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  • Articles: DFG German National Licenses  (103)
Source
  • Articles: DFG German National Licenses  (103)
Material
  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 637-646 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have studied the incorporation of heavily supersaturated C into Si using solid-phase epitaxy (SPE) of implanted amorphous layers. The strain in the Si1−xCx/Si heterostructures was measured using rocking curve x-ray diffraction. The microstructure and defect introduction were examined using ion channeling and transmission electron microscopy (TEM). The fraction of C located on substitutional lattice sites in the Si was monitored using Fourier transform infrared absorption spectroscopy and ion channeling at resonance energies. Carbon-depth profiles were monitored by secondary ion mass spectroscopy. The metastable solubility limit for the incorporation of C into Si by SPE was found to be 3.0–7.0×1020 atoms/cm3, which is over three orders of magnitude above the equilibrium solubility at the Si melting point. This limit was determined by the ability to regrow without the introduction of microtwins and stacking faults along {111} planes. We postulate the local bond deformation resulting from the atomic size difference between C and Si leads to the faceting of the amorphous–crystalline interface and allows defect introduction, thus limiting the C supersaturations achieved in Si by SPE. It was also found that the defect density in the regrown alloys could be reduced by higher SPE regrowth temperatures in rapid thermal anneal processing. © 1996 American Institute of Physics.
    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 75 (1994), S. 3959-3963 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Interdiffusion and reaction in Cu/PtSi/Si(100) structures have been investigated. During annealing Cu migrates across the intermediate PtSi layer and reacts with Si to form Cu silicides, with no indication of PtSi decomposition or a Cu-PtSi reaction. The diffusion of Cu through PtSi proceeds nonuniformly when PtSi is exposed to air before Cu deposition. Uniform transport is observed when the sample is prepared in situ without breaking vacuum. Cu silicides grow linearly with time, while the rates are independent of the thickness of the transport medium. The results indicate that Cu silicide formation is not controlled by Cu diffusion through the interposed PtSi layer.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 257-263 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The reaction kinetics of Ti films on SiO2 were investigated using Rutherford backscattering spectrometry, x-ray diffraction, Auger electron spectroscopy, and transmission electron microscopy. Consistent with earlier studies, the reaction results in the formation of a TiOw/Ti5Si3/SiO2 stack at temperatures in the range 700–820 °C. As the silicide layer grows, the concentration of O in TiOw increases, with the reaction ceasing at w∼1.2. In addition, the reaction rate depends on the initial Ti thickness, as thicker Ti films possess faster reaction rates. Applying current diffusion-controlled kinetic growth models, we find nominal agreement with our data at each thickness and predict activation energies in the range 3.0–3.4 eV. However, such a model is unable to account for either the Ti thickness dependence or the slowing and eventual cessation of silicide formation as the oxide composition approaches its limiting value. We implement a model which takes into account the reduction in the thermodynamic driving force for Ti5Si3 formation due to the incorporation of oxygen into the overlying Ti. This model predicts a silicide growth relationship of the form kt= (1/2)x2+ax2f∑∞n=3(1/n)(x/xf)n, with k independent of Ti thickness and given by k=k0 exp(−ΔE/kBT). The final Ti5Si3 thickness, xf, is determined by the initial Ti thickness, the stoichiometries of each phase formed and the final oxide composition. This model yields a more accurate fit to our data than if we assume parabolic growth since it predicts the eventual cessation of the reaction as x approaches xf. We find ΔE=2.9±0.1 eV. Our model also seems to explain the dependence on initial Ti thickness.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 5751-5762 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The interfacial reactions in the structures of Si/SiO2 (500 nm)/Ru (65 nm) (up to 950 °C) and Si/SiO2 (500 nm)/Ru (72 nm)/Al-0.8 wt % Si (630 nm) (up to 700 °C), were studied by Rutherford backscattering spectrometry, Auger electron spectroscopy, x-ray diffractometry, selected-area electron diffraction, energy-dispersive x-ray spectroscopy, scanning electron microscopy, and transmission electron microscopy. A thin film of Ru was stable on a SiO2 substrate up to 30 min in a vacuum anneal at 950 °C. In vacuum, a fast interfacial reaction between the Ru thin film and the Al-Si overlayer started between 550 and 575 °C, resulting in the formation of a Si/SiO2/ RuAl2/(Ru4Al13)Al-Si layer sequence. Similar to the reactions between Pt group metals and Al, the Ru/Al reaction is nonuniform. It is controlled by a nucleation mechanism and is accompanied by void formation. