Deep Learning Empowered Sub-Diffraction Terahertz Backpropagation Single-Pixel Imaging

TL;DR

This paper introduces a deep learning-based sub-diffraction THz single-pixel imaging method that achieves high-resolution imaging with minimal sampling time by integrating physical propagation models into neural network reconstruction.

Contribution

It presents a novel backpropagation SPI technique combining neural networks and physical models to achieve subwavelength resolution in THz imaging without ultrathin modulators.

Findings

Achieved 118 μm spatial resolution (~λ0/7) in THz imaging.

Reduced sampling ratio to 1.5625%, significantly decreasing data acquisition time.

Enabled sub-diffraction imaging using thick silicon wafers without ultrathin modulators.

Abstract

Terahertz single-pixel imaging (THz SPI) has garnered widespread attention for its potential to overcome challenges associated with THz focal plane arrays. However, the inherently long wavelength of THz waves limits imaging resolution, while achieving subwavelength resolution requires harsh experimental conditions and time-consuming processes. Here, we propose a sub-diffraction THz backpropagation SPI technique. We illuminate the object with continuous-wave 0.36-THz radiation ({\lambda}0 = 833.3 {\mu}m). The transmitted THz wave is modulated by prearranged patterns generated on a 500-{\mu}m-thick silicon wafer and subsequently recorded by a far-field single-pixel detector. An untrained neural network constrained with the physical SPI process iteratively reconstructs the THz images with an ultralow sampling ratio of 1.5625%, significantly reducing the long sampling times. To further suppress the THz diffraction-field effects, a backpropagation SPI from near field to far field is implemented by integrating with a THz physical propagation model into the output layer of the network. Notably, using the thick wafer where THz evanescent field cannot be fully recorded, we achieve a spatial resolution of 118 {\mu}m (~{\lambda}0/7) through backpropagation SPI, thus eliminating the need for ultrathin photomodulators. This approach provides an efficient solution for advancing THz microscopic imaging and addressing other inverse imaging challenges.