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This research demonstrates a novel method to generate spin squeezing directly from vacuum Rabi oscillations using geometric focusing on the Bloch sphere, offering a robust protocol for quantum metrology with atoms like $^{171}$Yb. By leveraging the curvature of the state space, the study achieves optimal squeezing parameters that scale favorably with atom number while remaining resilient to realistic dissipation. This advancement provides a practical pathway for enhancing precision measurements in neutral-atom quantum systems without requiring external squeezing resources.
Spin squeezing by geometric focusing in vacuum Rabi oscillations
arXiv:2609.02738v1 Announce Type: new Abstract: We show that vacuum Rabi oscillations can directly generate spin squeezing through geometric focusing on the Bloch sphere. Starting from a coherent spin state resonantly coupled to a cavity initially in the vacuum state, quantum fluctuations are focused by the curvature of the Bloch sphere as the collective spin approaches the atomic ground state, producing squeezing transverse to the direction of motion. The squeezing timescale is set by the collective Rabi frequency $t_s\sim 1/(g\sqrt{N})$. The optimal Wineland squeezing parameter scales as $\xi_{\rm opt}^2\propto N^{-1/3}$, which is an outcome of the competition between the geometric focusing effects and the cavity-field vacuum fluctuations. The squeezing remains robust against realistic dissipation. In the end, an application example of $^{171}$Yb is briefly discussed to show the feasibility of our protocol.
Abstract:We show that vacuum Rabi oscillations can directly generate spin squeezing through geometric focusing on the Bloch sphere. Starting from a coherent spin state resonantly coupled to a cavity initially in the vacuum state, quantum fluctuations are focused by the curvature of the Bloch sphere as the collective spin approaches the atomic ground state, producing squeezing transverse to the direction of motion. The squeezing timescale is set by the collective Rabi frequency $t_s\sim 1/(g\sqrt{N})$. The optimal Wineland squeezing parameter scales as $\xi_{\rm opt}^2\propto N^{-1/3}$, which is an outcome of the competition between the geometric focusing effects and the cavity-field vacuum fluctuations. The squeezing remains robust against realistic dissipation. In the end, an application example of $^{171}$Yb is briefly discussed to show the feasibility of our protocol.
arXiv:2609.02738 [quant-ph]
(or arXiv:2609.02738v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.02738 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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