Abstract:This paper investigates multicomponent gas adsorption at the active surface of plasmonic chemical sensors and shows that there are situations where transients in a single sensor element can be used for simultaneous detection of different gases in multicomponent mixtures. A general master equation set is provided, describing multicomponent adsorption. Analytical expressions for sorption rates are derived and high-accuracy simplified models are proposed. Expressions for adsorption rate constants and rates and fo… Show more
“…The proposed fractal architectures can be treated as a novel platform for multiple analyte SEIRA, which is a powerful biomedical analysis tool. 50,51 The quasi-3D nanochannels of the nanostructures in which volumetric enhancement of the electric field occurs can be potentially useful for such applications. Herein, because of the hybrid nature of the devices, we consider both purely plasmonic modes (D4′ and D1″) and the hybridized features (between D3′ and D4′ and between D3″ and D4″) and demonstrate their volumetric refractive index sensitivity in the reflection mode.…”
We
use a paradigmatic mathematic model known as
Sierpiński
fractal to reverse-engineer artificial nanostructures that can potentially
serve as plasmonic metasurfaces as well as nanogap electrodes. Herein,
we particularly demonstrate the possibility of obtaining multispectral
extraordinary optical transmission-like transmission peaks from fractal-inspired
geometries, which can preserve distinct spatial characteristics. To
achieve enhanced volumetric interaction and thermal responsiveness
within the framework, we consider a bilayer, quasi-three-dimensional
(3D) configuration that relies on the unique approach of combining
complementary and noncomplementary surfaces, while avoiding the need
for multilayer alignment on the nanoscale. We implement an improved
version of the model to (1) increase the volume of quasi-3D nanochannels
and enhance the lightening-rod effect of the metasurfaces, (2) harness
cross-coupling as a mechanism for achieving better sensitivity, and
(3) exploit optical magnetism for pushing the resonances to longer
wavelengths on a miniaturized platform. We further demonstrate vertical
coupling as an effective route for ultimate miniaturization of such
quasi-3D nanostructures. We report a wavelength shift up to 1666 nm/refractive
index unit and 2.5 nm/°C, implying the usefulness of the proposed
devices for applications such as dielectrophoretic sensing and nanothermodynamic
study of molecular reactions in the chemically active mid-IR spectrum.
“…The proposed fractal architectures can be treated as a novel platform for multiple analyte SEIRA, which is a powerful biomedical analysis tool. 50,51 The quasi-3D nanochannels of the nanostructures in which volumetric enhancement of the electric field occurs can be potentially useful for such applications. Herein, because of the hybrid nature of the devices, we consider both purely plasmonic modes (D4′ and D1″) and the hybridized features (between D3′ and D4′ and between D3″ and D4″) and demonstrate their volumetric refractive index sensitivity in the reflection mode.…”
We
use a paradigmatic mathematic model known as
Sierpiński
fractal to reverse-engineer artificial nanostructures that can potentially
serve as plasmonic metasurfaces as well as nanogap electrodes. Herein,
we particularly demonstrate the possibility of obtaining multispectral
extraordinary optical transmission-like transmission peaks from fractal-inspired
geometries, which can preserve distinct spatial characteristics. To
achieve enhanced volumetric interaction and thermal responsiveness
within the framework, we consider a bilayer, quasi-three-dimensional
(3D) configuration that relies on the unique approach of combining
complementary and noncomplementary surfaces, while avoiding the need
for multilayer alignment on the nanoscale. We implement an improved
version of the model to (1) increase the volume of quasi-3D nanochannels
and enhance the lightening-rod effect of the metasurfaces, (2) harness
cross-coupling as a mechanism for achieving better sensitivity, and
(3) exploit optical magnetism for pushing the resonances to longer
wavelengths on a miniaturized platform. We further demonstrate vertical
coupling as an effective route for ultimate miniaturization of such
quasi-3D nanostructures. We report a wavelength shift up to 1666 nm/refractive
index unit and 2.5 nm/°C, implying the usefulness of the proposed
devices for applications such as dielectrophoretic sensing and nanothermodynamic
study of molecular reactions in the chemically active mid-IR spectrum.
“…In the process of adsorption, different spacial orientations cause different numbers of occupied adsorption centers of the same gas species and in some cases may bond differently with different desorption energies. Consequently, the number of adsorption sites on the graphene surface cannot be modeled solely by using the information on the crystallographic structure of the surface as in the case of adsorption of small molecules on solid surfaces and it can not be modeled solely by using the information on the molecular structure and orientation, which is possible for modeling adsorption on homogeneous surfaces [13].…”
Section: Methodsmentioning
confidence: 99%
“…Analytical models of the rate constants for adsorption and desorption, based on the ideal gas theory, applicable to the gas adsorption on a homogeneous crystallographic surface, are presented in [13]. Apart from pressure, temperature, molar mass of the gas and its affinity towards the surface, the surface density of the adsorption sites on the surface and the desorption energy are needed for the calculation of the rate constants.…”
Surface density of adsorption sites on an adsorbent (including affinity-based sensors) is one of the basic input parameters in modeling of process kinetics in adsorption based devices. Yet, there is no simple expression suitable for fast calculations in current multiscale models. The published experimental data are often application-specific and related to the equilibrium surface density of adsorbate molecules. Based on the known density of adsorbed gas molecules and the surface coverage, both of these in equilibrium, we obtained an equation for the surface density of adsorption sites. We applied our analysis to the case of pristine graphene and thus estimated molecular dynamics of adsorption on it. The monolayer coverage was determined for various pressures and temperatures. The results are verified by comparison with literature data. The results may be applicable to modeling of the surface density of adsorption sites for gas adsorption on other homogeneous crystallographic surfaces. In addition to it, the obtained analytical expressions are suitable for training artificial neural networks determining the surface density of adsorption sites on a graphene surface based on the known binding energy, temperature, mass of adsorbate molecules and their affinity towards graphene. The latter is of interest for multiscale modelling.
“…24−27 In one theoretical model, the equation of the rate reaction for a single analyte could successfully be extended to account for an n VOCs mixture, assuming a single adsorbate molecule on one binding site. 26 Another theoretical model for evaluation of the AD noise in the microfluidic structure with biosensors operating in an n analytes environment could account for small fluctuations as a random process in the detection signal around the equilibrium. 27 To improve the GNP sensors and to enable quantitative measures for their reliability and sensitivity, a better and more comprehensive understanding of AD parameters is required.…”
Section: Introductionmentioning
confidence: 99%
“…Our results show that the AD parameters give quantitative measures of sensors’ reliability and sensitivity and can be extended for an n VOCs mixture, assuming a single VOC molecule per binding site. 26…”
We
herein provide quantitative measures of sensors’ reliability
and sensitivity as a function of the sensor’s capacity (maximum detection signal
or saturation state) in addition to other adsorption–desorption
parameters that define the detection signals toward volatile organic
compounds (VOCs). The measures we have developed show differentiation
between irregular dispersed points of sensors with low and high capacities.
We show that the sharpest capacity that separates between the two
types of distribution points, viz the reliability limit (RL), is tightly
linked with the desorption constant kd. Less sharp RLs give interpretations of other reliability indicators.
RL also provides information about the reliability of detecting signals
of VOCs for a given sensor and sensors for a particular VOC. We show
that sensors with high capacities are more reliable and sensitive
to detecting signals of VOCs than sensors with lower capacities.
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