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This research establishes fundamental limits on quantum metrology by proving that Gaussian diffusion noise imposes an atom-number-independent floor on GHZ state sensitivity, effectively canceling potential Heisenberg scaling gains. The study identifies the counting statistics of common noise as the critical factor bounding superdecoherence, distinguishing it from traditional spectral analysis for parallel Ramsey protocols. These findings are essential for optimizing quantum sensors and understanding the robustness of entangled states against realistic environmental disturbances.
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Entanglement Drives Common Noise into the Strong-Coupling Regime

arXiv2 min read

arXiv:2607.02962v2 Announce Type: replace Abstract: Under Gaussian collective dephasing parallel to the signal, the superdecoherence of an $N$-atom Greenberger--Horne--Zeilinger (GHZ) state cancels its gain in Fisher information, so GHZ frequency sensitivity is limited to an atom-number-independent floor. We demonstrate that this floor is a property of Gaussian diffusion: a single common phase kick can at most randomize the phase of an $N$-atom coherence, so discrete events at rate $\Gamma$ cannot dephase any coherence order faster than $2\Gamma$. At the same single-atom coherence time, finite-rate Poisson kicks with an absolutely continuous amplitude law therefore saturate the order-$N$ decay rate and restore Heisenberg scaling. We prove that Gaussian diffusion is the worst case for GHZ and Dicke-cat probes under this calibration, that only the Brownian component of L\'evy phase noise sets the asymptotic floor, and that the $1/N$ exponent is optimal for parallel Ramsey protocols. These results identify the counting statistics of the common noise, rather than its spectrum, as the property that bounds superdecoherence.

Abstract:Under Gaussian collective dephasing parallel to the signal, the superdecoherence of an $N$-atom Greenberger--Horne--Zeilinger (GHZ) state cancels its gain in Fisher information, so GHZ frequency sensitivity is limited to an atom-number-independent floor. We demonstrate that this floor is a property of Gaussian diffusion: a single common phase kick can at most randomize the phase of an $N$-atom coherence, so discrete events at rate $\Gamma$ cannot dephase any coherence order faster than $2\Gamma$. At the same single-atom coherence time, finite-rate Poisson kicks with an absolutely continuous amplitude law therefore saturate the order-$N$ decay rate and restore Heisenberg scaling. We prove that Gaussian diffusion is the worst case for GHZ and Dicke-cat probes under this calibration, that only the Brownian component of Lévy phase noise sets the asymptotic floor, and that the $1/N$ exponent is optimal for parallel Ramsey protocols. These results identify the counting statistics of the common noise, rather than its spectrum, as the property that bounds superdecoherence.

arXiv:2607.02962 [quant-ph]

(or arXiv:2607.02962v2 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.02962 Focus to learn more arXiv-issued DOI via DataCite

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