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  • American Meteorological Society
  • International Union of Crystallography (IUCr)
  • 1990-1994  (12,744)
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  • 101
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 149-155 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: High-resolution powder diffraction coupled with the total-pattern-fitting technique revealed unusual and hitherto unreported diffraction effects for samples of copper(II) oxide. Data were obtained with a conventional diffractometer and strictly monochromatic Cu Kα1 radiation and also with the Daresbury Laboratory synchrotron source (9.1 HRPD). It was found that most lines are skewed, by varying amounts, towards higher or lower angles and there is a small amount of line broadening, which is mainly order dependent. It is shown that the line profile asymmetry varies systematically throughout reciprocal space and that the magnitude of the effect is sample dependent. No significant peak displacements were detected, but the skewing of lines is consistent with a distribution in the dimensions of the unit cell and hence Cu—O bond lengths.
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  • 102
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 146-148 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: It is shown that Laue diffraction patterns may be obtained from a protein crystal using the continuous radiation emitted by a tungsten sealed-tube X-ray source and that precise structure amplitudes may be extracted from these patterns.
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  • 103
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 178-183 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Multiple-crystal diffraction profiles and multiple-crystal topography have been combined to characterize semiconductor materials. X-ray topographs have been measured on the same region of the sample as the diffraction profiles and diffraction space maps, by insetting a film cassette in the diffracted beam path of a high-resolution diffractometer. This has proved to be a very powerful combination for providing a deeper understanding of the structural features that give rise to the high-resolution diffraction profiles. The data collection mode is discussed and the problems associated with interpreting `rocking curves' of imperfect materials. The misorientation and nature of the mosaic blocks in semi-insulating GaAs have been revealed by this method.
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  • 104
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 187-189 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A function for finding the voids in a crystal structure by means of a single Fourier synthesis is described. The function handles the atoms as spheres with known radius and supplies, for each grid point of the Fourier map, the volumetric fraction of the search atom centered at this point that interpenetrates the neighbouring atoms. In this way, the time-consuming calculation of distances is avoided. Its application to a solid-state ionic conductor is shown.
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  • 105
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 196-196 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
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  • 106
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 239-242 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: If thermal-expansion-tensor components αij are determined from temperature-induced changes in d values, most authors first calculate the unit-cell parameters at different temperatures. From these, the αij are computed. It is shown that this procedure involves a reduced precision if compared with the direct least-squares determination of αij from changes in the d values.
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  • 107
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 261-262 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A practical equation is presented to determine the deadtime τd in conventional X-ray counting systems when the amount of deadtime is greater than that which can be accounted for by non-extended deadtime theory. The use of this equation to determine the deadtime increases the practical range over which conventional X-ray detection systems can be used.
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  • 108
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 263-263 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
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  • 109
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 265-266 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
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  • 110
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 304-311 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The contrast of dislocation images in X-ray section topographs of curved crystals has been investigated both experimentally and by computer simulation. Good agreement is found between experiment and simulation in both symmetric and asymmetric Laue geometries. Very little change is observed in the symmetric Laue images for radii of curvature as small as 18 m. In the asymmetric geometry, the background intensity rises and the Kato fringe visibility decreases as the curvature increases. The dynamical image becomes more localized and dominates the image as the direct image visibility falls. Our results explain the reversal of dislocation contrast in Lang projection topographs of curved crystals taken in asymmetric geometry.
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  • 111
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 331-339 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The orientation contrast at the head of slip bands at a grain boundary was studied by a modified Schulz technique. The images on the topographs were simulated using kinematical intensity calculations. The stress field of the macrodislocation, which represents the head of the slip band, includes the surface stress relaxation. The Burgers vectors of the macrodislocations were determined.
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  • 112
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 355-364 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A crystallographic orientation analysis to study heterogeneous polycrystalline samples is reported. A specific arrangement was realised to explore the total surface of large wafers or ribbons without destructive sampling. The surface texture is determined by X-ray diffraction using reflection geometry. Approximate size and orientation of crystallites at the sample surface are evaluated from a method taking iterative comparisons of intensities as a basis. For each explored (hkl) pole, two intensities are measured by reflection on the surface element studied: the first when the reflective surface is fixed at the (hkl) Bragg angle; the second when the surface is rocked around this position. The same measurements, obtained from an even surface of (hkl) monocrystals, provide calibration curves. Generally the exploration of five or six different (hkl) poles is enough to obtain a valid description of polycrystalline silicon materials elaborated for photovoltaic conversion.
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  • 113
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 403-404 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The spatial intensity profile of an X-ray beam reflected by a crystal with microdefects in the Bragg case is considered. A practically pure diffuse component was measured at the tail of the intensity distribution. From these data, static Debye–Waller factors of nearly perfect silicon crystals were obtained.
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  • 114
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 413-413 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
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  • 115
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 444-456 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The use of X-ray and neutron small-angle scattering in the study of microstructural changes in inorganic materials is reviewed, with emphasis on recent developments. In the kinetics of diffusion-controlled phase separation, reliable data on the evolution of size and shape of the decomposition products may be obtained especially from in situ ageing experiments. Magnetic neutron scattering is discussed for inhomogeneous ferromagnets. While for the structural characterization of binary systems single-wavelength experiments are sufficient, variable X-ray wavelengths now available at synchrotron-radiation facilities open possibilities for the study of partial structure functions in systems containing several components. The combined use of small-angle scattering and complementary techniques is of particular value in more complex cases. These points are illustrated by a survey of recent results on phase separation and precipitates in binary and ternary crystalline alloys and on radiation-induced microstructural changes in metallic and semiconducting materials.
