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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 38 (1982), S. 55-61 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Convergent-beam electron diffraction (CBED) patterns contain diffracted beams from higher-order Laue zones (HOLZ), in addition to the more often observed diffracted beams from the zeroth-order reciprocal lattice zone (ZOLZ) that contains the origin of the reciprocal lattice. Since HOLZ diffraction vectors have non-zero components along the incident electron beam direction, they can detect components of static real-lattice displacement fields that lie along the incident electron beam direction, an event not possible for diffracted beams normal to the incident electron beam direction (i.e. ZOLZ diffracted beams). This effect is used in the present work to determine Burgers vectors of straight dislocations and loops in silicon from observations of splitting of HOLZ lines within the forward scattered beam Bragg disk, and from splitting of Kikuchi lines associated with HOLZ Bragg reflections. The method was also applied with limited success to dislocations in aluminum; here splitting was more difficult to observe because of the rather strong diffuse background in the CBED patterns. Calculations of HOLZ line splitting due to the presence of a dislocation in the irradiated crystal volume were in good qualitative agreement with the experimental observations. Effects on CBED patterns to be expected from some partial dislocations are discussed. This CBED method can be very useful for the determination of non-ZOLZ fault vector components in an atomic resolution structure-imaging microscope. These instruments usually have specimen tilt ranges limited to about 10°; thus conventional Burgers-vector analysis is not generally possible. Finally, the present CBED results show clearly that the projection approximation generally used to interpret structure fringe images is not strictly valid. the changes in fringe images or weak-beam images from HOLZ excitations remain to be evaluated.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 7422-7426 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The band structure of hexagonal boron nitride (BN) has been calculated using an ab initio linear combination of pseudoatomic-orbitals method. The calculated band structure confirms a previous finding that this material is an indirect band-gap insulator and has two empty interlayer bands. Projected densities of states are compared with the experimental x-ray emission spectra of B and N K edges and the agreement is good. This good agreement between the present ground-state calculation and the experimental x-ray emission spectra supports our previous finding that there should be very little valence electron relaxation effect on x-ray emission spectra. A real-space Green's function technique and the Z+1 approximation have been used to calculate the exciton spectra of B and N K edges. The first peak at 192 eV in B K edge is found to be a bound exciton with a binding energy of 1.7±0.4 eV. Only resonance is found for the N K edge. The calculated exciton spectra agree very well with the experimental quantum-yield and electron-energy-loss spectra.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 68 (1990), S. 288-290 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Various approximations in the calculations of electron energy-loss cross section and x-ray absorption coefficient have been evaluated using the Si L2,3 edge as an example. It was found that the random phase approximation, for which the cross terms are neglected in the expressions of electron energy-loss cross section and x-ray absorption coefficient, is a very good approximation. The dipole approximation in the calculation of the electron energy-loss cross section was found to begin to break down even at small acceptance half angles, such as 12.5 mrad. For energy losses larger than that of the Si L2,3 edge the dipole approximation will break down faster. This approximation also fails for a large scattering angle even at a small energy loss. The electron energy-loss cross section and x-ray absorption coefficient of the Si L2,3 edge has been calculated and compared. The large difference in relative intensity reported experimentally between the two spectra is not confirmed in this study. More experimental comparisons between electron energy loss and x-ray absorption spectra are recommended for Si and other compounds.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 65 (1989), S. 5217-5220 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A modified parametrization of the complete neglect of the differential overlap molecular orbital method is applied to energy-band calculations of solids. Results of the band calculation are used to calculate the near-edge fine-structure of core-shell electronic absorption edges in electron energy loss spectra. Preliminary application is made to silicon crystal.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 6328-6335 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Valence shell electronic excitations in silicon, and its carbide, nitride, and oxide are studied using electron energy loss microspectroscopy in a transmission electron microscope, at 1-eV resolution with a 100-keV electron beam. This so-called "low-loss'' region of the spectrum is normalized to scattering cross section per valence electron for each compound, and a large, sequential, variation in the cross section across the series of compounds is reported. The low-loss cross section is calculated using the Born approximation by including single-electron transitions in the target. Both band-to-band and band-to-continuum transitions are included, by using extended Hückel band calculations to obtain the valence shell crystal states, using the electron gas model for the ionization states, and using the random phase approximation to obtain differential cross sections. The calculations yield semiquantitative results, and allow for a chemical interpretation of the experimental results. The relation of the present model to that for plasmon excitation is also briefly discussed.