“…Classically, this technique is based on the self-interference of an illumination beam passing through the sample over a photographic plate [ 34 ] which is substituted, in modern implementations, by a digital sensor [ 35 , 36 , 37 ]. Additionally, novel experiments have introduced several improvements in image capture and processing stages with approaches based on the introduction of tunable optical devices enhancing the hologram capture, focus distance, and magnifications [ 38 , 39 , 40 , 41 ]. More specifically, in this interferometric arrangement based on a classical Gabor in-line configuration, the reference beam directly comes as the non-diffracted light emanating from a partially coherent illumination source, and the object beam is created from the diffracted light coming from the illuminated sample, which is thus considered small in comparison with the reference beam (weak diffraction assumption).…”