“…More recently, the basic imaging configuration has settled to scanning a large 2D grid of points on a planar Lambertian wall, with emphasis on developing ever faster and more accurate reconstruction algorithms, including improved methods of filtering for back-projection 8,9 , fast Fourier transform-based methods such as the light-cone transform 10,11 and f-k migration 12 , and various other methods including Fermat paths 13 , Bayesian methods 14 , phasor fields 15,16 , and inverse rendering 17,18 . Regardless of the algorithm used, extremely low levels of informative light for macroscopic scenes typically force active NLOS experiments to use single-photon detectors, acquire transient information from many repeated illuminations, and limit the hidden scene to around 1 meter from the relay surface.…”