Globally optimal interferometry with lossy twin Fock probes

• URL: http://arxiv.org/abs/2308.05871v2
• Date: Wed, 15 May 2024 21:27:36 GMT
• Title: Globally optimal interferometry with lossy twin Fock probes
• Authors: T. J. Volkoff, Changhyun Ryu,
• Abstract summary: We show that a method of moments readout of two quadratic spin observables $J_z2$ and $J_+2+J_-2$ is globally optimal for Dicke state probes. In the lossy setting, we derive the time-inhomogeneous Markov process describing the effect of particle loss on twin Fock states.
• Score: 0.0
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: Parity or quadratic spin (e.g., $J_{z}^{2}$) readouts of a Mach-Zehnder (MZ) interferometer probed with a twin Fock input state allow to saturate the optimal sensitivity attainable among all mode-separable states with a fixed total number of particles, but only when the interferometer phase $\theta$ is near zero. When more general Dicke state probes are used, the parity readout saturates the quantum Fisher information (QFI) at $\theta=0$, whereas better-than-standard quantum limit performance of the $J_{z}^{2}$ readout is restricted to an $o(\sqrt{N})$ occupation imbalance. We show that a method of moments readout of two quadratic spin observables $J_{z}^{2}$ and $J_{+}^{2}+J_{-}^{2}$ is globally optimal for Dicke state probes, i.e., the error saturates the QFI for all $\theta$. In the lossy setting, we derive the time-inhomogeneous Markov process describing the effect of particle loss on twin Fock states, showing that method of moments readout of four at-most-quadratic spin observables is sufficient for globally optimal estimation of $\theta$ when two or more particles are lost. The analysis culminates in a numerical calculation of the QFI matrix for distributed MZ interferometry on the four mode state $\vert {N\over 4},{N\over 4},{N\over 4},{N\over 4}\rangle$ and its lossy counterparts, showing that an advantage for estimation of any linear function of the local MZ phases $\theta_{1}$, $\theta_{2}$ (compared to independent probing of the MZ phases by two copies of $\vert {N\over 4},{N\over 4}\rangle$) appears when more than one particle is lost.

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