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  • 116
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 457-466 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Structure self-assembling in the spinodal decomposition (SD) of polymer blends in its late stage has been explored for a near-critical mixture of polybutadiene and polyisoprene by a time-resolved light scattering technique, with a particular emphasis on the time evolution of the interface structure. By analysis of a scaled structure factor F(x, t) ≡ I(q, t)qm(t)3 over wide ranges of a reduced scattering vector x ≡ q/qm(t) and time, it was found relevant to divide the late stage of SD into two stages, I and II. Here, I(q, t) denotes the scattered intensity as a function of the scattering vector q and time t. In the intermediate stage preceding the late one, F(x, t) became sharper with its peak at x = 1 increasing with t. However, as time elapsed, F(x, t) turned out to be universal for t, first in the range of x smaller than about 2 and then over the entire range of x accessible by the present experiment. The time interval in which the former occurred is defined as late stage I and the one in which the latter was realised is called late stage II. In late stage I, the average thickness of phase-phase interfaces decreases towards an equilibrium value and the time evolution of the interfacial area density Σ(t) does not scale with qm(t), i.e. the exponents γ and α in the power laws Σ(t) ̃t−γand qm(t) ̃t−α do not coincide (actually, α 〈 γ). Late stage II corresponds to the process in which these exponents become equal and the interface thickness reaches equilibrium. Such conditions probably ensure the establishment of a complete dynamical scaling law in the SD process.
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  • 117
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 526-530 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The wavelet transform has recently received much attention in the fractals world due to its ability to characterize the scaling properties of multifractal aggregates. This paper is devoted to the optical version of the wavelet transform, with a special emphasis on instrumental aspects. The optical wavelet transform amounts to a series of distinct bandpass filterings of the optical Fourier spectrum of the system under study. One wavelet component is given by one filtered image of the system. The way in which the intensity at any point depends on the filter size directly gives the local scaling behavior around this point.
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  • 118
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 555-561 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A triple-axis diffractometer has been constructed and optimized in our laboratory. It is used on an X-ray point source, using the principle which was pioneered by Bonse and Hart 25 years ago. A triple-reflection channel-cut Ge crystal is used as monochromator and the same as analyser. The width of the direct beam is about FWHM = 17′′ for Cu Kα radiation. Owing to the low background, the stability of the mechanics and the two triple Ge reflections, a signal-to-noise ratio of 107 has been achieved between the direct beam and the parasitic scattering without sample. These characteristics allow routine measurement of scattering to be performed for Bragg spacings up to 6000 Å for typical colloidal samples in semilinear collimation.
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  • 119
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 568-570 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A brief description and characterization is given of the three small-angle neutron scattering instruments (SANS) in the new guide laboratory at the Jülich FRJ-2 reactor, namely two 40 m slit-collimation instruments and a very high-resolution double-crystal diffractometer. The combination of the two instruments allows one to cover a range of scattering vectors Q of nearly four orders of magnitude.
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  • 120
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 593-597 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: In the last decades, the kinetics of phase separation following a quench into the miscibility gap have been studied in a variety of systems by small-angle scattering techniques. A scaling behavior in the late stages of coarsening, first observed in computer simulations, was found to be a `universal' feature of the small-angle scattering intensity S(k,t) with S(k,t) = S[km(t),t]F[k/km(t)], where km(t) is the value of the modulus k of the scattering vector at which S(k,t) has its maximum. Furthermore, it was observed recently that, for many systems ranging from liquid and polymer mixtures to solid alloys and computer simulation models, the scaling function F(x) does not change appreciably from one system to another when the volume fraction is kept constant. This paper first reviews work carried out jointly with J. L. Lebowitz and O. Penrose, discussing various features of the scaling function F leading to a simple analytical expression suitable to fit experimental data. New small-angle X-ray scattering results on the shape of the scaling function for dilute Al–Ag and Cu–Fe systems are then presented and compared with the predictions of the model.
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  • 121
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    Applied crystallography online 24 (1991), S. 635-637 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A series of active C atoms was prepared by combination of activation (by steam, at 1173 K) and by heat treatment (at 1523 K, 2 h under nitrogen) and the structures of the samples were investigated by gas adsorption (nitrogen adsorption isotherms) and by X-ray scattering. An agreement is observed between the average chord length of segments in the solid phase measured by SAXS and the average micropore size determined by gas adsorption, suggesting that the diameters of micropores formed during the activation and the heat treatment have nearly the same size as the crystallites.
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  • 122
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 659-664 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Surprisingly, molecular weight can be determined from small-angle scattering data without using absolute intensities and the contrast factor. The formula underlying this novel procedure is illustrated by model calculations. Several examples of the successful use of the procedure applied to polymer solutions together with those where the method has failed are given.
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  • 123
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    Applied crystallography online 24 (1991), S. 692-701 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Five interpenetrating polymer network (IPN) epoxy-acrylate samples of the same composition synthesized with variable conditions – temperature and initiator rate – were studied by small-angle X-ray scattering (SAXS). The scattering curves, at first sight showing little detail, were meticulously analysed. The entire scattering curve of an IPN compound was analysed using new methods for background subtraction and desmearing. The treatment suggests a fractal behaviour of the internal surface, associated with this two-phase system, on a scale between 100 and 10 nm and, in the tail end of the SAXS curves, reveals maxima corresponding to those of two regular spheres with radii of the order of 7 and 14 nm. Analysis of the beginning of the curves yields one or two correlation lengths according to the conditions of the synthesis, close to 100 and 20 nm. These results are consistent with the general model of IPN structures as revealed by other physico-chemical techniques.
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  • 124
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 24 (1991), S. 709-711 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Aramid fibres show elongated microvoids parallel to the direction of the fibre axis, resulting in an equatorial streak in the small-angle X-ray scattering (SAXS) pattern. The scattered intensity in the equatorial direction has been measured for three samples of the same fibre: an untreated yarn specimen, yarn in which Ag2S was precipitated and a single filament of the latter. In the case of the untreated yarn, the interpretation of the SAXS pattern is hindered by the presence of residual water in the voids, resulting in a three-phase system. The SAXS pattern of the yarn with precipitated Ag2S follows the theoretical pattern (adapted for the two-dimensional case) for a system with random pores, but the interface between aramid and Ag2S shows fractal properties. The single filament with Ag2S shows a SAXS pattern analogous to that of the fibre with Ag2S, indicating that multiple scattering and interfilament scattering is negligible. It was also found that the Ag2S precipitates in the fibre with preferred orientation.
