Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

High-Resolution Near-Field Imaging and Far-Field Antenna Measurements with Atomic Sensors

David Alexander Anderson, Éric Paradis, Georg Raithe, Rachel Sapiro, Matthew T. Simons, Christopher L. Holloway

Published Aug 1, 2018• 2 citations
Publisher

Abstract

Measurements of radio-frequency (RF) electric fields using atomic sensors based on quantum-optical spectroscopy of Rydberg states in vapors has garnered significant interest in recent years for the establishment of atomic standards for RF electric fields and towards the development of novel RF sensing instrumentation. Here we describe recent work employing atomic sensors for sub-wavelength near-field imaging of a Ku- band horn antenna. We demonstrate near-field imaging capability at a spatial resolution of λ/10 and measurements over a 72 to 240 V/m field range using off-resonance AC-Stark shifts of a Rydberg-atom resonance. A fiber-coupled atomic-sensor probe is also employed in far-field measurements of a WR-90 standard gain horn.

DOI
10.1109/emceurope.2018.8485102

Related papers

High-Resolution Antenna Near-Field Imaging and Sub-THz Measurements with a Small Atomic Vapor-Cell Sensing Element

David Alexander Anderson, Éric Paradis, Georg A. Raithel +2 more

Atomic sensing and measurement of millimeterwave (mmW) and THz electric fields using quantum-optical EIT spectroscopy of Rydberg states in atomic vapors has garnered significant interest in recent years towards the development of atomic electric-field standards and sensor technologies. Here we describe recent work employing small atomic vapor cell sensing elements for near-field imaging of the radiation pattern of a Ku- band horn antenna at 13.49 GHz. We image fields at a spatial resolution of λ/10 and measure over a 72 to 240 V/m field range using off-resonance AC-Stark shifts of a Rydberg resonance. The same atomic sensing element is used to measure sub-THz electric fields at 255 GHz, an increase in mmW-frequency by more than one order of magnitude. The sub-THz field is measured over a continuous ±100 MHz frequency band using a near-resonant mmW atomic transition.

arXiv:1804.09789•Global Symposium on Millimeter-Waves•May 1, 2018•22 citations

Towards Rydberg Atom Synthetic Apertures: Wide-Area High-Resolution RF Amplitude and Phase Imaging With Rydberg Probes

David Alexander Anderson, Luís F. Gonçalves, Remy Legaie +1 more

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, 2023•1 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.

IEEE Antennas and Wireless Propagation Letters•Oct 5, 2022•54 citations

Synthetic Aperture RF Reception Using Rydberg Atoms

Nikunjkumar Prajapti, Alexandra B. Artusio‐Glimpse, Matthew T. Simons +5 more

Rydberg atoms show great promise for use as self-calibrated electric field sensors for a broad range of frequencies. Their response is traceable to the international system of units making them a valuable tool for a variety of applications including traceable channel sounding. The Rydberg atom sensor is an electrically small point probe. Its detection volume is defined by the overlap of probing and coupling lasers, which can be as small as hundreds of microns. We present measurements of the beam-formed output of a horn antenna in the far field at 28 GHz. We move a Rydberg atom sensor over a synthetic aperture to obtain high angular resolution of the received signal and employ electromagnetic induced transparency with AC stark shifting and a local oscillator signal radiated onto the atoms for magnitude and phase detection at each location in the area. These results demonstrate the use of these Rydberg atom sensors in a synthetic aperture configuration and inform their eventual use for traceable channel sounding measurements.

IEEE International Conference on Acoustics, Speech, and Signal Processing Workshops (ICASSPW)•Jun 4, 2023•7 citations

Atom-Based RF Electric Field Metrology: From Self-Calibrated Measurements to Subwavelength and Near-Field Imaging

Christopher L. Holloway, Matthew T. Simons, Joshua A. Gordon +4 more

We discuss a fundamentally new method for electric (E) field strength (V/m) metrology applicable to the near-field. This new approach is significantly different from currently used field measurement techniques in that it is based on the interaction of radio-frequency (RF) E-fields with Rydberg atoms (alkali atoms placed in a glass vapor cell that are excited optically to Rydberg states). The applied RF E-field alters the state of the atoms. The Rydberg atoms act like an RF-to-optical transducer, converting an RF E-field strength to an optical-frequency response. In this new approach, we employ the phenomena of electromagnetically induced transparency (EIT) and Autler-Townes splitting. The RF transition in the four-level atomic system causes a split of the EIT transmission spectrum of a probe laser into two peaks. This splitting is easily measured and is directly proportional to the applied RF E-field amplitude. The significant dipole response of Rydberg atoms enables this technique to make self-calibrating measurements over a large frequency band including 500 MHz to 500 GHz (and possibly up to 1 THz and down to 10s of megahertz). In this paper, we report on our results in the development of this metrology approach, including the first fiber-coupled vapor-cell for E-field measurements. We also discuss key applications, including self-calibrated measurements, millimeter-wave and sub-THz measurements, field mapping, and sub-wavelength and near-field imaging. We show results for mapping the fields inside vapor cells, for measuring the E-field distribution along the surface of a circuit board, and for measuring the near-field at the aperture in a cavity. We also discuss the uncertainties of this measurement technique.

