Abstract

Advances in integrated photonics open up exciting opportunities for batch-fabricated optical sensors using high-quality-factor nanophotonic cavities to achieve ultrahigh sensitivities and bandwidths. The sensitivity improves with increasing optical power; however, localized absorption and heating within a micrometer-scale mode volume prominently distorts the cavity resonances and strongly couples the sensor response to thermal dynamics, limiting the sensitivity and hindering the measurement of broadband time-dependent signals. Here, we derive a frequency-dependent photonic sensor transfer function that accounts for thermo-optical dynamics and quantitatively describes the measured broadband optomechanical signal from an integrated photonic atomic force microscopy nanomechanical probe. Using this transfer function, the probe can be operated in the high optical power, strongly thermo-optically nonlinear regime, accurately measuring low- and intermediate-frequency components of a dynamic signal while reaching a sensitivity of 0.7 fm/Hz1/2 at high frequencies, an improvement of ≈10× relative to the best performance in the linear regime. Counterintuitively, we discover that a higher transduction gain and sensitivity are achieved with lower quality-factor optical modes for low signal frequencies. Not limited to optomechanical transducers, the derived transfer function is generally valid for describing the small-signal dynamic responses of a broad range of technologically important photonic sensors subject to the thermo-optical effect.

Highlights

  • The rapid development of integrated photonics and nanotechnology has enabled a wide range of nanophotonic sensors applicable for thermal[1,2], magnetic[3,4], gas[5,6], force[7], and displacement[8,9] sensing

  • The signal-to-noise ratio of nanophotonic sensors improves with increasing transduction gains achieved by increasing the optical power in the photonic cavity

  • Experimental setup The nanophotonic sensor under study is an optomechanical device consisting of a curved cantilever probe held in the nearfield of a microdisk optical cavity supporting whispering-gallery modes (WGMs)

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Summary

Introduction

The rapid development of integrated photonics and nanotechnology has enabled a wide range of nanophotonic sensors applicable for thermal[1,2], magnetic[3,4], gas[5,6], force[7], and displacement[8,9] sensing. High-quality factor (Q) nanophotonic cavities strongly enhance local light-matter interactions via their small optical mode volumes and extended photon lifetimes, enabling an unmatched combination of ultrahigh precision and ultrawide bandwidth for optical sensing in a variety of applications. This includes cavity-optomechanical onchip motion transduction[10,11], where, for example, a lowloss nanomechanical resonator has been combined with a high-finesse optical cavity for ultrafast nanoscale optomechanical atomic force microscopy (AFM)[12,13,14] and recently applied for the direct measurement of local chemical and thermal properties using photothermalinduced resonance (PTIR)[15].

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