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  • 125
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    Applied crystallography online 24 (1991), S. 732-739 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Calcium carbonate dispersions stabilized by an adsorbed surfactant layer are used to regulate the acidity of lubricating oils for internal combustion engines. Three typical commercial samples have been examined using a combination of X-ray and neutron scattering techniques. The solid active material was extracted from the samples and redispersed in heptane and mixtures of toluene and toluene-d8 and n-octane and n-octane-d18. The results were in broad agreement with the core/shell model proposed by Ottewill [Markovic, Ottewill, Cebula, Field & Marsh (1984). Colloid Polym. Sci. 262, 648–656]. The core radius ( ̃12–28 Å) was obtained from SAXS data. The polydispersity was about 25% on all samples and the distribution skewed to larger sizes. The hydrogenated-solvent SANS data were too weak to be used to determine the core size. The total particle radius ( ̃20–50 Å) and hence the shell thickness were obtained by model fitting to the deuterated-solvent and 65% deuterated-solvent SANS data with the core radius from the X-ray data. In determining the best fit, the core density, amount of solvent in the shell and polydispersity were also adjusted to give fits with a shell-to-core-volume ratio and a volume fraction that agreed with the expected values. The SANS data were weaker than expected assuming a simple monodisperse core/shell model with a calcite core. This is consistent with the observed polydispersity and in addition implies diffuse boundaries. Although WAXS (wide-angle X-ray scattering) confirmed that the cores were non-crystalline the best model fits were obtained with a core scattering density not much less than that calculated for calcite. The absolute intensities suggested that some solvent was incorporated into the shells of all the samples and one sample showed a preference for uptake of octane as compared to toluene.
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  • 126
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    Applied crystallography online 24 (1991), S. 759-764 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The influence of pH, cations, F− and temperature on the aggregation, gelation and ageing of aqueous silica gels has been investigated using small-angle X-ray scattering (SAXS). At both low and intermediate pH (pH = 4 and 6–8, respectively), fractal aggregates are formed during gelation from silicic monomers or small oligomers. The fractal dimensionality is 2.20 (5), to be expected for reaction-limited cluster–cluster aggregates. During ageing silicic ions dissolve from the more soluble peripheral primary particles and condense in the crevices of the core of the aggregates. This process results in an increase in the size of the scattering primary particles and in a decrease in the fractal dimensionality of the silica aggregates from D = 2.25 to D = 2.0 or D = 1.85. The ageing processes are strongly enhanced by a slight increase in the pH of the solution, addition of fluorine anions and a rise in temperature. The aged silica gel is constructed of an ensemble of densified aggregates of which the density variation within the aggregates is larger than that of the freshly prepared aggregates. The primary particles of which the aggregates are built grow during ageing from molecular size to dense particles in the nanometer range, the ultimate radius depending on the type and duration of the ageing process.
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  • 127
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    Applied crystallography online 24 (1991), S. 815-821 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Structural information of clathrin-coated vesicles has been achieved by small-angle X-ray, neutron and dynamic light scattering studies. A characteristic peak in the X-ray and neutron scattering profile (in D2O) from intact coated vesicles is consistent with the polygonic structure of the clathrin coat. Neutron as well as dynamic light scattering gives a coated vesicle size close to 1000 Å. Dynamic light scattering detects a distribution of sizes for the coated vesicles demonstrating polydispersity of the samples. Quick freezing and slow thawing cause breakdown of the polygonic coat and production of large aggregates, as observed by dynamic light scattering and the reduction of the peak in the X-ray scattering profile as well as an increase in the scattering intensity at the lowest angles in the neutron scattering profile.
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  • 128
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    Applied crystallography online 24 (1991), S. 836-842 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A new experimental technique to investigate the structural rearrangements associated with thermal phase transitions of phospholipids is outlined. The method utilizes the changes in small-angle X-ray powder diffraction patterns, monitored with a time resolution of down to 1 ms, following fast temperature jumps of about 10 K height in 1–2 ms. This heating rate, effected by an erbium infrared laser pulse, provides a synchronous disequilibration of the lipid samples and the ensuing structural relaxation processes are observed by using the high-flux X-ray beam from a synchrotron source in combination with a rapid position-sensitive-detection and data-acquisition system. For the two symmetry heterologous phase transitions, the lamellar (Lβ')-to-monoclinic (Pβ') `pretransition' of synthetic phosphatidylcholines and the lamellar (Lα)-to-inverted hexagonal (HII) transition of phosphatidylethanolamines, this method provides the first evidence for the existence of transient intermediate ordered structures. In the pretransition, the first step is the rapid (〈 2 ms) formation of a second lamellar lattice, with a decreased repeat distance, which coexists for up to about 100 ms with the original Lβ' lattice. In a second, slower process, these two lattices merge and transform to the Pβ' structure within several seconds. In the Lα–HII transition, the first rapid step (τ ̃5 ms) consists of a uniform shrinkage of the lamellar lattice; this is followed after about 20 ms by the first appearance of a distorted hexagonal lattice and a slow transformation into the final HII lattice. Comparison of these results with X-ray diffraction data obtained under near-equilibrium conditions, where these intermediates cannot be detected, shows that the systems respond to the high thermodynamic driving force which exists under non-linear non-equilibrium conditions by formation of correlated intermediate structures which provide efficient pathways for relaxation.
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  • 129
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    Applied crystallography online 24 (1991), S. 874-877 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Model calculations have been performed on displacement disorder effects in equatorial X-ray diffraction patterns of skeletal muscle. Powder patterns are calculated for single-site standard deviations (σ) up to 0.3 × lattice constant. The area ratio of the 11 and 10 peaks in the powder patterns is discussed. Line broadening in these patterns as a function of correlation length shows paracrystal-like behaviour for sufficiently large σ. Asymmetric line shapes and peak shifts in the direction of the central beam occur for values of σ larger than 0.2 × lattice constant and small correlation lengths.
