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It is usually challenging to image objects that are beyond sight, yet this technology has many possible applications. In situations like autonomous driving, counterterrorism, and rescue operations, analyzing the object information in the hidden area might help people make better decisions. Ultrafast lasers and detectors with high sensitivity and time resolution have been developed thanks to advances in photoelectric technology. The flight time of photons can be measured with a single photon detector. The intermediary surface receives laser pulses from the laser. Through the reflection of the intervening surface, the laser illuminates the concealed object. The detector gathers the three reflected echo photons that were sent back by the intermediary surface once the hidden object's reflection reaches it, extracts the data from the echo photon, and then uses an image technique to reconstruct the hidden target. In order to complete the reconstruction of hidden objects, the researchers have also successively proposed the reverse projection algorithm (BP), the iterative error anti-projection algorithm, the light-cone transform algorithm (LCT), the surface normal algorithm, and the non-line-of-sight reconstruction algorithm based on virtual waves. However, the scanning of the intermediary surface by the laser can lead to long data acquisition times. Later researchers have used a digital micromirror device (DMD) to flip the echo signals into a single photon detector, which allows the acquisition of signals to be finished without the scanning component. In earlier research, back-projection was used to reconstitute signals obtained with DMDs. In this paper, the spectroscopic effect of the DMD element in the optical route is resolved, and the signal acquisition method of SMD is brought into the non-line-of-sight imaging of the confocal optical path. The hidden object signal is captured by switching the micromirror, and the reconstruction is finished using LCT and BP algorithms, employing a confocal non-line-of-sight imaging optical route with a DMD element. By comparing the reconstruction quality of BP and LCT, SSIM and PSNR demonstrate that LCT can achieve greater reconstruction quality when using the SMD acquisition method. Additionally, research have shown that using this acquisition method will increase the quality of the reconstruction by increasing the laser intensity and the number of sampling points.
Schematics of the experimental set-up for non-line-of-sight imaging
Hadamard observation pattern and matrix. (a) Hadamard observation pattern; (b) Hadamard observation matrix
Principle of spatial multiplexing detection non-line-of-sight imaging. (a) Original signal of each detection point; (b) Four kinds of measurement patterns obtained from Hadamard matrix; (c) Time photon histogram in each measurement mode; (d) Recover the signal of each detection point
Experimental light path diagram
Comparison of reconstruction results. (a) LCT algorithm reconstruction results; (b) BP algorithm reconstruction results
Reconstruction results of 16×16 pixel values for different hidden objects. (a) Rectangle result reconstructed by LCT algorithm; (b) Rectangle result reconstructed by BP algorithm; (c) Triangle result reconstructed by LCT algorithm; (d) Triangle result reconstructed by BP algorithm
The reconstruction result of the 8×8 pixel value of the triangular object. (a) Triangle result reconstructed by LCT algorithm; (b) Triangle result reconstructed by BP algorithm
The reconstruction results of the LCT algorithm obtained with different laser intensities. (a) Reconstruction results with an average laser power of 750 mW; (b) Reconstruction results with an average laser power of 500 mW
Reconstruction results of the LCT algorithm obtained by different sampling arrays. (a) Reconstruction result of the sampling array being16×16; (b) Reconstruction result of the sampling array being 8×8;