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This paper establishes a rigorous mathematical framework for simulating non-perturbative cavity optomechanics involving finite-thickness dielectric plates, addressing limitations in current models that rely on linearization or perturbative approximations. By self-consistently incorporating Fresnel reflection, internal propagation, and mechanical back-action into field equations, it provides essential transfer functions for analyzing coupled optical-mechanical systems in high-precision experiments like gravitational wave detectors. This work advances the theoretical foundation for next-generation quantum sensing architectures where intracavity dielectrics fundamentally reshape the optical mode structure.
Mathematical framework for simulation of non-perturbative cavity optomechanics with plate-like dielectrics
arXiv:2610.17475v1 Announce Type: cross Abstract: Cavity optomechanical models typically treat a sensor either as a perturbative polarizable object in a pre-existing optical field, or solve the field at a fixed equilibrium and linearize in a fixed optical-mode basis. Neither self-consistently determines the spatially resolved cavity field, the optical force, the mechanical equilibrium, and the back-action when a finite-thickness dielectric plate intercepts the entire optical mode and restructures the intracavity field. In this companion paper to [1], we develop that treatment by extending the vacuum two-photon formalism to finite-thickness planar dielectrics, incorporating their Fresnel reflection, internal propagation, optical forces, and mechanical back-action directly into the field equations. We derive the carrier and sideband transfer functions needed to describe the coupled optical-mechanical system, including optomechanical cooling and the response to external perturbations. The result is a systematic starting point for calculating detector response and noise budgets for cavity experiments with intracavity dielectrics, including gravitational wave detectors deploying levitated sensors.
Abstract:Cavity optomechanical models typically treat a sensor either as a perturbative polarizable object in a pre-existing optical field, or solve the field at a fixed equilibrium and linearize in a fixed optical-mode basis. Neither self-consistently determines the spatially resolved cavity field, the optical force, the mechanical equilibrium, and the back-action when a finite-thickness dielectric plate intercepts the entire optical mode and restructures the intracavity field. In this companion paper to [1], we develop that treatment by extending the vacuum two-photon formalism to finite-thickness planar dielectrics, incorporating their Fresnel reflection, internal propagation, optical forces, and mechanical back-action directly into the field equations. We derive the carrier and sideband transfer functions needed to describe the coupled optical-mechanical system, including optomechanical cooling and the response to external perturbations. The result is a systematic starting point for calculating detector response and noise budgets for cavity experiments with intracavity dielectrics, including gravitational wave detectors deploying levitated sensors.
General Relativity and Quantum Cosmology (gr-qc); Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Optics (physics.optics); Quantum Physics (quant-ph)
arXiv:2610.17475 [gr-qc]
(or arXiv:2610.17475v1 [gr-qc] for this version)
https://doi.org/10.48550/arXiv.2610.17475 arXiv-issued DOI via DataCite (pending registration)
Full text under the publisher's open licence · 183 words
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