2017
DOI: 10.1021/acssensors.6b00696
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Crossed Surface Relief Gratings as Nanoplasmonic Biosensors

Abstract: We present an original, low-cost nanoplasmonic (bio)sensor based on crossed surface relief gratings (CSRGs) generated from orthogonally superimposed surface relief gratings (SRGs) on gold-coated azo-glass substrate. This surface plasmon resonance (SPR)-based sensing approach is unique, since the light transmitted through a CSRG is zero except in the narrow bandwidth where the SPR conversion occurs, enabling quantitative monitoring of only the plasmonic signal from biomolecular interactions in real time. We val… Show more

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Cited by 69 publications
(49 citation statements)
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“…According to the above bulk RI sensitivities ( S ) and standard deviations (σ), the bulk RI resolutions of the resonance dip at λ 1 (calculated as σ/ S ) at different incidence angles were calculated to be 2.13391 × 10 −4 RIU for θ = 0°; 1.33549 × 10 −4 RIU for θ = 10°; 1.46952 × 10 −4 RIU for θ = 20°; 3.52736 × 10 −4 RIU for θ = 30°; and 4.64362 × 10 −4 RIU for θ = 40°, as depicted in Figure S8f (Supporting Information). These sensing resolutions of the resonance dip at λ 1 were comparable to those of asymmetric ring/disk nanocavity, nanomushroom arrays, nanohole arrays, nanodisk arrays, crossed nanogratings, and nanocrosses, which in principle could be further improved by optimizing the optical detection system, such as by using a high spectral resolution optical spectrometer and a stable light source. As shown in Figure S8 (Supporting Information), the resonance dip at λ 1 exhibited the best sensing resolution at an incidence angle of 10°, other than at the normal incidence.…”
Section: Resultsmentioning
confidence: 79%
“…According to the above bulk RI sensitivities ( S ) and standard deviations (σ), the bulk RI resolutions of the resonance dip at λ 1 (calculated as σ/ S ) at different incidence angles were calculated to be 2.13391 × 10 −4 RIU for θ = 0°; 1.33549 × 10 −4 RIU for θ = 10°; 1.46952 × 10 −4 RIU for θ = 20°; 3.52736 × 10 −4 RIU for θ = 30°; and 4.64362 × 10 −4 RIU for θ = 40°, as depicted in Figure S8f (Supporting Information). These sensing resolutions of the resonance dip at λ 1 were comparable to those of asymmetric ring/disk nanocavity, nanomushroom arrays, nanohole arrays, nanodisk arrays, crossed nanogratings, and nanocrosses, which in principle could be further improved by optimizing the optical detection system, such as by using a high spectral resolution optical spectrometer and a stable light source. As shown in Figure S8 (Supporting Information), the resonance dip at λ 1 exhibited the best sensing resolution at an incidence angle of 10°, other than at the normal incidence.…”
Section: Resultsmentioning
confidence: 79%
“…The study of biological analytes through optical and nanophotonic structures (mainly metallic‐based ones) has been an actively developing research area for the last few decades . The operation principle of the vast majority of proposed biosensors is based on the dependence of the plasmonic resonance of metal NPs on their environment, where the NPs are hosted .…”
Section: Biosensing With Resonant Dielectric Nanoparticlesmentioning
confidence: 99%
“…We performed a biotin-streptavidin assay on these nanostructures to assess this potential. The gold was functionalized with cysteamine via its thiol group, followed by the oriented attachment of biotin-NHS to the cysteamine (as described in [33,34]). This platform was used for an assay of fluorescently-labeled (Cy3) streptavidin.…”
Section: Nanostructure Functionalizationmentioning
confidence: 99%