We present on the recent development of an atomic antenna probe and front-end based on Rydberg atoms for applications in radio-frequency (RF) imaging and synthetic apertures. Fundamental atom-RF responses and RF amplitude and phase determination methods for Rydberg atom probes are described. We demonstrate electric field imaging in the near-field of a 2.5 GHz Yagi-Uda antenna device under test (DUT) using a portable Rydberg atom probe and integrated front-end, the Rydberg Field Probe (RFP). A wide-area RF electric field map is generated by positioning of the RFP at discrete spatial measurement locations in the near field of the DUT, from which a composite image of the two-dimensional antenna pattern is realized at a spatial resolution of $\lambda /2$ and field uncertainties within 5.5%. Finally, we demonstrate RF phase imaging of a 100 GHz field using a Rydberg EIT optical fluorescence imager and RF self-homodyning, towards RF phase-sensing and imaging at millimeter-wave frequencies.We present on the recent development of an atomic antenna probe and front-end based on Rydberg atoms for applications in radio-frequency (RF) imaging and synthetic apertures. Fundamental atom-RF responses and RF amplitude and phase determination methods for Rydberg atom probes are described. We demonstrate electric field imaging in the near-field of a 2.5 GHz Yagi-Uda antenna device under test (DUT) using a portable Rydberg atom probe and integrated front-end, the Rydberg Field Probe (RFP). A wide-area RF electric field map is generated by positioning of the RFP at discrete spatial measurement locations in the near field of the DUT, from which a composite image of the two-dimensional antenna pattern is realized at a spatial resolution of $\lambda /2$ and field uncertainties within 5.5%. Finally, we demonstrate RF phase imaging of a 100 GHz field using a Rydberg EIT optical fluorescence imager and RF self-homodyning, towards RF phase-sensing and imaging at millimeter-wave frequencies.

IEEE International Conference on Acoustics, Speech, and Signal Processing Workshops (ICASSPW)Jun 4, 20231 citation

Rydberg atoms in microwave fields

Thomas F. Gallagher

Annual Meeting Optical Society of AmericaJan 1, 19930 citations

Precise measurement of a weak radio frequency electric field using a resonant atomic probe*

Liping Hao, Yongmei Xue, Jiabei Fan +3 more

We present a precise measurement of a weak radio frequency electric field with a frequency of ≲ 3 GHz employing a resonant atomic probe that is constituted with a Rydberg cascade three-level atom, including a cesium ground state |6S1/2⟩, an excited state |6P3/2⟩, and Rydberg state |nD5/2⟩. Two radio frequency (RF) electric fields, noted as local and signal fields, couple the nearby Rydberg transition. The two-photon resonant Rydberg electromagnetically induced transparency (Rydberg-EIT) is employed to directly read out the weak signal field having hundreds of kHz difference between the local and signal fields that is encoded in the resonant microwave-dressed Rydberg atoms. The minimum detectable signal fields of E Smin = 1.36 ± 0.04 mV/m for 2.18 GHz coupling |68D5/2⟩ → |69P3/2⟩ transition and 1.33 ± 0.02 mV/m for 1.32 GHz coupling |80D5/2⟩ → |81P3/2⟩ transition are obtained, respectively. The bandwidth dependence is also investigated by varying the signal field frequency and corresponding −3 dB bandwidth of 3 MHz is attained. This method can be employed to perform a rapid and precise measurement of the weak electric field, which is important for the atom-based microwave metrology.We present a precise measurement of a weak radio frequency electric field with a frequency of ≲ 3 GHz employing a resonant atomic probe that is constituted with a Rydberg cascade three-level atom, including a cesium ground state |6S1/2⟩, an excited state |6P3/2⟩, and Rydberg state |nD5/2⟩. Two radio frequency (RF) electric fields, noted as local and signal fields, couple the nearby Rydberg transition. The two-photon resonant Rydberg electromagnetically induced transparency (Rydberg-EIT) is employed to directly read out the weak signal field having hundreds of kHz difference between the local and signal fields that is encoded in the resonant microwave-dressed Rydberg atoms. The minimum detectable signal fields of E Smin = 1.36 ± 0.04 mV/m for 2.18 GHz coupling |68D5/2⟩ → |69P3/2⟩ transition and 1.33 ± 0.02 mV/m for 1.32 GHz coupling |80D5/2⟩ → |81P3/2⟩ transition are obtained, respectively. The bandwidth dependence is also investigated by varying the signal field frequency and corresponding −3 dB bandwidth of 3 MHz is attained. This method can be employed to perform a rapid and precise measurement of the weak electric field, which is important for the atom-based microwave metrology.

Chinese Physics BJan 16, 202029 citations

Electric field effects in Rydberg atoms

David A. Harmin

Jan 1, 19851 citation

A High-Efficiency Fiber-Coupled Rydberg-Atom Integrated Probe and Its Imaging Applications

Ruiqi Mao, Yi Lin, Kai Yang +2 more

Atomic sensing and electric field measurements based on the use of the all-optical electromagnetic induction transparency (EIT) spectrum of Rydberg atoms have attracted great interest due to the advantages of self-calibration, Le Système International d'unités traceability, and a broadband spectrum. At the same time, this methodology also promotes the development of atomic sensor technology. We present a novel high-efficiency Rydberg-atom radio-frequency (RF) electric (E) field integrated probe (Rydberg Field Probe or RFP). The high-efficiency RFP consists of a 10 mm cubic 133Cs vapor cell, a dichroic mirror, three collimating lenses, and three fibers. This system can be used to independently control two counterpropagating lasers passing through a vapor cell, easing the design effort. In addition, the overall system efficiency can reach a value of 40.4%, reducing the EIT power broadening doe conventional RFPs. Based on the designed high-efficiency RFP, near-field electric field measurement and imaging of a C-band horn antenna at 4.48 GHz are performed by using the resonant RF field of the 133Cs atomic Rydberg state at room temperature with a spatial resolution of λ/6. These results promote the development of atomic sensing technology and show great application potential for the measurement of measuring high-resolution radio frequency electric fields and arrays of RFPs.Atomic sensing and electric field measurements based on the use of the all-optical electromagnetic induction transparency (EIT) spectrum of Rydberg atoms have attracted great interest due to the advantages of self-calibration, Le Système International d'unités traceability, and a broadband spectrum. At the same time, this methodology also promotes the development of atomic sensor technology. We present a novel high-efficiency Rydberg-atom radio-frequency (RF) electric (E) field integrated probe (Rydberg Field Probe or RFP). The high-efficiency RFP consists of a 10 mm cubic 133Cs vapor cell, a dichroic mirror, three collimating lenses, and three fibers. This system can be used to independently control two counterpropagating lasers passing through a vapor cell, easing the design effort. In addition, the overall system efficiency can reach a value of 40.4%, reducing the EIT power broadening doe conventional RFPs. Based on the designed high-efficiency RFP, near-field electric field measurement and imaging of a C-band horn antenna at 4.48 GHz are performed by using the resonant RF field of the 133Cs atomic Rydberg state at room temperature with a spatial resolution of λ/6. These results promote the development of atomic sensing technology and show great application potential for the measurement of measuring high-resolution radio frequency electric fields and arrays of RFPs.

IEEE Antennas and Wireless Propagation LettersOct 5, 202254 citations

\lambda /2

and field uncertainties within 5.5%. Finally, we demonstrate RF phase imaging of a 100 GHz field using a Rydberg EIT optical fluorescence imager and RF self-homodyning, towards RF phase-sensing and imaging at millimeter-wave frequencies.