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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 1043-1048 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Metal-coated, nanometer-size particles are modeled with a realistic distribution of coating thicknesses. General expressions are given for the local-field enhancement, absorption, and nonlinear optical response. In addition, heuristic arguments are used to determine the effects of a diffuse, rather than a sharp interface. The linear and nonlinear optical properties are discussed within the context of the effective medium theory for small volume fractions. An efficient method of solution is used with the flexibility to handle an arbitrary number of coatings.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 3453-3457 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: High-energy synchrotron-radiation (SR) light was applied to the photochemical-vapor deposition of amorphous carbon films. The source gases of CH4 and H2 have been directly photodissociated by the ultraviolet SR light to deposit carbon films on the heated Si substrate. The film structure was characterized by field-emission scanning electron microscopy, Raman scattering, and infrared absorption, which indicate the film to be a rigid amorphous structure comprised of mostly sp3-bonded carbon. The advantage as well as the limitation of the synchrotron-radiation process to the synthesis of functional materials is discussed. © 1995 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 82 (1997), S. 2655-2661 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Amorphous SiO2 was deposited on three single-crystalline substrates: alumina, CaF2, and hydrogen-terminated silicon, by chemical vapor deposition (CVD) using tetraethoxysilane (TEOS) and ozone (O3). The deposited layers were then examined by using atomic force microscopy (AFM). For deposition times of 3, 8, 15, and 180 s, the film thickness ranged from less than 2.4 to 150 nm, respectively. Comparison of the surface roughness with the film thickness, as determined independently by ellipsometry, indicated that the thinnest film formed on the silicon surface (2.4 nm) was continuous. During film formation, for all three substrates, the surface roughness increased initially, reached a maximum, and then decreased. Surprisingly, the surface became smooth (within the resolution of 0.2 nm of our AFM). For the silicon substrate, this smoothing occurred between 3 and 8 s, which corresponds to 2.4 and 6.4 nm of deposition, respectively. Furthermore, just before the smoothing started, the surface of the deposited film contained protuberances, 1.6 nm high and 16 nm×16 nm in area. This indicates that smooth film of a few tens angstroms in thickness can form on the silicon. The smoothing of the protuberances occurred between 3 and 8 s for the CaF2 substrate, and between 15 to 180 s for the alumina substrate. The initial formation of a rough surface followed by smoothing is likely to be inherent in TEOS/O3 CVD systems, irrespective of substrate type. Surface-tension-induced flows of the surface, which has liquidlike properties, is a plausible mechanism. © 1997 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 82 (1997), S. 1404-1407 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Growth mechanisms of nanometer-sized particles prepared by rf sputtering on silica glass layers were examined. Gold and gallium arsenide (GaAs) particles synthesized with varying sputtering times on a SiO2 sputtered layer were subsequently buried in a SiO2 film by sputtering a SiO2 target. Transmission electron microscopy showed that in both cases, with increasing sputtering time, the number density decreased and the distance between neighboring particles increased in the initial stage of the growth, which suggests that the particles migrate on the SiO2 surface and coalesce with each other as they grow. Differences of GaAs and gold particle formation suggest that the mobility of the GaAs particles is much larger than that of gold. The results suggest that the migration of nanoparticles is activated by the bond-formation energy released during the incorporation of precursors into growing particles. © 1997 American Institute of Physics.
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  • 5
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Low pressure chemical vapor deposition (LPCVD) was carried out to deposit tungsten silicide films (WSix) from WF6 and SiH4 in a low temperature range from 80 to 390 °C, using a tubular reactor system. Drastic decrease of the deposition rate occurred at an extinction temperature Tex. Increase of the reactor size in the range from 4 to 22 mmφ decreased Tex from 140 to 80 °C. Above Tex, the sticking probability of the film forming species (η) and the film composition, x of WSix , did not depend on the reactor diameter. Dependence of Tex on the reactor diameter and independence of η and x above Tex from the reactor diameter indicates that a radical chain process dominates CVD-WSix process to form film forming species.
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  • 6
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 61 (1992), S. 2162-2163 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The temperature dependence of the electrical conductivity of a C60 single crystal is presented in this letter. The single-crystal samples free from solvent contamination were grown up to a size of millimeters order by sublimation of C60 powder with oscillation of the crystal temperature. The electrical conductivity of the single crystal was measured at temperatures between 250 and 295 K. The sharp decrease of the electrical conductivity with temperature around 256 K was observed in association with the phase transition of C60.
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  • 7
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 64 (1994), S. 1306-1308 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Diamond particles were deposited using a hot filament-assisted chemical vapor deposition (HFCVD) method in which the substrate temperature ranged from 210 to 700 °C. The size of the diamond particles measured as a function of time showed that a diamond grows via two periods of incubation and growth. Compared with an activation energy of 10–25 kcal/mol for substrate temperatures higher than 600 °C as reported in literature, the growth rate for a diamond grown using a HFCVD method was much less dependent on the substrate temperature for that temperature range investigated in our study. The apparent activation energy, determined from the Arrhenius plot of the substrate temperature versus diamond growth rate, decreased from 5 to 1 kcal/mol with decreasing temperature.
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  • 8
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 61 (1992), S. 764-765 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Tungsten silicide films (WSix) were deposited from WF6 and SiH4 by low pressure chemical vapor deposition (LPCVD) using a tubular reactor system. At the deposition temperature of 150 °C, films having low concentrations of residual fluorine (∼1.5×1021 cm−3) deposited quite conformally on micron-sized trenches. The sticking probability of the film precursor was determined from the step coverage quality, as a function of deposition temperature ranging from 120 to 390 °C. While the sticking probability remained constant above 270 °C, it changed with an activation energy of 7±2 kcal/mol in the temperature range 120–240 °C. The decreased probability of sticking improved the step coverage quality at low temperatures.
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  • 9
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 63 (1993), S. 3524-3526 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Chemical composition of the gas phase during the diamond growth by a hot-filament method was measured gaschromatographically for two different configurations with feed gas introduction, the conventional method from a nozzle equipped on a reactor wall and the jet feed from a hole bored in a substrate located just beneath the filament. CH4 and C2H2, diluted in H2, were used as a source gas. The results indicated that equilibration took place so rapidly near the filament that even the jet-feed mixture was converted to a thermodynamically stable composition composed mainly of C2H2, H, and H2. Insensitivity of the diamond process to the source hydrocarbon and its sensitivity to the filament-and-substrate configuration can be well interpreted.
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 59 (1991), S. 1473-1475 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Diamond films were deposited on the silicon wafer at as low a temperature as 135 °C by filament-assisted chemical vapor deposition. Silicon wafer substrate scratched with diamond powder was cooled by a stream of water flowing around a substrate holder. The films were identified as diamond by Raman spectroscopy. Clearly faceted crystals were shown in scanning electron micrographs.
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