2015
DOI: 10.1021/ph500461w
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Polymer Distributed Bragg Reflectors for Vapor Sensing

Abstract: We establish a new strategy to achieve fast and responsive hybrid distributed Bragg reflectors for environmental vapor sensing. We fabricated easily processable zinc oxide-polystyrene nanocomposites to grow high quality multilayers with large gas permeability and dielectric contrast, which enable fast and sensitive detection of vapor analytes. Multilayers fabricated by simple spin-coating of the nanocomposite and cellulose acetate show a 10-fold enhancement of the optical response to toluene exposure compared … Show more

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Cited by 101 publications
(155 citation statements)
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“…This interpretation is confirmed by theoretical calculation of the optical response (Fig. SI1 of Supporting Information), reproducing the spectra by using the complex refractive index of HB‐PVS reported in Figure 353 and CA for film thicknesses d HB‐PVS = 104 nm and d CA = 142 nm as input. The spectral tunability of the PBG can be obtained by changing the polymer concentration and/or the spinning velocity as shown in Supporting Information Fig.…”
Section: Resultssupporting
confidence: 79%
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“…This interpretation is confirmed by theoretical calculation of the optical response (Fig. SI1 of Supporting Information), reproducing the spectra by using the complex refractive index of HB‐PVS reported in Figure 353 and CA for film thicknesses d HB‐PVS = 104 nm and d CA = 142 nm as input. The spectral tunability of the PBG can be obtained by changing the polymer concentration and/or the spinning velocity as shown in Supporting Information Fig.…”
Section: Resultssupporting
confidence: 79%
“…The very good homogeneity combined with the very high reflectance intensity (measured above 70%, 76% calculated from eq ) is indicative of the quality of the prepared DBR. For this kind of structures, the presence of second order diffraction peaks is also expected, being an even tighter fingerprint of optical quality . In our samples, characterized by the principal PBG positioned around 760 nm, the second order is expected to be at λ PBG /2–380 nm, which is however resonant with electronic transitions in HB‐PVS, thus almost completely canceling it (except for a weak structure at 400 nm).…”
Section: Resultsmentioning
confidence: 62%
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