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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 74 (1993), S. 6425-6426 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ultrathin organic films can be used in electronics for several applications. There are a few ways of preparation of such films and one is plasma polymerization. Traditionally, comparatively thick films, 100–1000 nm, are deposited by this method and studied. But, for electronic devices, 10 nm or thinner films are of great importance to any wet technique considered to be unsuitable for perfect layer formation. In this work we have deposited 2–10 nm scale ultrathin hydrocarbon films on silicon wafers. A capacitively coupled rf discharge was initiated in a short residence time box-type reactor in a uniform flow of an acetylene/argon mixture. The gas kinetic residence time in the plasma zone was limited to 5–70 ms to decrease synthesis of heavy gas phase products and to suppress particulate formation. Distribution of film thickness after the deposition was measured by an ellipsometer. The film surface topography was studied by an atomic force microscope that shows the films are smooth and pinhole free. Thus our preliminary results suggest that ultrathin uniform smooth organic films suitable for electronic applications can be deposited in a reproducible manner.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 68 (1990), S. 2528-2529 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Fresh surfaces of polycrystalline Al-49.2%Cu, Al, and In are fabricated in duffusion pump oil, and observed in situ using a scanning tunneling microscope. The current images reflect the atomic arrays on their surfaces. More clear images with atomic resolution are observable about 10 h later compared with those just after the fabrication. Atomic resolution images are observable in oil several days after, with increasing noise.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The Large Helical Device (LHD) experiments [O. Motojima, et al., Proceedings, 16th Conference on Fusion Energy, Montreal, 1996 (International Atomic Energy Agency, Vienna, 1997), Vol. 3, p. 437] have started this year after a successful eight-year construction and test period of the fully superconducting facility. LHD investigates a variety of physics issues on large scale heliotron plasmas (R=3.9 m, a=0.6 m), which stimulates efforts to explore currentless and disruption-free steady plasmas under an optimized configuration. A magnetic field mapping has demonstrated the nested and healthy structure of magnetic surfaces, which indicates the successful completion of the physical design and the effectiveness of engineering quality control during the fabrication. Heating by 3 MW of neutral beam injection (NBI) has produced plasmas with a fusion triple product of 8×1018 keV m−3 s at a magnetic field of 1.5 T. An electron temperature of 1.5 keV and an ion temperature of 1.4 keV have been achieved. The maximum stored energy has reached 0.22 MJ, which corresponds to 〈β〉=0.7%, with neither unexpected confinement deterioration nor visible magnetohydrodynamics (MHD) instabilities. Energy confinement times, reaching 0.17 s at the maximum, have shown a trend similar to the present scaling law derived from the existing medium sized helical devices, but enhanced by 50%. The knowledge on transport, MHD, divertor, and long pulse operation, etc., are now rapidly increasing, which implies the successful progress of physics experiments on helical currentless-toroidal plasmas. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 61 (1990), S. 3147-3147 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Several forbidden lines of titanium have recently become strong enough to be identified in ATF plasmas in the ultraviolet and in the visible. The increase in intensity has resulted from gettering of the vacuum vessel with titanium both to suppress light impurities and to control hydrogen recycling. Three orders of the forbidden Ti xiv line at 2117.1 A(ring) have been observed in vacuum, and the second and third orders have been observed in air using two different Czerny–Turner spectrometers. Doppler broadening of this line has been used to infer ion temperatures in the interior of ATF plasmas. These data supplement ion temperature measurements employing lines from carbon, nitrogen, and oxygen reported earlier [R. C. Isler et al., Nucl. Fusion 29, 1391 (1989)]. Tentative identifications of other forbidden lines such as Ti vii at 1938.4 A(ring), Ti xv at 2544.8 A(ring), Ti xvii at 3370.8 A(ring) and 3834.4 A(ring), and Ti xviii at 1778.1 A(ring) have also been made. Research was sponsored by the Office of Fusion Energy, U.S. Department of Energy, under contract DE-AC05-84OR21400 with Martin Marietta Energy Systems, Inc.
