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  • 1
    Electronic Resource
    Electronic Resource
    Westerville, Ohio : American Ceramics Society
    Journal of the American Ceramic Society 86 (2003), S. 0 
    ISSN: 1551-2916
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: For the first time, a periodicity of 14 Å is recognized as a typical modulation period in metakaolinite. Energy-filtered electron diffraction data confirm that dehydroxylation does not occur abruptly in kaolinite. The degree of ordering becomes much lower during the progression of dehydroxylation in metakaolinite than in kaolinite. However, different types of modulations, with periods in the range from ∼1.4d001 (9.47 Å) to 2.9d001 (19.89 Å), form along the c*-axis in metakaolinite. Modules (14.2 Å= 2.1d001) that have a length that is approximately twice as long as the metakaolinite layer (6.86 Å) are the most common. Presumably, the remnant oxygens and vacant anion sites rearrange to acquire stability in the layer structure, which builds modulations along the c*-axis in the metakaolinite.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Westerville, Ohio : American Ceramics Society
    Journal of the American Ceramic Society 82 (1999), S. 0 
    ISSN: 1551-2916
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: The phase transformation from kaolinite to mullite was examined with new electron diffraction data obtained using an energy-filtering transmission electron microscope. Kaolinite was finally transformed to mullite and cristobalite through several steps of endothermic and exothermic reactions, which resulted in metakaolinite, a microcrystalline spinel-type phase and amorphous silica. Metakaolinite maintained its short-range order even at 920°C. The spinel-type phase resulted from a topotactic transformation of metakaolinite. Mullite first appeared at around 940°C, showing no clear crystallographic relationships to the parent metakaolinite structure. It coexisted with metakaolinite and the spinel-type phase produced previously. The first strong exothermic peak on the DTA curve was mainly due to the extraction of amorphous silica from metakaolinite and the gradual nucleation of the mullite phase. The initially formed spinel-type and mullite phases were suggested to be Al-rich, but to progressively gain Si in their structures at higher temperatures. The spinel-type phase decomposed completely through a second weak exothermic reaction, promoting the crystallization of cristobalite from amorphous silica, and the growth of mullite.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Westerville, Ohio : American Ceramics Society
    Journal of the American Ceramic Society 84 (2001), S. 0 
    ISSN: 1551-2916
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Both energy-filtered electron diffraction and EDS data clearly indicate extraction of amorphous silica from the parent metakaolinite by electron beam heating. Compared with the extracted silica through furnace heating, a larger population with inhomogeneous distribution and higher structural disorder of extracted silica by beam heating was noticed. There is a possibility that the spinel-type phase has lower symmetry than the suggested cubic symmetry, while the 〈111〉 orientation of the spinel-type phase is not perpendicular to the (001) plane of metakaolinite. HRTEM images of mullite crystals apparently demonstrate their random orientations with respect to the parent metakaolinite.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 22 (1995), S. 30-40 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract MX-1 tridymite is one of the room-temperature polymorphs of SiO2 tridymite and has an underlying monoclinic structure (Cc) with incommensurate modulations along a * and c * (Hoffmann et al. 1983; Löns and Hoffmann 1987). With increasing temperature up to 500° C, MX-1 is reported to experience at least five structural phase transitions. However, its structures and the relationships to other tridymite polymorphs are unclear. We present here a 29Si MAS NMR study of the room-temperature incommensurate structure of MX-1 and its structural phase transitions up to 540° C. Our results suggest that at room temperature, all the Si sites in MX-1 tridymite are in positions with similiar ∠Si-O-Si of ∼150° and are consistent with the presence of two incommensurate modulations proposed by Hoffmann et al. (1983). Simulations of the spectra yield modulation amplitudes of 1.33 and 0.87 ppm, corresponding to 0.009 and 0.006 Å for Si-Si. The maximum atomic displacements along a and b due to the modulations appear to be ∼0.01–0.02 Å. The structural phase transitions of MX-1 are significantly different from those of MC tridymite below 220° C. Our high temperature results confirm that MX-1 tridymite transforms to the H5 phase at about 65° C. The most important transition occurs near 110° C, where the H5 phase transforms to a phase yielding a single, narrow NMR peak, indicating the disappearance of the superstructure and possibly the onset of the dynamic averaging. The NMR lineshapes of H5 are consistent with the metrically orthorhombic unit cell and commensurate superstructure of 2a, 2b and 10c proposed by Graetsch and Flörke (1991). The phase present above 110° C is probably similar to the OC phase, but has a mean ∠Si-O-Si of ∼152.0° at 113° C, 152.9° at 185° C and 154.1° at 500° C. The transitions at ∼160 and 220° C for MX-1 are subtle and probably due to impurity MC. Analysis of the modulations in the OS phase of MC tridymite indicates that their amplitudes are of the order of 0.02 Å, significantly less than the value 0.3 Å proposed by Nukui et al. (1979).
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Advanced materials research Vol. 26-28 (Oct. 2007), p. 1097-1100 
    ISSN: 1662-8985
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Characteristic 60° dislocations occurred in hexagonal phase of Ge2Sb2Te5 thin foil cooledfrom 500°C to room temperature in a high voltage transmission electron microscope. The Burgersvector of dislocation was identified as 1/ 24 〈 9902 〉 which is the edge component of 1 3 〈 2110 〉projected on the (1120) lattice plane. The dislocation resulted from the cooling-induced stress/strainin the Ge2Sb2Te5 alloy
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Advanced materials research Vol. 26-28 (Oct. 2007), p. 1195-1198 
    ISSN: 1662-8985
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Transformation of uniformly strained GexSi1-x layers into GeSi dots of 3 ~ 7 nm which arecompositionally ordered by one or concurrently two sets of {111} planes was carried out for the firsttime under non-equilibrium conditions induced by 1.25 MeV electron irradiation at Tc ≥ 200 oC inthe high voltage electron microscope (JEM-ARM1300S). This microscope installed in the KBSI ischaracterized by an excellent point-to-point resolution of 0.12 nm allowing obtaining detailedinformation on chemical ordering at specific parameters of defocus (-800 Å) and crystal thickness(200~250 Å) determined by extensive HRTEM image simulation for the ordered dots
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Advanced materials research Vol. 26-28 (Oct. 2007), p. 1199-1202 
    ISSN: 1662-8985
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Phase transformation and crystal growth behavior of Ge2Sb2Te5 were investigatedsystematically by means of in situ heating (from room temperature to 500 oC) of amorphousGe2Sb2Te5 alloy in a high voltage electron microscope with real-time monitoring. Large-scalecrystallization occurred to amorphous Ge2Sb2Te5 around 200 oC. Large crystal growth developed onheating from 200 oC to 400 oC, and single crystalline grains grew up to 150 nm. Eventually the onsetof partial melting of thin Ge2Sb2Te5 foil was at 500 oC and liquid Ge2Sb2Te5 was observed for the firsttime by high-resolution transmission electron microscopy. Hexagonal Ge2Sb2Te5 phase remains aftera subsequent cooling
    Type of Medium: Electronic Resource
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