aiqbench analysis
This research demonstrates a versatile optomechanical platform capable of continuously tuning coupling ratios across three orders of magnitude, enabling seamless transitions between dissipation- and dispersion-dominated regimes. By utilizing a single experimental setup with adjustable mechanical resonators, the study provides a robust framework for investigating quantum effects in massive mechanical systems and advancing quantum-limited measurements. The ability to freely adjust these parameters represents a significant step toward more flexible quantum simulation and sensing architectures.
Optomechanical system with tunable dissipative and dispersive couplings
arXiv:2606.10318v1 Announce Type: new Abstract: We demonstrate an optomechanical system with tunable dissipative and dispersive couplings using a Fabry-Perot cavity and a string mechanical resonator. By varying the diameter and material of the mechanical resonator, and the relative location between the mechanical resonator and the cavity, the relative strengths of dissipative and dispersive coupling could be tuned continuously from dissipation-dominated regime to dispersion-dominated regime. In our experiments, the dissipative-to-dispersive coupling ratios of 1.3 and 0.6 are achieved by using two different mechanical resonators, corresponding to a transition from dissipation-dominated to dispersion-dominated optomechanical system. Theoretically, the coupling ratio could be tuned from 25 to 0.02 by optimizing the mechanical resonator, spanning over three orders of magnitude. These two distinct coupling regimes are achieved with the same experimental platform. The capability to freely adjust the coupling ratio provides a versatile platform for exploring quantum effects of massive mechanical resonators and quantum-limited measurements.
Abstract:We demonstrate an optomechanical system with tunable dissipative and dispersive couplings using a Fabry-Perot cavity and a string mechanical resonator. By varying the diameter and material of the mechanical resonator, and the relative location between the mechanical resonator and the cavity, the relative strengths of dissipative and dispersive coupling could be tuned continuously from dissipation-dominated regime to dispersion-dominated regime. In our experiments, the dissipative-to-dispersive coupling ratios of 1.3 and 0.6 are achieved by using two different mechanical resonators, corresponding to a transition from dissipation-dominated to dispersion-dominated optomechanical system. Theoretically, the coupling ratio could be tuned from 25 to 0.02 by optimizing the mechanical resonator, spanning over three orders of magnitude. These two distinct coupling regimes are achieved with the same experimental platform. The capability to freely adjust the coupling ratio provides a versatile platform for exploring quantum effects of massive mechanical resonators and quantum-limited measurements.
Quantum Physics (quant-ph); Optics (physics.optics)
arXiv:2606.10318 [quant-ph]
(or arXiv:2606.10318v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2606.10318 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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Full text under the publisher's open licence · 241 words
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