Noise Mitigation in Quantum-Enhanced Fiber Optic Gyroscopes

We analyze noise in a quantum-enhanced fiber optic gyroscope (FOG), focusing on one of the leading sources of phase uncertainty—uncorrelated photon saturation. Taking a squeezed state input as a source for N00N states, we compute the uncorrelated false coincidence counts at the optimal phase bias and determine an upper limit to the squeezed amplitude ξ which allows for sub-shot noise precision. As examples, we apply parameters of present-day quantum FOG experiments and determine the maximum possible precision enhancement based on their respective ξ and optimal phase bias points. With the aim of supporting future FOG setups with higher N00N state fluxes, our result highlights the need to transition to multimode states to bypass the ξ limitation, such as photon pairs generated by the dynamical Casimir effect.

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Publication Details

Journal
Quantum Reports
Published
2026-05-01
DOI
https://doi.org/10.3390/quantum8020043
Primary Topic
Mechanical and Optical Resonators
Type
article
Field-Weighted Citation Impact
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article

Noise Mitigation in Quantum-Enhanced Fiber Optic Gyroscopes

Joanna Ptasinski, Stefan Evans
Quantum Reports
Mechanical and Optical Resonators
article

Noise Mitigation in Quantum-Enhanced Fiber Optic Gyroscopes

Joanna Ptasinski, Stefan Evans
article en

Abstract

We analyze noise in a quantum-enhanced fiber optic gyroscope (FOG), focusing on one of the leading sources of phase uncertainty—uncorrelated photon saturation. Taking a squeezed state input as a source for N00N states, we compute the uncorrelated false coincidence counts at the optimal phase bias and determine an upper limit to the squeezed amplitude ξ which allows for sub-shot noise precision. As examples, we apply parameters of present-day quantum FOG experiments and determine the maximum possible precision enhancement based on their respective ξ and optimal phase bias points. With the aim of supporting future FOG setups with higher N00N state fluxes, our result highlights the need to transition to multimode states to bypass the ξ limitation, such as photon pairs generated by the dynamical Casimir effect.

Quantum ReportsVol. 8(2)
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Mechanical and Optical Resonators
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