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  • 130
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    Applied crystallography online 24 (1991), S. 893-909 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A method for calculating the flux at the sample position and the resolution function based on the general description of synchrotron X-ray beamlines in position–angle–wavelength space has been developed. A mathematical formulation is presented, in which source, transmission function for the slits and acceptance windows of the monochromator crystals are approximated by Gaussian functions. These approximations allow all of the algebra in connection with combining the different contributions to be done analytically. When the beam passes the various components of the beamline, such as flight paths, monochromators and mirrors, it results in coordinate transformations in parameter space. By inserting the transformations in the intensity distribution of the source, transmission functions of the slits and acceptance windows of the monochromators, these are transformed to the position of the sample. Their product gives the intensity distribution at this position and from this the resolution function in reciprocal space is calculated. The resolution of the detector is easily included by a convolution. The transmissions of the slits and the acceptance windows of the monochromator crystals have been normalized to give the same integrated transmission and reflectivities as the functions they approximate. Therefore the flux at the sample position can be calculated by multiplication of the brilliance of the source and the result obtained from an integration of the distribution over the two position parameters, the two angle parameters and the wavelength. The theory has been applied to an example and gives reasonable results for sample intensity and resolution function.
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  • 131
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    Applied crystallography online 24 (1991), S. 931-935 
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    Notes: Xenon gas can be used as a heavy atom for determining phases in a protein. We demonstrate that an interpretable electron density map can be obtained for sperm whale metmyoglobin from a single xenon derivative using iterative single isomorphous replacement with the anomalous scattering method.
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  • 132
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    Applied crystallography online 24 (1991), S. 950-955 
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    Notes: A program has been developed to help design a geometric representation of the atomic structure of interfaces between two crystalline structures. The C-language program run on a graphics-oriented computer has proved to be a simple precise tool to use. It provides a clear picture of the atomic positions at the interface and, simultaneously, a stereographic projection and diffraction pattern for each crystal and bicrystal. Examples of multiple twinning in the sphalerite structure and of various metal–ceramic interfaces are presented.
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  • 133
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    Applied crystallography online 24 (1991), S. 955-958 
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    Notes: With DEMUX and MUX, a pair of subroutines is provided that allows for the straightforward removal of multiple scattering from small-angle scattering data (DEMUX) or the simulation of the effect of multiple scattering (MUX). The data may be given in an arbitrary scaling. The parameter that must be given to fix the amount of multiple scattering is the transmission reduction of the sample due to small-angle scattering. The algorithm used is based on the method of Schelten & Schmatz [J. Appl. Cryst. (1980), 13, 385–390]. It is valid for a plane flat sample exhibiting scattering of significant intensity at small angles only.
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  • 134
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    Applied crystallography online 24 (1991), S. 968-971 
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    Notes: In the KTiOPO4 (KTP) structure, it is shown that there are hole sites related by pseudosymmetry to the inequivalent potassium sites K(1) and K(2). The formation of twin domains is through a twofold rotation with the principal feature of the twinning being the displacements of the K atoms onto their respective hole sites thus reversing the polarity of the crystal. Ionic diffusion paths for K+ along [001] involving both potassium and hole sites are described and are used to explain the enhanced ionic conductivity seen along this direction in KTP crystals. With this structural model, an explanation is also given for the reported phenomenon of domain inversion which is known to occur in the modified layer when Rb+ and Ba2+ are substituted into one of the {001} surfaces of KTP. It is shown from structural principles that ion exchange should be more efficient at the −Z end of the crystal, as is indeed observed in practice.
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  • 135
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    Applied crystallography online 24 (1991), S. 974-974 
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    Applied crystallography online 24 (1991), S. 982-986 
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    Notes: A new method for complete determination of polarization state in the hard X-ray region is described. The system consists of a perfect-crystal phase retarder and a linear polarization analyzer. This method gives not only the amplitude ratio of mutually perpendicular electric vector components and the phase shift between them but also the proportion of unpolarized radiation.
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  • 137
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    Applied crystallography online 24 (1991), S. 994-998 
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    Notes: The problem of the optimization of small-angle neutron scattering instruments installed at steady neutron sources is discussed. The optimum solution is shown to be that in which full use is made of either the available luminous area of the source or the available hall space and not necessarily that corresponding to the equal-flight-paths design. Design criteria and their implementation are discussed taking into account space constraints on the instrument's layout. It is shown that the performance of currently operating SANS facilities can be substantially improved by following the optimization procedure proposed by the authors.
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  • 138
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    Applied crystallography online 24 (1991), S. 987-993 
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    Notes: The dichotomy method for indexing powder diffraction patterns for low-symmetry lattices is studied in terms of an optimization of bound relations used in the comparison of observed data with the calculated patterns generated at each level of the analysis. A rigorous mathematical treatment is presented for monoclinic and triclinic cases. A new program, DICVOL91, has been written, working from the cubic end of the symmetry sequence to triclinic lattices. The search of unit cells is exhaustive within input parameter limits, although a few restrictions for the hkl indices of the first two diffraction lines have been introduced in the study of triclinic symmetry. The efficiency of the method has been checked by means of a large number of accurate powder data, with a very high success rate. Calculation times appeared to be quite reasonable for the majority of examples, down to monoclinic symmetry, but were less predictable for triclinic cases. Applications to all symmetries, including cases with a dominant zone, are discussed.
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  • 139
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    Applied crystallography online 24 (1991), S. 1009-1014 
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    Notes: Real-time neutron powder diffraction and small-angle scattering techniques have been developed on the TOF diffractometer DN-2 at the IBR-2 pulsed reactor at JINR (Dubna) with a total flux on the sample of 107 neutrons cm−2 s−1 and a resolution of about 1%. A special arrangement of the detector system ensures a high counting rate of diffracted neutrons. Depending upon sample type and experimental conditions, the measuring time ts of one neutron pattern varies from a few minutes to several seconds. The performance of the diffractometer is discussed and typical data are shown to demonstrate current achievements using real-time techniques at a pulsed reactor.
