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Chinese Physics B

Rydberg-Atom-Based Terahertz Reflection System for Full-Field Imaging of Surface Characteristics

X J Li, Yu Wu, Bin Zhang, Qi-Rong Huang, Jun Wan, H. W. Zhao, Tao Li, Xin-Yu Yang, Lie Feng, Kai-Qing Zhang, Wei Huang, Hai-Xiao Deng

Published Jul 17, 2026• 0 citations
Publisher

Abstract

Abstract Rydberg-atom–based Terahertz (THz) reflection imaging provides ultra-high sensitivity and, in principle, the potential for MHz-level imaging speed, overcoming the limitations of THz transmission imaging for strongly absorbing samples. Here, we experimentally demonstrate a Rydberg-atom THz reflection imaging system, converting reflected THz fields into visible fluorescence using a cesium vapor cell along the 14 P 3/2 → 13 D 5/2 → 6 P 3/2 pathway, and sequentially imaging the fluorescence with a sCMOS camera. The system achieves clear reflection images with a minimum resolvable line-pair period of approximately 1.26 mm, and a minimum detectable power of 2.41 fW·s -1/2 per (6.5×6.5) μ m 2 pixel. Representative applications include reflection imaging of metallic samples, discrimination of Polar Liquids, and non-contact visualization of superficial human vasculature and finger motion. This system offers a promising route toward high-frame-rate, room-temperature, full-field THz imaging for both industrial and scientific applications.

DOI
10.1088/1674-1056/ae8c1a

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Terahertz imaging has become increasingly important across various fields and practical production applications. Achieving both high sensitivity and high speed remains a primary challenge for most current THz imaging technologies. In this work, we present an imaging system based on Rydberg atomic vapor operating at frequencies exceeding 1 THz. By utilizing Cesium 133 atoms coupled with THz waves, de-excitation radiation generated after atomic excitation to Rydberg states converts invisible THz waves into visible light, enabling the acquisition of spatial information and intensity distributions of THz fields. The system achieves a minimum detectable power of 330 fW /s 1/2 per (2.4×2.4) μm 2 , an imaging resolution of approximately 1.7 mm, and an imaging bandwidth of 8.6 MHz. Additionally, the theoretical imaging rate can exceed 1 MHz. The Rydberg-atom-based THz imaging system exhibits a simple structure and is amenable to miniaturization. This THz imaging method holds promise for advancing applications in THz nondestructive testing, biomedical imaging, and concealed object detection.
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Rydberg atom-based sensors have emerged as highly sensitive tools for terahertz (THz) metrology, yet most current imaging techniques discard crucial phase information. In this Letter, we present a coherent THz-to-optical conversion scheme in warm Rb vapor that enables complex-amplitude field imaging. By manipulating the phase-matching conditions via an adjustable interference pattern of optical probe beams, we demonstrate the ability to perform tomographic reconstruction of the THz field distribution. We experimentally validate the spatial resolution and phase-sensitivity of the system by resolving sub-centimeter features and identifying incident angles of arrival. Our results establish a robust framework for phase-resolved THz imaging and holography using atomic vapors at room temperature.
Broadband and sensitive terahertz (THz) detectors are essential for advancing applications in THz technology. Rydberg atoms were proven to be a promising THz detector, but its detection bandwidth and sensitivity still remain challenging. In this paper, a four-level cesium Rydberg atom system was designed, and it can be operated using electromagnetically induced transparency (EIT). Above all, a high-performance THz detection scheme was demonstrated by introducing frequency detuning of the THz wave relative to the atomic resonance and analyzing the asymmetric splitting between the EIT main peak and the off-resonant Autler–Townes (AT) peak. This method exploits the linear dependence of Rydberg eigenfrequencies on THz detuning and allows us to resolve weak THz electric fields even in the nonlinear regime. Furthermore, the probe laser power was found to influence the EIT signal, with low power producing a narrow but weak signal and high power yielding a stronger yet broader signal; therefore, under a probe power of 20 μW, a minimum detectable field of 2.43 V/m at 108.9 GHz was achieved, while a probe power of 500 μW allowed the detection bandwidth to be extended to 14 GHz. That means that the sensitivity was improved by 50% and the bandwidth was improved by three orders compared with the conventional EIT–AT method. Theoretical modeling results based on the Lindblad master equation are consistent with the experimental results. This frequency-detuning-based strategy offers a physically traceable and scalable approach to advancing quantum-enhanced THz sensing under ambient conditions.
A Rydberg atom detector provides a promising approach for characterizing terahertz (THz) electric fields. Electric field polarization detection is crucial for accurately characterizing THz wave propagation, identifying signal sources and interference, and so on. This paper demonstrates a method for accurate measurement of THz polarization using a four-level cesium Rydberg-atom system. By analyzing the evolution of electromagnetically induced transparency and Autler-Townes spectra under different polarization configurations, the THz polarization angle is quantitatively determined from the relative intensities and asymmetry of the spectral peaks. The results show that the spectral response exhibits a clear dependence on the polarization angle with symmetry about 90°, enabling unambiguous angle determination, and a polarization resolution of 1.28° is achieved. Furthermore, compared with a Schottky diode detector, the proposed method exhibits comparable sensitivity while providing improved fitting consistency and robustness. This approach simplifies both theoretical analysis and experimental implementation for THz polarization measurement, and is promising for applications in THz sensing and spectroscopy.