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Communications Physics

On-demand instantaneous bandwidth microwave receiver via scalable Rydberg Vapor cell array with Stark comb

Yuechun Jiao, Yuwen Yin, Yunhui He, Jinlian Hu, Cheng Lu, Jingxu Bai, Zhengyang Bai, Weibin Li, Suotang Jia, Jianming Zhao

Published Nov 1, 2026• 0 citations
Publisher

Abstract

Rydberg-atom-based microwave (MW) sensors offer high sensitivity and intrinsic traceability, but their instantaneous bandwidth is fundamentally limited by atomic coherence time. Here, we introduce a scalable sensing architecture that overcomes this limitation by spatially multiplexing atomic detection channels with a Stark comb, in which an MW frequency comb (MFC) and a position-dependent Stark field enable each Rydberg vapor cell to function as an independent frequency-selective heterodyne receiver. We experimentally validate the 210 MHz instantaneous-bandwidth channelized receiver architecture through sequential characterization of individual Stark-shifted channels using a 21-line MFC, while maintaining an overall sensitivity of 326.6 nVcm −1 Hz −1/2 despite a 160 MHz tuning of the carrier resonance frequency. Full simultaneous operation across the 210 MHz bandwidth requires parallel implementation and readout of all channels. This scalable architecture enables on-demand instantaneous bandwidth while preserving sensitivity, providing a pathway toward real-time broadband MW detection for radar, communications, and spectrum monitoring.