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  • 140
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    Applied crystallography online 24 (1991), S. 999-1004 
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    Notes: A simple method and simple camera of small size for obtaining X-ray topographs with a microfocus X-ray source are described and initial results and their interpretation are given for an LiF crystal. The method is based on scanning a Kossel line across the recording film by simultaneously translating the crystal and film relative to the source and to a stationary mask that blocks most of the scattered and fluorescence radiation. The mask, which is located between the specimen and the film, is made by using the Kossel line recorded on a film in the mask plane as a pattern; this provides self-alignment of the system. Theoretical calculations are given that indicate the potential angular resolution of the method when applied to nearly perfect crystals. The advantages of this method over similar methods using the X-ray continuum diverging from a point source are discussed.
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    Applied crystallography online 24 (1991), S. 1005-1008 
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    Notes: In the past, crystal structure determination of solids consisting of molecules (or atom groups) whose geometry and size are known approximately has often been attempted using neutron powder diffraction profile refinement techniques, but without inclusion of this information. A method of structure solution has therefore been developed to include it. The proposed method does not require a set of structure factors and thus avoids the problems encountered in separating peaks in a powder diffraction scan. A successful test was conducted with a previously determined (yet treated as unknown) crystal structure, where direct methods had failed to solve the structure due to incorrect peak separation. Two computer programs, MODEL and PARAM, that implement the method are described.
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    Applied crystallography online 24 (1991), S. 1023-1026 
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    Notes: The crystal structures of Zr2CO11 and HfCo7 intermetallic compounds were examined by transmission electron microscopy using both selected-area and convergent-beam electron diffraction. Results show that both have an orthorhombic crystal structure, space group Pcna. The unit cells of both compounds appear to be comprised of two long-period superlattices in antiphase relation to one another along [001].
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    Applied crystallography online 24 (1991), S. 1042-1050 
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    Notes: Very high-energy resolution measurements using X-rays can be achieved by extreme backreflection (Bragg angle close to 90°) from perfect crystals. This technique, combined with the high intensity of X-rays emitted by synchrotron-radiation sources, allowed the development of the instrument INELAX for inelastic scattering experiments. The principles and test results are discussed.
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    Applied crystallography online 24 (1991), S. 1035-1041 
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    Notes: Methods, implemented into a computer program (LSABS), are described which calculate transmission factors and their first derivatives with respect to the positions of the faces of a convex polyhedral monocrystal. Both Gaussian and analytical integration procedures are considered in detail. LSABS has been implemented as a module of the Xtal system of programs. It functions independently of the instrument used to collect the intensity data. Test results obtained with this program are compared with standard literature values. Correlation coefficients of an absorption-corrected intensity data set of calcite, CaCO3 are reported. The need for transmission factor derivatives in the refinement of crystal shape and in the elimination of correlated absorption-corrected structure amplitudes is explained.
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    Applied crystallography online 24 (1991), S. 1027-1034 
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    Notes: A large rapidly decreasing intensity called the `scattering tail' is generally observed at the smallest recorded angles during small-angle measurements of metallic alloys. Since this tail was interpreted as caused by a bimodal phase separation in Cu–Ni–Fe alloys and by long-wavelength concentration fluctuations in Invar alloys, these two systems were re-examined with anomalous X-ray scattering. The variation of the alloying atomic contrasts allows a discrimination between the different types of particles or defects. In neither of the two systems can the tails be interpreted as caused by large-scale concentration fluctuations. In Cu–Ni–Fe alloys, the tail is due to some kind of superficial defect (surface roughness etc.). In Invar alloys, the tail is probably due to residual impurity particles.
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    Applied crystallography online 24 (1991), S. 1015-1022 
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    Notes: X-ray diffraction studies are made on proton conducting polar lithium hydrazinium sulfate and ferroelectric lithium ammonium sulfate. The X-ray rocking curves recorded with in situ electric field along the polar b axis of lithium hydrazinium sulfate (direction of proton conductivity) show a strong enhancement of the 0k0 diffraction intensity. The corresponding 0k0 X-ray topographs reveal extinction contrast consisting of striations parallel to the polar axis. They disappear when the electric field is switched off. The effect is very strong in 0k0 but invisible in h0l reflections. It is present only if the electric field is parallel to the polar axis b. This unusual X-ray topographic contrast is correlated with the proton conduction. It is supposed that, under electric field, an inhomogeneous charge distribution develops, distorting the crystal lattice. Similar experiments on lithium ammonium sulfate also show contrast variations, but of quite different behaviour than before. In this case they result from changes of the ferroelectric domain configuration under electric field.
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    Applied crystallography online 24 (1991), S. 1051-1059 
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    Notes: The intensity profile of the X-ray reflection from a crystalline material is related to the lattice disorder and the distribution of crystal sizes through its Fourier cosine coefficients. However, existing methods of obtaining these structural parameters from the coefficients require more than one order of reflection and this is seldom available with polymer fibres. They also rely heavily on the low-order harmonics which are those determined with least accuracy. The development and testing of a method which overcomes this weakness and which is suitable for use with a single order is described. The coefficients are calculated for a model with paracrystalline disorder and an assumed distribution of crystal sizes and the parameters describing this model are refined to minimize the discrepancy between the calculated and experimental values of the coefficients. Provided the distribution of lengths is asymmetric this discrepancy is no greater than would be expected from experimental error and so the assumed model cannot be rejected on the evidence available. Since a range of model parameters all gave equally good agreement with experiment, it was not possible with a single order to obtain a well defined set of values. Diffraction patterns displaying two orders had been chosen and results from the second order were consistent with the first, only a narrow range satisfying both simultaneously. The method was further developed by calculating the intensity profile from the harmonics and using this in the refinement. There was no advantage over using harmonics; indeed, on occasions the refinement algorithm was unstable producing unreliable results.
