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    Impact of Thermal Fields on Rydberg Atom Radio Frequency Sensors

    Channprit Kaur1, Pinrui Shen2, Donald Booth2, Andrew Todd1, and James P. Shaffer2,*

    • 1National Research Council Canada, Metrology, Ottawa, Ontario K1A 0R6, Canada
    • 2Quantum Valley Ideas Laboratories, 485 Wes Graham Way, Waterloo, Ontario N2L 6R1, Canada

    • *Contact author: jshaffer@qvil.ca

    Phys. Rev. Lett. 136, 123201 – Published 24 March, 2026

    DOI: https://doi.org/10.1103/lngc-vpr4

    Abstract

    Rydberg atom radio frequency sensors are unique in a number of ways, including possessing extraordinary carrier bandwidth, self-calibration, and accuracy. In this Letter, we examine the impact of thermal radiation on Rydberg atom sensors. Antennas are limited by their thermal background, while Rydberg atom sensors are coherent sensors. Incoherent thermal radiation does not limit Rydberg atom sensors in the same way as an antenna. The primary consequence of a thermal radiation field on Rydberg atom sensors is to decrease their coherence, as the decay rates of the Rydberg states used for sensing the radio frequency field are increased due to the thermal field, i.e., blackbody, modification of the atomic decay rates. Thermal and coherent field excitation are fundamentally different in that thermal fields produce statistically independent excitations with well-defined frequency, polarization, and propagation direction, while coherent states are coherent superpositions of photon number states. Consequently, thermal fields do not contribute to the coherences of the density matrix that are used for Rydberg atom sensing, except for damping them.

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