2015
DOI: 10.1021/acsami.5b02901
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Real-Time Monitoring of Morphology and Optical Properties during Sputter Deposition for Tailoring Metal–Polymer Interfaces

Abstract: The reproducible low-cost fabrication of functional metal-polymer nanocomposites with tailored optoelectronic properties for advanced applications remains a major challenge in applied nanotechnology. To obtain full control over the nanostructural evolution at the metal-polymer interface and its impact on optoelectronic properties, we employed combined in situ time-resolved microfocus grazing incidence small angle X-ray scattering (μGISAXS) with in situ UV/vis specular reflectance spectroscopy (SRS) during sput… Show more

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Cited by 115 publications
(195 citation statements)
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“…Although the resulting values are up to 9 orders of magnitude larger than typical experimental values, the observed nucleation and coalescence of stable clusters is in accordance with the expected physical behavior and the wide-ranging agreement with experimental data for gold on polystyrene from Ref. [20] supports the significance of the results. Nevertheless, it presently remains difficult to perform benchmarks that go beyond comparisons with experimental results.…”
Section: Discussionsupporting
confidence: 87%
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“…Although the resulting values are up to 9 orders of magnitude larger than typical experimental values, the observed nucleation and coalescence of stable clusters is in accordance with the expected physical behavior and the wide-ranging agreement with experimental data for gold on polystyrene from Ref. [20] supports the significance of the results. Nevertheless, it presently remains difficult to perform benchmarks that go beyond comparisons with experimental results.…”
Section: Discussionsupporting
confidence: 87%
“…This method relies on the analysis of the angledependent intensity structure of scattered X-rays. Most cluster properties were obtained by projecting the scattered structures onto a geometrical model of uniform [20] and MD simulations with selected values for the re-evaporation probability, pre = 1 × 10 −4 , and the fraction of trapped Au particles, γ = 1 × 10 −2 . For deposited thicknesses δ less than about 2 nm, all quantities agree with experimental trends.…”
Section: B Experimental Methodsmentioning
confidence: 99%
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