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    Applied crystallography online 24 (1991), S. 1060-1062 
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    Notes: The application of an ultrafast analogue-to-digital converter and a high-performance-single board microcomputer permits the construction of a very fast and versatile multichannel analyser (MCA) at low cost. With the powerful instruction set of the microprocessor MC 68000, an intelligent all-round MCA could be realised with useful correction software on the single-board microcomputer. This MCA was used successfully for a data collection by Laue techniques with a four-circle diffractometer.
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    Applied crystallography online 24 (1991), S. 1067-1070 
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    Notes: A new version of DIRECT*SEARCHER (DIRECT-SEARCHER automatic system) for personal computers (PC) consisting of several crystallographic programs has been developed for automatic structure analysis of organic compounds as an innovation of the DS*SYSTEM [Koyama & Okada (1975). Acta Cryst. A31, S18]. Each program is improved and rewritten in Fortran77 for the 32 bit PC. The PC version of DS*SYSTEM is used by organic chemists rather than professional crystallographers.
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    Applied crystallography online 24 (1991), S. 1062-1062 
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    Notes: Owing to a typsetting error, the heading ER was wrongly mis-set as Eg in Table 1 of the paper by Misra, Bisoyi, Khan & Patel [J. Appl. Cryst. (1991), 24, 712–714]. The correct table is given.
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    Applied crystallography online 24 (1991), S. 1071-1072 
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    Notes: A program for the automatic definition of an asymmetric unit is described. Starting from the space-group symbol, an asymmetric unit is automatically calculated by means of a simple algorithm in the case of space groups up to the orthorhombic system. For higher symmetry a tabulation is used.
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    Applied crystallography online 24 (1991), S. 1063-1066 
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    Notes: An automatic processing program system of the molecular replacement method AUTOMR is presented. The program solves the initial model of the target crystal structure using a homologous molecule as the search model. It processes the structure-factor calculation of the model molecule, the rotation function, the translation function and the rigid-group refinement successively in one computer job. Test calculations were performed for six protein crystals and the structures were solved in all of these cases.
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    Applied crystallography online 24 (1991), S. 1072-1073 
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    Applied crystallography online 24 (1991), S. 1079-1079 
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    Applied crystallography online 24 (1991), S. 1074-1075 
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    Applied crystallography online 24 (1991), S. 1073-1074 
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    Notes: A novel method of heavy-atom equilibration with protein crystals is presented. This method utilizes a central drop of mother liquor containing the crystal surrounded by a locus of small drops containing the heavy-atom reagent.
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    Applied crystallography online 24 (1991), S. 1079-1080 
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    Applied crystallography online 24 (1991), S. 1080-1081 
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    Applied crystallography online 24 (1991), S. 1076-1078 
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    Notes: Converse-transformation theory and NIST*LATTICE open a new approach to study many theoretical and practical problems in crystallography. In this approach a new operator, the converse-transformation operator, is defined. The focus of this approach is based on the calculation of groups of matrices relating two lattices and subsequent analysis of these matrices to deduce crystallographic relationships. An efficient algorithm has been designed that has the ability to find all matrices (H) that relate ANY two cells (no matter how skewed) to within any specified tolerances (t) of the cell parameters. A Fortran program, NIST*LATTICE, that enables this new approach to be used is available to the scientific community. There are many immediate applications of converse-transformation analysis including the full automation of the single-crystal diffractometer and phase characterization using lattice-matching techniques.
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    Applied crystallography online 24 (1991), S. 1082-1082 
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    Applied crystallography online 24 (1991), S. 1081-1082 
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    Applied crystallography online 24 (1991), S. 1082-1082 
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    Applied crystallography online 24 (1991), S. 1083-1087 
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    Applied crystallography online 25 (1992), S. 1-5 
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    Notes: Based on investigations at 9 and 295 K, Na2UI6 has been shown to crystallize in a new structure type corresponding to space group R{\bar 3}, in contrast to ionic conductors of the type Na2UX6 for X = Cl, Br which crystallize in the space group P{\bar 3}ml. Atomic positions of sodium and iodine have been refined using the Rietveld profile fitting procedure. It was found that in space group R{\bar 3} the U, Na and I atoms occupy positions 3(a), 6(c) and 18(f), respectively. The relation between the Na2UCl6-type structure and the structure of Na2UI6 is discussed.
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    Applied crystallography online 25 (1992), S. 11-15 
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    Notes: An in situ observation of the structure transition of GeO2 has been made under 3.0 GPa at various temperatures with a diamond-anvil pressure cell. The time-resolved energy-dispersive (ED) diffraction experiment was undertaken using synchrotron X-radiation. A profile analysis of ED spectra observed every 15 min elucidates the transition process from the α-quartz form (P3221, Z = 3) to the rutile form (P42/mmm, Z = 2). The time-resolved measurement of their diffraction intensity ratio reveals the change of the mass fraction of the transformed product with time, which provides the transition rate. A transition curve showed three stages at low temperature; firstly a long inductance period after initiation of heat supply, secondly a rapid initiation of transition and finally a marked deceleration of growth. At high temperatures the inductance period of the transition was not observable. The transition is extremely sluggish. An apparent activation energy was calculated by the Avrami–Erofeev equation for the solid-solid transition and found to be 57.4 kJ mol−1.
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    Applied crystallography online 25 (1992), S. 6-10 
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    Notes: Nonlinear equations are given for determining the crystallographic orientation of surfaces of single crystals. The equations are solved by an iterative method in several variables. The angle φ between the surface plane and the lattice plane in question is decomposed into two components α and β. These two components are obtained from the solution of a nonlinear system of equations using two measurements and the Bragg angle. The diffractometric system considered is the well known θ/2θ with a sufficiently large area of X-ray detection and the capability of holding single-crystal samples. The results obtained are discussed from experimental and theoretical points of view.
