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arXiv:2305.08707 · Applied Physics Letters

Satellite radio detection via dual-microwave Rydberg spectroscopy

Peter K. Elgee, Joshua C. Hill, Kermit-James E. LeBlanc, Gabriel D. Ko, Paul D. Kunz, David H. Meyer, Kevin C. Cox

Published Aug 21, 2023• 26 citations
arXivHTMLPDF

Abstract

Rydberg electric field sensors exploit the large number of Rydberg resonances to provide sensitivity over a broad range of the electromagnetic spectrum. However, due to the difficulty of accessing resonant Rydberg states at ultra-high frequency (UHF) and below, ubiquitous bands in the world's current wireless communications infrastructure, they currently fall, short in sensitivity in this range. We present a resonant Rydberg electric field sensor operating in the UHF band using a dual-optical dual-microwave spectroscopy scheme. Adding an additional microwave photon allows us to access transitions between Rydberg states with higher angular momentum (L=3→4), which have lower resonant frequencies than transitions typically used in Rydberg sensors. We discuss the applicability of this type of sensor across the UHF band and below and measure the resonant sensitivity of our system at 2.3 GHz to be 70(5) μV m−1 Hz−1∕2, 57 times better than the measured sensitivity with a far off-resonant probing scheme at this frequency. We also show the effectiveness of this sensing scheme by measuring Sirius XM satellite radio (2.320–2.345 GHz) received outside the laboratory and rebroadcast onto the atoms.

DOI
10.1063/5.0158150

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physics.atom-phCross-listedarXiv:2610.40952•Nov 2, 2026
Rydberg electric field sensors exploit the large number of Rydberg resonances to provide sensitivity over a broad range of the electromagnetic spectrum. However, due to the difficulty of accessing resonant Rydberg states at ultra-high frequency (UHF) and below, ubiquitous bands in the world's current wireless communications infrastructure, they currently fall, short in sensitivity in this range. We present a resonant Rydberg electric field sensor operating in the UHF band using a dual-optical dual-microwave spectroscopy scheme. Adding an additional microwave photon allows us to access transitions between Rydberg states with higher angular momentum (L=3→4), which have lower resonant frequencies than transitions typically used in Rydberg sensors. We discuss the applicability of this type of sensor across the UHF band and below and measure the resonant sensitivity of our system at 2.3 GHz to be 70(5) μV m−1 Hz−1∕2, 57 times better than the measured sensitivity with a far off-resonant probing scheme at this frequency. We also show the effectiveness of this sensing scheme by measuring Sirius XM satellite radio (2.320–2.345 GHz) received outside the laboratory and rebroadcast onto the atoms.
Rydberg electric field sensors exploit the structured multitude of electronic transitions between Rydberg atomic states. In this way, they can detect electric fields with frequencies spanning DC to THz. However, difficulty accessing resonant transitions at ultra-high frequencies (UHF, 0.3-30 GHz) and below hinders their applicability within this ubiquitous band of the world’s wireless communications infrastructure. We present a Rydberg electric field sensor operating in the UHF band using a resonant dual-optical dual-microwave spectroscopy scheme. This enables access to transitions with lower resonant frequencies, and higher angular momentum (L = 3→4), than those typically used in Rydberg sensors. We measure the resonant sensitivity of our system at 2.3 GHz to be 70(5) µVm−1Hz−1/2, 50 times better than the measured sensitivity with a far off-resonant probing scheme at this frequency. Moreover, we demonstrate the effectiveness of this scheme by measuring Sirius XM satellite radio (2.320 - 2.345 GHz) received outside the laboratory and rebroadcast onto the atoms.
We present a Rydberg atom-based microwave electric field sensor that achieves extended dynamic range and enhanced sensitivity across a broad bandwidth. By characterizing the Autler-Townes (AT) splitting induced by a single-tone microwave field, we demonstrate a spectroscopic method that simultaneously extracts both the microwave frequency and electric field strength directly from the splitting pattern. We implement dual-tone heterodyne detection, achieving a minimum detectable field strength on the order of uV/cm and a sensitivity in the sub-uV/cm/Hz^1/2 regime, while extending the operational bandwidth up to 3 GHz. Through systematic characterization of frequency and power dependencies, we identify optimal operating conditions to minimize power broadening in the resonant AT regime and maximize sensitivity in the far-off-resonance AC Stark regime. The resulting platform combines high sensitivity, broad bandwidth, and a dynamic range of approximately 90 dB, establishing Rydberg atoms as practical sensors for precision electric field metrology.
Detecting microwave signals over a wide frequency range has numerous advantages as it enables simultaneous transmission of a large amount of information, and access to more spectrum resources. This capability is crucial for applications such as microwave communication, remote sensing, and radar. However, conventional microwave receiving systems are limited by amplifiers and band-pass filters that can only operate efficiently in a specific frequency range. Typically, these systems can only process signals within a three-fold frequency range, which limits the data transfer bandwidth of the microwave communication systems. Developing novel atom-integrated microwave sensors, for example, radio frequency (RF)-chip coupled Rydberg atomic receiver, provides opportunities for a large working bandwidth of microwave sensing at the atomic level. Here, an ultra-wide dual-band RF sensing scheme is demonstrated by space-division multiplexing two RF-chip-integrated atomic receiver modules. The system can simultaneously receive dual-band microwave signals that span a frequency range exceeding 6 octaves (300 MHz and 24 GHz). This work paves the way for multi-band microwave reception applications within an ultra-wide range by RF-chip-integrated Rydberg atomic sensor.
Rydberg atomic electric field sensors have attracted the attention of international researchers due to their powerful electric field measurement capabilities. Especially in the shortwave (SW) frequency band (3–30 MHz), using only millimeter-level sensors to receive SW signals is undoubtedly attractive. However, due to the extremely difficult excitation of the Rydberg atoms that resonate with the SW frequency, the sensitivity of the Rydberg atoms SW measurement is low. Here, we report that a method to improve the SW sensitivity by using an SW resonator, which is extremely small in electrical size ($0.0043\lambda \times 0.0035\lambda \times 0.007\lambda $), can achieve continuous resonant frequency coverage from 9.365 to 10.223 MHz and can increase the sensitivity of electric field measurement by a factor of 8633. In the state of far off-resonant, we have achieved a detectable field strength as low as$2.41~\mu $V/m with a sensitivity of$1.71~\mu V/mHzV/mHzV/mHz^{1/2}$using the heterodyne Rydberg atom-based mixer method, which realizes ultrahigh-sensitivity measurement of SWs. In addition, for the first time outside the laboratory, we directly received an amplitude-modulated broadcast signal with 880 km (the straight-line distance between Changsha and Baoji) at 9.81 MHz in the form of a subminiature resonator combined with a Rydberg field probe (RFP), which verified the powerful ability of this sensing scheme.
We present a characterization of the sensitivity of broadband electric field measurements in the Very High Frequency (VHF) and Ultra High Frequency (UHF) bands using AC stark shifting of Rydberg states. The dependence of the sensitivity and dynamic range of the field measurements using nD5/2 states of cesium for principal quantum numbers n= 60, 70, 80, 90 and 100 is presented, detailing the intricacies involved. The frequencies considered for the measurement range from 50 MHz to 900 MHz for which a transverse electromagnetic (TEM) cell is used to excite the Rydberg atoms with the RF fields. The corresponding sensitivities achieved are in the (μV/m)/Hz(μV/m)/\sqrt{Hz}(μV/m)/Hz​ range. A general trend of better sensitivity for higher principal quantum numbers is observed. This work paves the way for a better understanding of the AC Stark dependent field measurements using Rydberg sensors.