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PreprintCC BY 4.0arXiv

Entanglement Drives Common Noise into the Strong-Coupling Regime

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 Γ cannot dephase any coherence order faster than 2Γ. 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.

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BibTeX
@misc{zhou2026entanglement,
  title = {{Entanglement Drives Common Noise into the Strong-Coupling Regime}},
  author = {Yizhe Zhou and Xusheng Lei and Xing Heng and Zuoxian Wang and Danyue Ma},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2607.02962},
  eprint = {2607.02962},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2607.02962},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Entanglement Drives Common Noise into the Strong-Coupling Regime
AU  - Yizhe Zhou
AU  - Xusheng Lei
AU  - Xing Heng
AU  - Zuoxian Wang
AU  - Danyue Ma
PY  - 2026
DA  - 2026/09/12
PB  - arXiv
DO  - 10.48550/arxiv.2607.02962
UR  - https://arxiv.org/abs/2607.02962
AB  - 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 Γ cannot dephase any coherence order faster than 2Γ. 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.
ER  -