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  • 167
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    Applied crystallography online 25 (1992), S. 26-30 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A method to improve the scaling of multiple intensity data sets is presented. A general scaling function K(x, s), which uses the direction cosine of the diffraction vector (x) and (sin θ)/λ (s) as scaling parameters, is developed by combining an isotropic scaling function, K(s) = A exp (Bs2), and a multiple s-shell anisotropic scaling function, K(x)s = (Σ Σ cijxij)s. This combined scaling function can greatly reduce the systematic differences in intensities among multiple data sets measured independently. This scaling method for the multiple data sets consists of three steps. In the first step, the individual isotropic scaling functions, K(s), are determined by an indirect least-squares method. Then the weighted mean intensity, 〈I〉, is calculated by applying the K(s) to the individual data sets. In the second step, the data in each data set are divided equally into 20 thin shells of (sin θ)/λ (s). The anisotropic scaling functions, K(x)s, of each s shell are determined by using the weighted mean intensity, 〈I〉, obtained in the first step as the target quantity in a least-squares minimization, i.e. Σ wi{〈I〉i − K(x)s[K(s)Ii]}2. In the final step, the new weighted mean intensity, 〈I〉, is calculated by applying the combined scaling function, K(x, s) = K(s)K(x)s, to the individual data sets. The new multiple s-shell anisotropic scaling functions are determined using the new weighted mean intensity, 〈I〉, as the target quantity in another least-squares minimization. By repeating this procedure three to five times, the least-squares minimization will converge. The method was successfully used to scale and merge 27 sets of S-adenosylmethionine synthetase data into a single data set. It was also used to scale the isomorphous replacement data sets of the enzyme.
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  • 168
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    Applied crystallography online 25 (1992), S. 16-25 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: This work presents a new method of synthesizing the reflection profile, based on the calculation of Fourier coefficients of instrumental functions. The classification and construction of Fourier coefficients are effected, in a general way, from the analysis of the possible paths of beams in the diffractometer. Relationships were obtained which made it possible to synthesize the line profiles in different experimental conditions. The possibility of calculating the reflection profiles of a standard (annealed BaF2) without introducing varying profile parameters is shown. Better results in describing the reflection profiles have been obtained than by applying the Pearson VII function with varying profile parameters.
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  • 169
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    Applied crystallography online 25 (1992), S. 31-38 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A model of size distribution and structural disorder for palladium grown on pumice is developed. The model parameters are determined by fitting the simulated powder pattern to the experimental data. Three samples, characterized by 2.4, 1.14 and 0.86 wt.% Pd respectively were examined. The results point to nearly spheroidal crystallites, with sizes ranging from 40 to 20 Å, affected by stacking faults in the sequence of the close-packed (111) layers to an extent independent of size and by intralayer second-kind distortions. A comparison with the results obtained following classical procedures is supplied. In the Appendix a new approach for the determination of growth stacking faults from peak shifts is presented.
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  • 170
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    Applied crystallography online 25 (1992), S. 39-45 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Approximate analytic expressions for determining the transmission of neutron benders which take into account reflectivity losses using the mean number of reflections agree well with computer simulation results which track the neutron trajectories directly, provided that the reflectivity is high. The exact calculation which can be performed using exponential integral functions for any value of the reflectivity is presented. Ray-tracing techniques for determining the transmission and number of reflections for non-perfect reflectivity can therefore be replaced by direct calculation.
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  • 171
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    Applied crystallography online 25 (1992), S. 46-51 
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    Topics: Geosciences , Physics
    Notes: The simulation of the experimental symmetric X-ray rocking curve of a coherent heteroepitactic structure, using first-order expressions in the incidence parameter, is shown to give a strain-depth profile not consistent with asymmetric rocking curves taken on the same sample. Two different expressions are suggested for the incidence parameter to attain internal consistency among all the rocking curves. The former involves second-order approximations and considers both normal and parallel lattice mismatches. The latter is the result of an exact derivation and takes into account only the normal mismatch. These models make the data from rocking-curve simulation reliable, provided that the angle between the surface and the planes corresponding to the nominal crystallographic orientation is not ignored.
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  • 172
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    Applied crystallography online 25 (1992), S. 65-68 
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    Notes: A procedure for evaluating peaks in the difference Patterson maps calculated from a complete native data set and partial (incomplete) potential isomorphous heavy-atom-derivative data sets is described. A sampling function is defined such that it is unity where data are available and zero elsewhere. It is the Patterson of this sampling function whose characteristics are useful. This function will not reconstruct unavailable information, but can reveal the presence of distorted and/or `false' peaks introduced by the sampling technique used in collecting partial data. This procedure is useful in screening potential heavy-atom derivatives using a minimum number of crystals.
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  • 173
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    Applied crystallography online 25 (1992), S. 52-64 
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    Notes: The theory of surface differential diffraction (SDD) is extended to the case of polarized neutron diffraction. Nuclear and magnetic surface contributions are thus separated. A method for coherent description of the geometry of the grains is proposed. A saturated D layer chemisorbed on Ni carried by silica is studied with the following results: (111) faces represent the majority of the surface; D atoms sit above the centers of surface Ni triangles with no Ni atom in the underlying layer, the Ni–D distance is equal to 0.215 (7) nm; the magnetic moment modification induced by chemisorption is mainly localized in the surface layer of nickel. Two possible interpretations of the magnetic structure factor are discussed: one assumes no magnetic moment on D atoms but Ni displacements; the other is based on opposite assumptions.
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  • 174
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    Applied crystallography online 25 (1992), S. 69-72 
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    Topics: Geosciences , Physics
    Notes: A method and algorithm are described for solution of the autoindexing problem of multiphase polycrystals. A Fortran program, called MRIAAU, which implements the algorithm, runs on a PC and can solve the problem in some minutes (IBM PC with 80286 and higher).
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  • 175
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    Applied crystallography online 25 (1992), S. 69-69 
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    Notes: In the paper by Schwarzenbach & Flack [J. Appl. Cryst. (1989). 22, 601–605], the equation describing the transformation properties of the crystal-based azimuthal angle ψ is incorrect. The correct formula is derived.
