4.6 Article

Generalized echo squeezing protocol with near-Heisenberg-limit sensitivity and strong robustness against detection noise and variation in squeezing parameter

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PHYSICAL REVIEW A
卷 107, 期 3, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevA.107.032610

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We introduce a generalized echo squeezing protocol (GESP) as a generalization of the Schrodinger cat state protocol. The GESP allows the squeezing parameter to take on arbitrary values instead of being limited to pi/2. Analytically, we demonstrate that over a broad range of the squeezing parameter, the GESP achieves sensitivity close to the Heisenberg limit within a factor of 2, which is independent of the parity of the number of atoms.
We present a generalized echo squeezing protocol (GESP) as a generalization of the Schrodinger cat state protocol with the value of the squeezing parameter being an arbitrary number rather than pi /2. We show analyti-cally that over a very broad range of the squeezing parameter the sensitivity of the GESP reaches the Heisenberg ./ limit within a factor of 2. For a large number of atoms, N, this plateau interval is almost the whole range from zero to pi /2, and the sensitivity is independent of the parity of N. Therefore, it is possible to operate a sensor over a wide interval of the squeezing parameter without changing the sensitivity. This is to be contrasted with the conventional echo squeezing protocol (CESP) which only works for a very small interval of the squeezing parameter. We also show that, in contrast to the CESP, the sensitivity of the GESP is close to the quantum Cramer-Rao bound over the whole range of the squeezing parameter, indicating that the phase-shift information contained in the quantum state is near-optimally extracted. We find that the enhancement in sensitivity in the case of the GESP is due to a combination of two parameters: the phase magnification factor (PMF) and the noise amplification factor (NAF). As the value of the squeezing parameter increases, both PMF and NAF increase, while keeping the ratio of the PMF to the NAF essentially constant, yielding a net enhancement of sensitivity ./ at the Heisenberg limit within a factor of 2 over the whole plateau interval. An important consequence of this behavior is that the robustness of the GESP against detection noise easily exceeds that of the CESP for a broad range of values of the squeezing parameter. As such, in the context of an experimental study, it should be possible to achieve a net enhancement in sensitivity higher than that for the CESP, under typical conditions where detection noise exceeds the quantum projection noise of an unsqueezed state with the same number of atoms. Finally, we consider the fragility of the GESP against decoherence mechanisms, and show how a balance between the fragility against the decoherence mechanisms and the robustness against detection noise would in practice determine the optimal choice of parameters for the GESP.

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