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 62 (1987), S. 2439-2449 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Core-shell electronic absorption edges from thin specimens of silicon, α-silicon carbide, β-silicon nitride, and amorphous silica are studied by using electron-energy-loss spectroscopy in a transmission electron microscope. The elemental and chemical effects in the near-edge regions of the Si L2,3 and C, N, and O K edges are calculated by using some semiempirical models. The chemical effects in the region of the edges near-edge onset are due to valence-shell excited states, which we have modeled as linear combinations of atomic orbitals using the extended Hückel method, with the effects of translational periodicity in crystals included by using Bloch wave functions. Population analyses of valence-shell electronic structure and cross sections for bound→bound atomic transitions are used to interpret and calculate theoretical near-edge fine structure for direct comparison with experiment. The near-edge ionization region is calculated by using a plane-wave excited state to account for elemental effects. Chemical effects in the ionization region are accounted for by including contributions from the elastic backscattering of outgoing waves by the atoms that neighbor the excited atom. The elemental and chemical effects in the edges are shown to be separable to a large extent by using these models, and calculated cross sections are in good semiquantitative agreement with experimental results.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 58 (1985), S. 3463-3469 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Transmission electron energy loss spectra were obtained from small (approximately 100-A(ring) diam) regions of a series of single-phase silicon-containing specimens at 100-keV incident beam energy, using a field emission source transmission electron microscope fitted with a magnetic sector spectrometer. The specimen foils were diamond cubic silicon, α-silicon carbide, α-silicon nitride, and amorphous silica. The SiL near-edge structure depends markedly upon the chemical environment of the silicon. In this paper we show that the changes in near-L-edge structure, including threshold onset energy shift and edge profile, result from bond-induced changes in the valence shell electronic structure of the specimen materials. Extended Hückel molecular orbital theory was used to calculate the valence shell electronic structure of five-atom tetrahedral clusters, with silicon as the central atom and the other atoms noted above in corner positions. Inelastic electron scattering cross sections for silicon 2p and 2s core shell transitions to valence shell excited states were then calculated using the first Born approximation.
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  • 8
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 11 (1978), S. 564-568 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Two methods for performing small-angle electron scattering (SAES) experiments in transmission electron microscopes are described: the long-camera-length method and the selected-area-diffraction method. It is shown experimentally that angular resolutions of a few microradians and a few tenths of milliradians, respectively, are easily obtained by these two methods. A number of examples of the application of SAES to problems in materials science are presented. The use of new high-brightness electron sources is expected to produce significant increases in angular resolution, and the use of electron-energy analyzers will permit the separation of most of the inelastic contribution to the SAES intensity distribution.
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials synthesis and processing 6 (1998), S. 345-358 
    ISSN: 1573-4870
    Keywords: Ceramic interfaces ; metal/silicon carbide interfaces ; chemical interface width ; high resolution electron microscopy
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Instrumentation requirements, particularly for small probes, for high resolution analytical electron microscopy are described. Analysis of structure and chemistry of interfaces in conventionally processed Si3N4/SiC(w) ceramic matrix composites (CMCs) and metal/(0001) 6H-SiC single crystal substrates are presented. All of these interfaces are characterized by a chemical and a structural width. In the CMCs, which were processed at high temperatures, the chemical widths formed by diffusion of sintering aids into the bulk microstructure and were always much larger than the corresponding structural widths. The metals on SiC were deposited near room temperature, where diffusion is slow. Significant chemical widths did not form, and microstructure was determined by crystallographic factors. Upon annealing, reaction zones with appreciable chemical widths did form, with interesting morphologies that separated naturally into two groups. For metals that formed stable silicides and carbides, e.g. Ti, all interfaces in the reaction zones remained nearly atomically flat over large distances. For metals that formed only stable silicides interfaces in the reaction zones were often curved, and sometimes formed closed surfaces, for relatively low annealing temperatures, suggesting that interface melting had occurred even at temperatures less than expected for Si-metal eutectics.
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 25 (1990), S. 2943-2948 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Intragranular inclusions and multiphase regions at triple grain junctions in (B+C)-doped sintered α-SiC were investigated using analytical and high-resolution electron microscopy. Both regions were two-phase, composed of graphite and amorphous material. The triple junctions also contained pores. The amorphous regions were principally carbon and oxygen. Graphite was formed by partial transformation of the amorphous regions. Only the triple-junction regions contain typical impurities from the starting α-SiC powder, inferring that they are the main sinks for all grain-boundary/surface impurities in the material system.
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