) combined with a cooled monochrome camera (Retiga R6, QImaging, Teledyne Photometrics, Tucson, AZ, USA, spectral range 300-1000 nm); the interferometer supplied high-quality interferograms which provided high-quality spectral images of the PL emission by Fourier transform [51,52]. The spectral resolution of the hyperspectral camera was set by the maximum scan delay introduced by the interferometer and could be as good as 4 nm at 600 nm wavelength.…”