Bounding the quantum limits of precision for phase estimation with loss and thermal noise

Abstract

We consider the problem of estimating an unknown but constant carrier phase modulation $\theta$ using a general -- possibly entangled -- $n$-mode optical probe through $n$ independent and identical uses of a lossy bosonic channel with additive thermal noise. We find an upper bound to the quantum Fisher information (QFI) of estimating $\theta$ as a function of $n$, the mean and variance of the total number of photons $N_{\mathrm{S}}$ in the $n$-mode probe, the transmissivity $\eta$ and mean thermal photon number per mode ${\bar{n}}_{\mathrm{B}}$ of the bosonic channel. Since the inverse of QFI provides a lower bound to the mean-squared error (MSE) of an unbiased estimator $\tilde{\theta }$ of $\theta$, our upper bound to the QFI provides a lower bound to the MSE. It already has found use in proving fundamental limits of covert sensing, and could find other applications requiring bounding the fundamental limits of sensing an unknown parameter embedded in a correlated field.

No major changes to previous version. Change in the title and abstract, change in the presentation and structure, an example of the bound is now included, and some references were added. Comments are welcome

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• Gaussian phase sensitivity of boson-sampling-inspired strategies
• Simultaneous optical phase and loss estimation revisited: measurement and probe incompatibility
• Optimal finite-dimensional probe states for quantum phase estimation
• High-precision estimation of the parameters in the reservoir via the two-level system
• Linear-optical protocols for mitigating and suppressing noise in bosonic systems
• Multiparameter quantum metrology with postselection measurements