Memory-assisted squeezed light velocimetry under realistic loss and incoherent noise

arXiv:2605.27723 · quant-ph, physics.optics · Submitted 2026-05-26 · Read on arXiv

quant-ph, physics.optics

Submitted: 2026-05-26

Updated: 2026-05-26

Comments: 9 pages, 5 figures. Comments are welcome

Journal ref: AVS Quantum Sci. 8, 034405 (2026)

DOI: 10.1116/5.0345557

License: http://creativecommons.org/licenses/by/4.0/

The gist: We propose a velocity sensor based on a two-memory Mach--Zehnder interferometer fed by a coherent probe and squeezed vacuum, read out by balanced homodyne detection.

Terminology

Abstract

We propose a velocity sensor based on a two-memory Mach--Zehnder interferometer fed by a coherent probe and squeezed vacuum, read out by balanced homodyne detection. One memory is taken as a stationary reference, while the second memory moves during storage, so that its velocity is mapped onto a differential interferometric phase at readout. The two memories are otherwise assumed identical and are described by a Gaussian write--store--read lifetime together with the associated unconditional noise floor. Using the classical Fisher information, we derive the velocity sensitivity, the transmission threshold required for a target quantum gain, and the optimum storage time. The squeezed scheme improves on equal-resource coherent homodyne within an operating window set mainly by total transmission and phase stability. For representative near-term parameters, unconditional memory noise floors up to about 10-1 photons per trial do not by themselves remove the advantage; after optimization the improvement remains at the few-percent level and is limited chiefly by loss.

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