Ingenieurwissenschaften und zugeordnete Tätigkeiten
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For many years now, the so-called three layer model (free-surface, bulk-like, and adsorbed layers) has been commonly used, along with other parameters, to explain the deviations seen in glass transition and glassy dynamics for polymers confined into thin films, compared to their bulk value. Nevertheless, due to the hard accessibility of the adsorbed layers in supported films, little is known about the nature of their dynamics and how they really influences the overall dynamics of the thin films. Here, the irreversibly self-assembled adsorbed layer of a low MW Poly (vinyl methyl ether) (PVME) is solvent-leached from a 200 nm film. The thickness and topography of this layer is checked with Atomic Force Microscopy (AFM), to insure no dewetting and low roughness. Further, the dynamics of the adsorbed layer is then in-situ probed with Broadband Dielectric Spectroscopy (BDS). A recently developed nano-structured capacitor arrangement was employed; where a silicon wafer with nanostructured SiO2 nano-spacers, with heights of 35 nm, is placed on top of a thin film spin coated on an ultra-flat highly conductive silicon wafer. All results will be discussed in detail and quantitatively compared to our recent work on the glassy dynamics of PVME thin films (50 nm- 7nm), where BDS measurements showed two thickness-independent relaxation processes. The first process was assigned to the -relaxation of a bulk-like layer. Whereas the second process showed a different temperature dependence and was ascribed to the relaxation of polymer segments adsorbed at the substrate. To our knowledge, this is the first in-situ study of the dynamics of an irreversibly adsorbed layer.
Background: Gas sensors are very important in several fields like gas monitoring, safety and environmental applications. In this approach, a new gas sensing concept is investigated which combines the powerful adsorption probability of metal oxide conductive sensors (MOS) with an optical ellipsometric readout. This concept Shows promising results to solve the problems of cross sensitivity of the MOS concept.
Results: Undoped tin oxide (SnOx) and iron doped tin oxide (Fe:SnOx) thin add-on films were prepared by magnetron sputtering on the top of the actual surface plasmon resonance (SPR) sensing gold layer. The films were tested for their sensitivity to several gas species in the surface plasmon resonance enhanced (SPREE) gas measurement. It was found that the undoped tin oxide (SnOx) shows higher sensitivities to propane (C3H8) then to carbon monoxide (CO). By using Fe:SnOx, this relation is inverted. This behavior was explained by a change of the amount of binding sites for CO in the layer due to this iron doping. For hydrogen (H2) no such relation was found but the sensing ability was identical for both layer materials. This observation was related to a different sensing mechanism for H2 which is driven by the Diffusion into the layer instead of adsorption on the surface.
Conclusion: The gas sensing selectivity can be enhanced by tuning the properties of the thin film overcoating. A relation of the binding sites in the doped and undoped SnOx films and the gas sensing abilities for CO and C3H8 was found. This could open the path for optimized gas sensing devices with different coated SPREE sensors.
A combination of nanosized dielectric relaxation (BDS) and thermal spectroscopy (SHS) was utilized to characterize the dynamics of thin films of Poly(vinyl methyl ether) (PVME) (thicknesses: 7 nm – 160 nm). For the BDS measurements, a recently designed nano-structured electrode system is employed. A thin film is spin-coated on an ultra-flat highly conductive silicon wafer serving as the bottom electrode. As top electrode, a highly conductive wafer with non-conducting nanostructured SiO2 nano-spacers with heights of 35 nm or 70 nm is assembled on the bottom electrode. This procedure results in thin supported films with a free polymer/air interface. The BDS measurements show two relaxation processes, which are analyzed unambiguously for thicknesses smaller than 50 nm. The relaxation rates of both processes have different temperature dependencies. One process coincidences in its position and temperature dependence with the glassy dynamics of bulk PVME and is ascribed to the dynamic glass transition of a bulk-like layer in the middle of the film. The relaxation rates were found to be thickness independent as confirmed by SHS. Unexpectedly, the relaxation rates of the second process obey an Arrhenius-like temperature dependence. This process was not observed by SHS and was related to the constrained fluctuations in a layer, which is irreversibly adsorbed at the substrate with a heterogeneous structure. Its molecular fluctuations undergo a confinement effect resulting in the localization of the segmental dynamics. To our knowledge, this is the first report on the molecular dynamics of an adsorbed layer in thin films.