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This theoretical study explores using microwave fields to control the photonic Spin Hall Effect within atomic systems, enabling precise microwave electrometry and potential quantum optical switching. The research demonstrates how tuning relative phases can switch this effect on or off, offering new pathways for high-sensitivity quantum sensing applications. By leveraging closed-loop atomic configurations, the work bridges concepts from optics and quantum physics to advance next-generation sensing technologies.
Microwave Controlled Photonic Spin Hall Effect in Atomic System and Microwave Electrometry
arXiv:2512.14586v2 Announce Type: replace-cross Abstract: The photonic Spin Hall Effect (SHE) causes a polarization dependent transverse shift of light at an interface. In this paper, we theoretically investigate the microwave controlled photonic SHE and microwave electrometry in a closed-loop $\Lambda$-type atomic system. At zero probe detuning ($\Delta_p = 0$) and relative phase $\phi=0,\pi$, the photonic SHE magnitude remains at the intrinsic finite beam saturation limit $w_0/2$, whereas the microwave field shifts its angular position linearly with opposite slopes (signs) for the two phases, enabling differential microwave electric field sensing. At $\phi=\pi/2$, the photonic SHE magnitude decays exponentially with $\Omega_\mu$, providing weak microwave electric field sensing. In contrast, at $\Delta_p = \pm \Omega_c$ (control field coupling), the photonic SHE reaches a maximum of half the incident beam waist when $\Omega_{\mu} \geq \Omega_p$ and the phase $\phi$ is optimized. Interestingly, we observed microwave controlled switching of photonic SHE by tuning the relative phase $\phi$ at an optimized value of $\Omega_{\mu}$ and $\Omega_{c}$. Our results may have potential applications in microwave quantum sensing and quantum optical switches based on the photonic SHE.
Abstract:The photonic Spin Hall Effect (SHE) causes a polarization dependent transverse shift of light at an interface. In this paper, we theoretically investigate the microwave controlled photonic SHE and microwave electrometry in a closed-loop $\Lambda$-type atomic system. At zero probe detuning ($\Delta_p = 0$) and relative phase $\phi=0,\pi$, the photonic SHE magnitude remains at the intrinsic finite beam saturation limit $w_0/2$, whereas the microwave field shifts its angular position linearly with opposite slopes (signs) for the two phases, enabling differential microwave electric field sensing. At $\phi=\pi/2$, the photonic SHE magnitude decays exponentially with $\Omega_\mu$, providing weak microwave electric field sensing. In contrast, at $\Delta_p = \pm \Omega_c$ (control field coupling), the photonic SHE reaches a maximum of half the incident beam waist when $\Omega_{\mu} \geq \Omega_p$ and the phase $\phi$ is optimized. Interestingly, we observed microwave controlled switching of photonic SHE by tuning the relative phase $\phi$ at an optimized value of $\Omega_{\mu}$ and $\Omega_{c}$. Our results may have potential applications in microwave quantum sensing and quantum optical switches based on the photonic SHE.
Optics (physics.optics); Atomic Physics (physics.atom-ph); Quantum Physics (quant-ph)
arXiv:2512.14586 [physics.optics]
(or arXiv:2512.14586v2 [physics.optics] for this version)
https://doi.org/10.48550/arXiv.2512.14586 Focus to learn more arXiv-issued DOI via DataCite
https://doi.org/10.1002/qute.70432 Focus to learn more DOI(s) linking to related resources
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Full text under the publisher's open licence · 281 words
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