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. 2020 Dec 1;11:6154. doi: 10.1038/s41467-020-19696-8

Fig. 3. Imaging through scattering media using back-scattered fluorescence and finite memory effect.

Fig. 3

a Images recorded on the control camera when the illumination is focused on two different beads of an extended object represented in f, where the scattering medium is made by two surface diffusers separated by 0.78 mm. We define u12 as the relative displacement between the two foci (i.e. beads). b If the two beads are within the same ME patch their two fluorescent patterns, #1 and #2, are spatially shifted by u12. c u12 is estimated from cross-correlation #1⋆#2. d This operation is repeated between #1 all the other eigen-patterns #j with j=1, …, 13. If bead #j is within the ME patch of #1, indicated by the dashed circle, a peak of correlation appears and a sub-part of the object is retrieved. e To obtain the full extended object, the reconstruction is done as in d for all the ME patches. The result is in good agreement with the ground truth (f) which is a fluorescence image recorded without scattering medium. P = 14,336 − Acq. speed = 20 Hz − NSLM = 1024.