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 3656-3668 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have studied the thermal stability of Si1−yCy/Si (y=0.007 and 0.014) heterostructures formed by solid phase epitaxial regrowth of C implanted layers. The loss of substitutional C was monitored over a temperature range of 810–925 °C using Fourier transform infrared absorbance spectroscopy. Concurrent strain measurements were performed using rocking curve x-ray diffraction to correlate strain relaxation with the loss of substitutional C from the lattice. Loss of C from the lattice was initiated immediately without an incubation period, indicative of a low barrier to C clustering. The activation energy as calculated from a time to 50% completion analysis (3.3±5 eV) is near the activation energy for the diffusion of C in Si. Over the entire temperature range studied, annealing to complete loss of substitutional C resulted in the precipitation of C into β-SiC. The precipitates are nearly spherical with diameters of 2–4 nm. These precipitates have the same crystallographic orientation as the Si matrix but the interfaces between the Si and β-SiC precipitates are incoherent. During the initial stages of precipitation, however, C-rich clusters form which maintain coherency with the Si matrix so the biaxial strain in the heterostructure is partially retained.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 3936-3943 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Kinetics and electrical properties of solid-phase epitaxial regrown (SPEG) layers of Sb-implanted strained Si1−xGex alloys are reported. Two sets of Si1−xGex epilayers with compositions of x=0.08 and 0.18, molecular beam epitaxy grown on Si(100) substrates, were implanted at room temperature with Sb+ ions at an energy of 200 and 100 keV, respectively, and doses of 1014 and 1015 ions/cm2. A set of Si(100) samples was also implanted as a reference. The samples were annealed at temperatures of 525, 550, and 575 °C for durations between 5 s and 10 min. For the higher-dose Sb-implanted Si0.92Ge0.08 layer (1015 cm−2) ion backscattering measurements in the channeling mode show a decrease in the regrowth rate compared to Sb-implanted Si(100). The activation energy of the SPEG process for the Si0.92Ge0.08 alloy was 2.9±0.2 eV, higher than the value of 2.4±0.2 eV obtained for pure Si. For the alloy with 18% Ge the SPEG rate for the 1015 cm−2 dose was much smaller compared to the sample with 8% Ge. For the lower-dose implantation (1014 cm−2) the regrowth rates for Si0.92Ge0.08 and pure Si were very close, and the activation energies were 2.8±0.2 and 2.7±0.2, respectively. It was also found that the SPEG rate in a rapid thermal annealing was significantly higher than that for a sample heated in a conventional furnace.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Macromolecules 20 (1987), S. 513-518 
    ISSN: 1520-5835
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    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 65 (1989), S. 1957-1967 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Reactions of thin Co55 W45 films in contact with Si(100) substrates and aluminum overlayers annealed in vacuum in the temperature ranges of 625–700 °C and 500–600 °C, respectively, and of thin Co55W45 films in air from 500 to 600 °C were investigated by Rutherford backscattering spectrometry, glancing angle x-ray diffraction, and scanning electron microscope techniques. CoW alloy films were amorphous and have a crystallization temperature of 850 °C on SiO2 substrates. The compound formed is Co7 W6. Phase separations were found in all the reactions. A layer of cobalt compounds (CoSi2 in Si/CoW, Co2 Al9 in CoW/Al, and Co3 O4 in CoW with air) was found to form at the reaction interfaces. In addition, a layer of mainly tungsten compounds (WSi2 in Si/CoW, WAl12 in CoW/Al, and WO3 in CoW with air) was found next to cobalt compound layers, but further away from the reaction interfaces. The reactions started at temperatures comparable to those required for the formation of corresponding tungsten compounds.
    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 65 (1989), S. 300-304 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Pd50Ti50 and Pt50Ti50 alloy films were deposited on stainless-steel substrates and irradiated with ion beams. The samples were tested on pin-on-disk wear equipment and analyzed by Rutherford backscattering spectrometry and scanning and transmission electron microscopy. Adding Pd50Ti50 and Pt50Ti50 as a surface layer to stainless steel resulted in reduced wear and friction. Xe implantation slightly improved tribomechanical properties, while N implantation led to a dramatic reduction in wear and friction. The improvement was thought to be associated with nitride precipitation hardening and/or forming lubricious oxides during sliding. The as-deposited films exhibited amorphous structures and transformed to equilibrium compounds upon annealing. Sliding tests on amorphous and crystalline films did not show a significant difference in friction and wear behavior.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 4651-4654 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Direct, ion induced formation of metastable compounds in the Pt-Si system has been investigated by implantation with Xe ions through the PtSi-Si interface in the temperature range of 35–325 °C. The mixing increased parabolically with dose and exhibited an exponential dependence on reciprocal temperature with an apparent activation energy of about 0.11 eV. The mixed layer became progressively uniform in composition with increasing temperatures and a well-defined surface layer with a composition of Pt4Si9 was obtained at relatively high temperatures. The Pt4Si9 phase was indexed as a hexagonal crystal structure and transformed back into PtSi and Si at temperatures above 550 °C by thermal steady-state annealing.
    Type of Medium: Electronic Resource
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