IEEE Transactions on Electromagnetic Compatibility•Jan 10, 2017•158 citations

Atom-based RF field probe: From self-calibrated measurements to sub-wavelength imaging

Christopher L. Holloway, Josh A. Gordon, Matthew T. Simons +5 more

In this presentation, we discuss a fundamentally new approach for an electric (E) field probe design. This new approach is significantly different than currently used field probes in that it is based on the interaction of RF-fields with Rydberg atoms (alkali atoms placed in a glass vapor cell are excited optically to Rydberg states). The applied RF-field alters the resonant state of the atoms. The Rydberg atoms act like an RF-to-optical transducer, converting an RF E-field to an optical-frequency response. The RF probe utilizes the concept of Electromagnetically Induced Transparency (EIT). The RF transition in the four-level atomic system causes a split of the EIT transmission spectrum for a probe laser. This splitting is easily measured and is directly proportional to the applied RF field amplitude. The significant dipole response of Rydberg atoms enables this technique to make self-calibrating measurements over a large frequency band including 1-500 GHz. In this paper, we report on our results in the development of this probe. We also discuss two key applications: that is, self-calibrated measurements and sub-wavelength imaging and field mapping.

IEEE International Conference on Nanotechnology (IEEE-NANO)•Jul 1, 2015•1 citation
Measurements of radio-frequency (RF) electric fields using atomic sensors based on quantum-optical spectroscopy of Rydberg states in vapors has garnered significant interest in recent years for the establishment of atomic standards for RF electric fields and towards the development of novel RF sensing instrumentation. Here we describe recent work employing atomic sensors for sub-wavelength near-field imaging of a Ku- band horn antenna. We demonstrate near-field imaging capability at a spatial resolution of λ/10 and measurements over a 72 to 240 V/m field range using off-resonance AC-Stark shifts of a Rydberg-atom resonance. A fiber-coupled atomic-sensor probe is also employed in far-field measurements of a WR-90 standard gain horn.
Atomic sensing and measurement of millimeterwave (mmW) and THz electric fields using quantum-optical EIT spectroscopy of Rydberg states in atomic vapors has garnered significant interest in recent years towards the development of atomic electric-field standards and sensor technologies. Here we describe recent work employing small atomic vapor cell sensing elements for near-field imaging of the radiation pattern of a Ku- band horn antenna at 13.49 GHz. We image fields at a spatial resolution of λ/10 and measure over a 72 to 240 V/m field range using off-resonance AC-Stark shifts of a Rydberg resonance. The same atomic sensing element is used to measure sub-THz electric fields at 255 GHz, an increase in mmW-frequency by more than one order of magnitude. The sub-THz field is measured over a continuous ±100 MHz frequency band using a near-resonant mmW atomic transition.
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 λ/2\lambda /2λ/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.
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.
Rydberg atoms show great promise for use as self-calibrated electric field sensors for a broad range of frequencies. Their response is traceable to the international system of units making them a valuable tool for a variety of applications including traceable channel sounding. The Rydberg atom sensor is an electrically small point probe. Its detection volume is defined by the overlap of probing and coupling lasers, which can be as small as hundreds of microns. We present measurements of the beam-formed output of a horn antenna in the far field at 28 GHz. We move a Rydberg atom sensor over a synthetic aperture to obtain high angular resolution of the received signal and employ electromagnetic induced transparency with AC stark shifting and a local oscillator signal radiated onto the atoms for magnitude and phase detection at each location in the area. These results demonstrate the use of these Rydberg atom sensors in a synthetic aperture configuration and inform their eventual use for traceable channel sounding measurements.
We discuss a fundamentally new method for electric (E) field strength (V/m) metrology applicable to the near-field. This new approach is significantly different from currently used field measurement techniques in that it is based on the interaction of radio-frequency (RF) E-fields with Rydberg atoms (alkali atoms placed in a glass vapor cell that are excited optically to Rydberg states). The applied RF E-field alters the state of the atoms. The Rydberg atoms act like an RF-to-optical transducer, converting an RF E-field strength to an optical-frequency response. In this new approach, we employ the phenomena of electromagnetically induced transparency (EIT) and Autler-Townes splitting. The RF transition in the four-level atomic system causes a split of the EIT transmission spectrum of a probe laser into two peaks. This splitting is easily measured and is directly proportional to the applied RF E-field amplitude. The significant dipole response of Rydberg atoms enables this technique to make self-calibrating measurements over a large frequency band including 500 MHz to 500 GHz (and possibly up to 1 THz and down to 10s of megahertz). In this paper, we report on our results in the development of this metrology approach, including the first fiber-coupled vapor-cell for E-field measurements. We also discuss key applications, including self-calibrated measurements, millimeter-wave and sub-THz measurements, field mapping, and sub-wavelength and near-field imaging. We show results for mapping the fields inside vapor cells, for measuring the E-field distribution along the surface of a circuit board, and for measuring the near-field at the aperture in a cavity. We also discuss the uncertainties of this measurement technique.
In this presentation, we discuss a fundamentally new approach for an electric (E) field probe design. This new approach is significantly different than currently used field probes in that it is based on the interaction of RF-fields with Rydberg atoms (alkali atoms placed in a glass vapor cell are excited optically to Rydberg states). The applied RF-field alters the resonant state of the atoms. The Rydberg atoms act like an RF-to-optical transducer, converting an RF E-field to an optical-frequency response. The RF probe utilizes the concept of Electromagnetically Induced Transparency (EIT). The RF transition in the four-level atomic system causes a split of the EIT transmission spectrum for a probe laser. This splitting is easily measured and is directly proportional to the applied RF field amplitude. The significant dipole response of Rydberg atoms enables this technique to make self-calibrating measurements over a large frequency band including 1-500 GHz. In this paper, we report on our results in the development of this probe. We also discuss two key applications: that is, self-calibrated measurements and sub-wavelength imaging and field mapping.