integration of mid-IR resonators with 2D materials has been shown to enhance sensing performance. [14] For the practicality of these applications, it is often desirable to implement the platform with a simple and cost-effective optical configuration, using inexpensive light sources and photodetectors operating in the visible spectrum. The practical aspect of localized surface plasmon (LSP)-based sensing lies in the mode excitation that can be carried out in a microscope setting, in contrast to its integrated optics and surface plasmon polariton counterparts that require complex optical configurations to meet their phase-matching conditions. [15,16] The performance of a plasmon-based sensor is gauged by the sensitivity (S) and the figure of merit (FOM), with the former describing the susceptibility of the plasmonic confinement to the refractive index changes and the latter, dependent on the resonance Q factor, describing the sensing resolution. The sensitivity has been shown to increase linearly with the resonance wavelength (λ R ), that is, S∝λ R [17,18] indicating that sensitivity progressively decreases toward the visible frequency range. This presents a dilemma in the realization of practical and cost-effective sensing platform, where high sensitivity and high FOM are the desirable parameters for visible frequency operation.Various types of planar resonators, including split ring resonators (SRR), [19] nanorods, [20,21] crescents, [22] and pyramids [23] have been reported to have sensitivities of 100-300 nm per RIU and FOM of ≈2 in the visible frequency range. Higher sensitivity is achievable in self-assembled metal nanoparticles due to their lower damping loss and negligible interaction with the substrate. [24,25] However, such an approach is not preferable in the context of a practical sensing platform requiring precise control of nanoantenna dimensions and placements. Another approach for improving sensing parameters is through planar multi-cavity configurations that allow bright and dark modes to interfere and produce a narrow Fano resonance, [26][27][28][29] where the cancellation of radiative loss gives rise to linewidth reduction and consequently higher Q factors. Sensing based on Fano resonance has been reported with structures such as The nanoscale confinement of plasmonic fields, coupled with their high susceptibility to refractive index changes, makes localized surface plasmons (LSPs) an excellent platform for rapid and label-free sensing. However, the small spatial overlap of the LSP fields with the adsorbed analyte dictates the sensitivity and figure of merit (FOM) of LSP-based sensing. The linear dependence of sensitivity on resonance wavelength, coupled with the dependence of FOM on the achievable resonance Q factor, leads to a sensitivity of ≈100-300 nm per RIU and FOM < 5 for gold-based LSP resonance in the visible range. This presents a dilemma for the realization of a practical sensing platform that requires high sensitivity and high FOM in the visible spectrum. Higher sensitivity and reso...