    Type of Medium: Electronic Resource
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  • 5
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Neutral beam injection heated discharges at the density limit in the Large Helical Device [O. Motojima, H. Yamada, A. Komori et al., Phys. Plasmas 6, 1843 (1999)] are terminated with asymmetric radiative collapse (ARC) exhibiting several properties in common with the MARFE (multifaceted asymmetric radiation from the edge) phenomenon: (1) A highly poloidally asymmetric radiation profile which is stronger on the inboard side. (2) This asymmetry is well correlated with the signal from the multichord interferometer. (3) Moreover, evidence from several diagnostics at different toroidal locations supports the possibility that ARC may be toroidally symmetric. However in contrast to MARFE, ARC is only observed in the period just prior to the quench of the plasma. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In neutral-beam-injection (NBI) heated plasmas of the Compact Helical System (CHS) heliotron/torsatron [K. Matsuoka et al., Plasma Physics and Controlled Nuclear Fusion Research, 1988 (International Atomic Energy Agency, Vienna, 1989), Vol. 2, p. 441], inward turbulent particle flux is observed at a particular radial location near the plasma edge. The observed reversal of the particle flux is connected to the change in the cross-phase between electron density and poloidal electric field fluctuations. This phenomenon is observed in the parameter regime of low collisionality at the electron temperature Te〉15 eV, electron density ne〈3×1018 m−3, which approximately corresponds to the effective collision frequency normalized by the transit frequency of a circulating particle ν*(approximately-less-than)1. The large inward particle flux ((approximately-greater-than)1×1020 m−2 s−1) correlates with the positive shear of the radial electric field Er′ ((approximately-greater-than)1×106 V m−2), but does not have clear correlation with the radial electric field Er and the curvature Er″. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 7
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The radial electric field is driven to positive value by off-axis second harmonic electron cyclotron heating (ECH) in the Compact Helical System [Plasma Physics and Controlled Nuclear Fusion Research 1988, Nice (International Atomic Energy Agency, Vienna, 1989), Vol. II, p. 411]. The observed positive electric field is associated with the outward particle flux enhanced with ECH. The enhanced particle flux triggered by the production of the electrons accelerated perpendicularly to the magnetic field with ECH results in the change of the electric field.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 78 (1995), S. 2242-2247 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Nanometer-thick hydrocarbon films were plasma polymerized in a rf pulse discharge in an acetylene/argon mixture and were mechanically patterned by the AFM (atomic force microscope). In addition a dc bias voltage was applied to the gold coated Si3N4 AFM tip. Depending on the experimental conditions, different patterns have been observed: mechanical indentation, electric charge, and material deposition. The viscous properties of the plasma deposited film affects the movement of the AFM tip while it is scanning the surface in a contact mode, and also affects the size and shape of the patterned area. Spikes of about 25–72 nm height and 60–200 nm width were formed from gold transferred from the newly mounted gold coated tips. The mechanism of gold deposition could be assigned to the Joule heating of the tip, resulting from the electric breakdown of underlying dielectric layers. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 58 (1985), S. 3185-3189 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: B–C–N–H thin films were deposited by plasma chemical-vapor deposition with an external capacitively coupled reactor at an rf frequency of 13.56 MHz. The films were formed from a gas mixture of B2H6 (5.25 vol % in N2), methane, and argon or nitrogen as carrier gases. The deposition was carried out at room temperature and without heating the substrate. The films were transparent in the range of 10 000–2000-A(ring) wavelengths. The Knoop microhardnesses were 1825–3324 kg/mm2 and the refractive index was 1.3–1.6. An extensive discussion of the effect of the deposition conditions on both microhardness and film composition is given. In addition, the interrelation between the microhardness and composition is illustrated.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Journal of neurochemistry 11 (1964), S. 0 
    ISSN: 1471-4159
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Medicine
    Notes: Gross and microscopic radioautographic observations have been made on the sequential distribution of 32P in the brain and spinal cord of the dog after intracisternal injection as orthophosphate.There appear to be two stages in the process of 32P incorporation into central nervous tissues. In the first, the phosphate in the CSF penetrates the central nervous tissue by diffusion. In the second, the phosphate is incorporated into various organic compounds in response to metabolic processes.The chronological changes in intraneuronal 32P localization indicate incorporation into cellular protein, RNA, DNA, and lipid and depend upon the turnover rate of 32P in these fractions.In the metabolism of phosphate the molecular layer of the cerebellum probably is involved only in rapid changes reflected by the acid-soluble fraction. The cellular layers in addition are concerned with slower processes such as incorporation into structural compounds.
    Type of Medium: Electronic Resource
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