Optical microcavities are widely used as transducers for gas sensing, yet their performance is constrained by a natural trade-off between sensitivity and dynamic range. Here we introduce a laser-tagging optofluidic microcavity that overcomes this limitation, enabling hydrogen detection across a concentration range spanning from the single-molecule level to 1.53 × 105 ppm. The architecture features a hollow whispering-gallery-mode microcavity, functionally coated on its interior surface with a Pt/WO3 nanofilm. Gas detection is mediated via thermal phonon transfer, which allows efficient gas–material interaction without perturbing the optical field, preserving an ultrahigh intrinsic Q factor of 1.89 × 109 during sensing. Through so-called laser tagging, a probe laser is dynamically locked to the microcavity’s optimal operating point, enabling real-time resonance tracking. This scheme not only suppresses phase noise by more than three orders of magnitude but also facilitates wide-bandwidth optoelectronic heterodyne demodulation. We achieve hertz-level frequency-shift resolution and a measurable resonance shift of up to 1 GHz, allowing the sensor to detect hydrogen concentrations from 3 × 10−5 ppm to 1.53 × 105 ppm. With lock-in amplification, even individual molecular dynamics can be resolved. The device’s integrated, centimetre-scale footprint ensures robust operation outside the laboratory, offering a universal strategy to advance optical microcavities towards ultraprecise metrology applications. Laser tagging in an optofluidic microcavity enables precise hydrogen concentration detection across a broad dynamic range. Using thermal phonon transfer and dynamic resonance tracking, this spectrometry method achieves high sensitivity, low noise and effective selectivity.
Atmospheric methane (CH4) monitoring requires an optimal balance between ultra-high sensitivity and mechanical field-readiness. Conventional multi-pass architectures, such as Herriott cells, are fundamentally constrained by rigid geometries and alignment sensitivities that limit real-time optimization capability. To ov...
Single-fiber photoacoustic spectroscopy is attractive for compact, remote, and intrinsically safe trace-gas sensing, but its sensitivity is limited by the short absorption length and weak photoacoustic excitation in a miniaturized sensing head. Here, we propose and demonstrate an ultrasensitive single-fiber Fabry–Pé...
Refractive index (RI) sensors are indispensable for label-free biochemical analysis, environmental monitoring, and food safety. However, conventional optical sensors fundamentally rely on weak evanescent fields for analyte interaction, creating a persistent sensitivity bottleneck. Here, we overcome this limitation by i...
We report an elastic Fabry-Pérot microcavity (μFP) acoustic transducer that combines mechanical compliance with resonantly enhanced optical interrogation, boosting the conversion of pressure-induced diaphragm displacement into an optical signal. The transducer comprises a high-reflectivity concave mirror fabricated on...
We report a fiber-optic tuning-fork–cantilever coupled photoacoustic
(TFCC-PA) sensor for the simultaneous detection of methane
(CH
4
) and acetylene (C
2
H
2
). The
sensor integrates a custom square-head 6063 aluminum-alloy tuning fork
(ATF) and a laser-cut polyethylene terephthalate cantilever within a
s...
Fiber-optic ultrasound sensors hold considerable promise for diverse applications, benefiting from their high sensitivity and advantageous physical characteristics. However, their practical adoption is often hindered by the operational instability of conventional high-speed demodulation techniques, which rely on si...
Wei-Xuan Luo, Bai-Qing Nan, Wei-Jia Bao et al.· Photonic Sensors· 0 citations
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