Zheng H Y, Luo Y H, Li T L, et al. Confocal non-line-of-sight imaging based on spatial multiplexing detection[J]. Opto-Electron Eng, 2023, 50(5): 220256. doi: 10.12086/oee.2023.220256
Citation: Zheng H Y, Luo Y H, Li T L, et al. Confocal non-line-of-sight imaging based on spatial multiplexing detection[J]. Opto-Electron Eng, 2023, 50(5): 220256. doi: 10.12086/oee.2023.220256

Confocal non-line-of-sight imaging based on spatial multiplexing detection

    Fund Project: National Natural Science Foundation of China (62271468)
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  • Non-line-of-sight imaging techniques can be used to capture images of objects that are hidden away in corners, and this technology has many useful applications. The captured signal is insufficient when the laser sends laser light to the intermediate surface, which is a problem when utilizing a digital micromirror device (DMD) in a confocal non-line-of-sight optical route because of the spectroscopic impact of the DMD. In order to increase the signal-to-noise ratio of the echo signal, the acquisition method of spatial multiplexing detection (SMD) is introduced into the confocal optical path in this study. SMD is integrated with the reconstruction algorithm of the light-cone transform (LCT). Based on the confocal non-line-of-sight imaging optical path, the laser initially emits laser pulses, followed by SMD collecting concealed object echoes, and the LCT algorithm concludes the reconstruction. The experimental results demonstrate that the single-pixel camera can complete the reconstruction using the LCT algorithm after employing the SMD acquisition method in the confocal non-line-of-sight optical route, which may improve the signal-to-noise ratio and the reconstruction quality.
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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.

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