DOI
10.1038/s42005-026-02941-9

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Rydberg-atom-based microwave (MW) sensors offer high sensitivity and intrinsic traceability, but their instantaneous bandwidth is fundamentally limited by atomic coherence time. Here, we introduce a scalable sensing architecture that overcomes this limitation by spatially multiplexing atomic detection channels with a Stark comb, in which an MW frequency comb (MFC) and a position-dependent Stark field enable each Rydberg vapor cell to function as an independent frequency-selective heterodyne receiver. We experimentally validate the 210 MHz instantaneous-bandwidth channelized receiver architecture through sequential characterization of individual Stark-shifted channels using a 21-line MFC, while maintaining an overall sensitivity of 326.6 nVcm −1 Hz −1/2 despite a 160 MHz tuning of the carrier resonance frequency. Full simultaneous operation across the 210 MHz bandwidth requires parallel implementation and readout of all channels. This scalable architecture enables on-demand instantaneous bandwidth while preserving sensitivity, providing a pathway toward real-time broadband MW detection for radar, communications, and spectrum monitoring.
Broadband Rydberg Atomic Microwave Sensing with 44.6 \,MHz Instantaneous Bandwidth
Rydberg atoms have become a promising novel type of microwave sensor due to their excellent physical properties -- broad frequency coverage and large electric dipole moments. High sensitivity and broad instantaneous bandwidth are two indispensable requirements for deployable Rydberg microwave sensors. However, enabling broadband operation while retaining high sensitivity has been a longstanding barrier limiting their applications. We propose and experimentally demonstrate a Rydberg microwave sensor whose instantaneous bandwidth is significantly enhanced via an auxiliary microwave field. By finely modulating the Rydberg energy levels with this field, we broaden the bandwidth substantially while retaining the sensor's inherent high sensitivity. An instantaneous bandwidth of 44.6 \,MHz ($\pm22.322.322.3\,MHz)withasensitivityof225.7MHz) with a sensitivity of 225.7MHz)withasensitivityof225.7\,nVnVnV\,cmcmcm^{-1}\,HzHzHz^{-1/2}$ is realized in a thermal 87^{87}87Rb vapor with the local microwave frequency of 16.03 \,GHz. Our work delivers concurrent broad instantaneous bandwidth and high sensitivity for Rydberg microwave sensors, paving a technically viable path for their practical deployment in broadband microwave metrology, radar, and wireless communication.
Microwave frequency comb represents one of the effective solutions to address the bandwidth limitation in Rydberg atom-based microwave measurements. Here, we demonstrate that by optimizing the phase and intensity of the microwave frequency comb, the average spectral response can be enhanced to achieve optimal flatness in the microwave frequency comb spectrum. This optimization enables the realization of instantaneous bandwidth for a Rydberg receiver at a resonant frequency of 8.556 GHz. This work holds significant implications for the detection of broadband instantaneous microwave signals in Rydberg atom systems, with substantial application potential in fields such as microwave frequency metrology, communications, and radar.
Achieving 100 \,MHz Instantaneous Bandwidth in a Broadband Rydberg Microwave Sensor
Rydberg atoms have attracted considerable attention in recent years as a novel platform for microwave sensing, owing to their unique physical merits: large transition dipole moments between Rydberg levels and broad frequency coverage. As a critical figure of merit for Rydberg microwave sensors, instantaneous bandwidth serves as a key benchmark for evaluating their viability in practical applications. Previous studies on instantaneous bandwidth remain limited to single-frequency operation, with typical demonstrated values of only tens of megahertz, a constraint that hampers the real-world deployment of this sensing technology. Here, we experimentally achieve an instantaneous bandwidth of over 100 \,MHz across a broad frequency range of 2.7-20 \,GHz and realize a sensitivity in the hundreds of nV \,cm−1 ^{-1}\,−1Hz−1/2^{-1/2}−1/2 range. The physical mechanism lies in the dressed-state coherence and the interference effect between different transition channels. Our work substantially broadens the instantaneous bandwidth of Rydberg microwave sensors and paves the way for their practical deployment in fields such as radar and wireless communications.
Rydberg-atomic receivers exhibit exceptional sensitivity yet are fundamentally constrained by the narrow instantaneous bandwidth, limiting their practical deployment in broadband scenarios. Prior approaches typically expand the bandwidth by physically broadening the atomic response, which usually requires auxiliary electromagnetic fields or stringent parameter tuning, thereby increasing overall system complexity. Here, we propose a compressive spectral multiplexing framework implemented in a waveguide-coupled Rydberg atomic receiver using a frequency-modulated local oscillator (FMLO). The FMLO creates multiple parallel sensing channels that collectively constitute a physical compressive sensing matrix, generating multiple narrowband intermediate-frequency replicas of the input signal. Thus, a broadband microwave spectrum is projected onto a set of narrowband atomic responses. It is demonstrated that spectral information spanning a bandwidth of over 640 MHz can be effectively compressed into the intrinsic atomic bandwidth of 126 kHz, achieving a spectrum compression ratio exceeding 1000. Furthermore, these output replicas offer intrinsic measurement redundancy and facilitate signal-to-noise ratio enhancement. An approximate 10 dB gain is achieved in the required bit-energy-to-noise-power-density ratio for multi-channel communication via maximal-ratio combining. This approach requires no auxiliary fields or broadband electronics, providing a simple and scalable pathway for chip-scale quantum receivers, latency-critical sensing, and next-generation wireless communications.
We demonstrate the continuous broadband microwave receivers based on AC Stark shifts and Floquet states of Rydberg levels in a cesium atomic vapor cell. The resonant transition frequency of two adjacent Rydberg states 78 S1/2 and 78 P1/2 is tuned based on AC Stark effect of 70 MHz radio frequency (RF) field that is applied outside the vapor cell. The use of the j=1/2 Rydberg states ensures that only a single mj sublevel is involved. The generated Rydberg Floquet states act to enhance the sensitivity of the AC-Stark-tuned states when the frequency is matched and further extend the bandwidths. We achieve microwave field measurements with over 1.172 GHz continuous frequency tuning and a sensitivity ranging from 280.2 nVcm−1Hz−1/2 to 14.6 μ Vcm−1Hz−1/2. The achieving of continuous frequency and high sensitivity microwave detection will promote the application of Rydberg receivers in the radar technique and wireless communication.
Quantum sensing using Rydberg atoms offers unprecedented opportunities for next-generation radar systems, transcending classical limitations in miniaturization and spectral agility. Implementing this paradigm for radar sensing, this work proposes a quantum-enhanced radar reception architecture enabled by the emerging Rydberg atomic receiver, replacing conventional antenna-to-mixer chains with a centimeter-scale vapor cell. The proposed approach is based on electromagnetically induced transparency with the Autler-Townes splitting enabling direct RF-to-optical downconversion within the atomic medium via an external co-frequency reference. To circumvent the intrinsic bottleneck on instantaneous bandwidth of atomic receiver, we invoke a non-uniform stepped-frequency synthesis strategy combining coarse laser frequency tuning with fine AC-Stark shift compensation. Additionally, we establish a nonlinear response model of the Rydberg atomic homodyne receiver and propose a customized nonlinear compensation method that extends the linear dynamic range by over 7 dB. We develop a compressive sensing algorithm (CS-Rydberg) to suppress noise and mitigate the undersampling problem. Experimentally, we demonstrate a compact prototype achieving centimeter-level ranging precision (RMSE = 1.06 cm) within 1.6-1.9 m. By synthesizing GHz-bandwidth (2.6-3.6 GHz), resolvable target separations down to 15 cm are observed under controlled sparse scenarios. These results not only validate the feasibility of quantum sensing based on Rydberg atomic receivers but also underscore the architecture's inherent scalability: by harnessing the atoms' ultra-broad spectral response, the synthesized bandwidth can be extended well beyond the current range, enabling sub-centimeter resolution in future radar systems while preserving quantum-traceable calibration and a highly simplified front end.