3,016 research outputs found

    Author Correction: Casimir forces exerted by epsilon-near-zero hyperbolic materials (Scientific Reports, (2020), 10, 1, (16831), 10.1038/s41598-020-73995-0)

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    In the original version of this Article, Igor S. Nefedov was incorrectly affiliated with “Saratov State University, Astrakhanskaya 83, Saratov, Russian Federation, 410012”. The correct affiliation is listed below: Peoples’ Friendship University of Russia (RUDN University), 6 Miklukho-Maklaya St., Moscow 117198, Russia. This error has now been corrected in the HTML and PDF versions of the Article. © 2020, The Author(s)

    PKE–Nefedov*: plasma crystal experiments on the International Space Station

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    Abstract. The plasma crystal experiment PKE–Nefedov, the first basic science experiment on the International Space Station (ISS), was installed in February 2001 by the first permanent crew. It is designed for long-term investigations of complex plasmas under microgravity conditions. ‘Complex plasmas ’ contain ions, electrons, neutrals and small solid particles—normally in the micrometre range. These microparticles obtain thousands of elementary charges and interact with each other via a ‘screened ’ Coulomb potential. Complex plasmas are of special interest, because they can form liquid and crystalline states (Thoma

    Real time investigation of the initial stages of a-C films growth

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    a-C films were deposited by rf-PACVD. Their growth rate, thickness, density and roughness were derived during deposition from time dependent X-ray reflectivity (XRR) at a wavelength of 1.54 A and at a fixed incidence angle of 18. It is shown that the film density and surface roughness are not constant at the initial stages of growth. The density increases with increasing film thickness, while the surface roughness depends on the substrate roughness. The evolution of these parameters was measured also while etching the film in oxygen plasma and revealed the smoothing effect brought about by etching to the carbon surfac

    A study of capacitance-voltage characteristics of amorphous carbon multilayer nanostructures

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    Dark and illuminated capacitance–voltage (C–V) characteristics and admittance measurements were carried out on multilayer carbon structures.The latter were produced by depositing ultrathin amorphous carbon layers with different optical band gaps on a monocrystalline boron-doped silicon substrate.The carbon layers were grown either by magnetron sputtering (MS) of a graphite target in argon or by plasma ion beam deposition (IBD) in cyclohexane.The structures were characterised by X-ray reflectivity (XRR). With respect to their electrical properties, it was shown that light strongly affects both the C–V-characteristics and the admittance.The results were interpreted in terms of the energy levels in these amorphous carbon multilayer structure

    X-ray reflectivity study of the early stages of a-C:H film growth

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    The initial stages of hydrogenated amorphous carbon films growth are investigated by in situ and ex situ X-ray reflectivity (XRR) at a wavelength of 1.54 Å. Hydrogenated amorphous carbon films were deposited by rf-plasma-assisted chemical vapor deposition. The results are considered in connection with the main models of film growth, namely, layer-by-layer or island (hemispherical, cylindrical) formation. It is shown that the film density increases at the initial stages of growth and different possible reasons for this are discusse

    Iodine incorporation into polymeric films investigated by angle-resolved XPS

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    Distribution of elements into subsurface layers (up to 120 angstrom thickness) of polyphenylacetylene (PPA) films doped with I2 vapour has been determined by X-ray photoelectron spectroscopy data using a unique numerical technique. Concentration of incorporated iodine has been shown to increase with exposure time; the concentration profiles are dome-shaped and iodine does not penetrate much into the bulk of PPA films, even when exposed to I2 vapours for 1 h. The depth of the layer corresponding to maximum iodine concentration is directly proportional to the iodine exposure time. The non-homogeneous distribution of the doping species in the polymer may be responsible for the low conductivity observed for heterogeneously doped PPA films
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