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  • 176
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    Applied crystallography online 25 (1992), S. 87-87 
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  • 177
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    Applied crystallography online 25 (1992), S. 73-80 
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    Notes: BLAF represents an original computer program to devise the Bravais lattice symmetry or possible pseudo-symmetries (with allowance for large axial and angular distortions) of an experimental unit cell. The matrix approach to symmetry formulated by Himes & Mighell [Acta Cryst. (1987). A43, 375–384] is further developed and employed to analyse admittable mappings of a lattice onto itself. Solutions of the matrix equations G = MtGM, where G is the metric tensor of the Buerger reduced lattice, are integral matrices M with det(M) = + 1 and −1 〈 tr(M) ≤ 3, composing the seven axial hemihedral point groups 432, 622, 422, 32, 222, 2, 1. For non-triclinic symmetries these matrices carry information about important symmetry directions in the lattice, subsequently used in building up an overall transformation matrix to find a conventional (symmetry-conditioned) unit cell. The average of the generated G tensors in accordance with the particular point-group rules is a tensor Gav bearing information about the symmetry-constrained lattice parameters. Gruber's [Acta Cryst. (1989), A45, 123–131] algorithms have been used to evaluate both Buerger cells and the Niggli cell of a triclinic lattice. BLAF is realised as a separate module suitable for incorporation in the commonly used crystallographic program packages and in the form of two subroutines: enBLAF – to tackle the lattice symmetry problem by automated single-crystal diffractometers; and rBLAF – to be used for lattice symmetry analysis in, for example, programs for autoindexing of powder data. Applications of the three modules are demonstrated in several test examples.
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  • 178
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    Applied crystallography online 25 (1992), S. 81-86 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
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    Notes: Normal and half-normal probability plots have been used extensively in the analysis of data and parameters in small-molecule crystallography. A procedure and computer program is described to apply this method to macromolecular data. The utility of this procedure is that a subset of data from a putative heavy-atom derivative can be analyzed and compared with a native set of data providing a quantitative indicator of individual and overall changes in intensity. A qualitative measure of the scattering contribution as a function of resolution can be obtained from comparisons of different resolution ranges. The results from comparisons of (i) native data collected by different techniques and (ii) native and heavy-atom-derivative data suggest a set of guidelines which can be used as an aid in the selection of data with a significant heavy-atom contribution.
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  • 179
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    Applied crystallography online 25 (1992), S. 92-96 
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    Notes: An indexing method for single-crystal diffractometry is described which is applicable to especially difficult cases such as twin lattices, incommensurate structures, fragmented crystals, long axes and unreliable data. Finding the reciprocal lattice from a cloud of reciprocal-lattice points (reflections) is reduced to finding elementary periods in one-dimensional rows, obtained by projecting all observed points onto the normal to the plane formed by any three of these points. Row periodicity and offending reflections are easily recognized. Each row, by its direction and (reciprocal) spacing, defines one direct axis vector, based upon all cooperating observations. From the direct vectors so obtained a primitive direct cell is chosen and refined against the fitting reflections. The result is one main lattice, or a main lattice and a set of alien reflections. The method operates semi-automatically in the program DIRAX and has been tested, without failure, on hundreds of CAD4 reflection files, among which there were many auto-indexing-resistant lists.
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  • 180
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    Applied crystallography online 25 (1992), S. 88-91 
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    Notes: A study of X-ray diffraction in single silicon and quartz crystals in a strong ultrasonic field has been carried out. The dependence of diffraction intensity I(w) on sound amplitude w has been obtained right up to the kinematical limit Ik = I(∞). It is shown that the ratio η = I(∞)/I(0) depends on the crystal quality. Experimental data for different reflections, sound frequencies and X-ray wavelengths are compared with the model calculations for several lattice-distortion mechanisms.
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  • 181
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    Applied crystallography online 25 (1992), S. 97-104 
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    Notes: A new procedure of pattern decomposition in energy-dispersive powder diffraction is presented. The total observed pattern is taken as a sum of incoherent and coherent scattering. The incoherent part is calculated from theoretical cross sections for individual atoms, the coherent part is described as a sum of discrete Bragg peaks and acoustic and optic phonon thermal diffuse scattering (TDS) is calculated from the Debye and Einstein models, respectively. The total TDS is scaled to be the scattering missing from the Bragg reflections due to thermal motion. The model pattern is convoluted by the instrument function calculated from the diffraction geometry, and the pattern is fitted to the observed one by varying the integrated Bragg intensities and thermal motion parameters. The method is applied to patterns of Mg, Al and Ti powders, leading to an unambiguous and self-consistent division to the background and the pattern of Bragg reflections. As an application, the flux of continuous radiation from a W-anode X-ray tube is determined using theoretical integrated Bragg intensities.
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  • 182
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    Applied crystallography online 25 (1992), S. 109-121 
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    Topics: Geosciences , Physics
    Notes: A convolution approach to X-ray powder line-profile fitting is developed in which the line shape is synthesized from the Cu Kα emission profile, the dimensions of the diffractometer and the physical variables of the specimen. In addition to the integrated intensities and 2θ positions of the line profiles, the parameters that may be fitted include the receiving-slit width, the receiving-slit length, the X-ray-source size, the angle of divergence of the incident beam, the X-ray attenuation coefficient of the specimen and the crystallite size. This is a self-consistent approach to fitting as the instrumental parameters are usually known by direct measurement. To minimize correlation between refined instrumental parameters, profiles at high and low 2θ values should be fitted simultaneously. The Cu Kα emission profile used in this work is based on recent monolithic double-crystal spectrometer measurements that have identified a doublet structure in both the Kα1 and Kα2 components. Fast and accurate convolution procedures have been developed and a mixture of multilinear regression and Gauss–Newton non-linear least squares with numerical differentials is used for fitting the profiles. The method is evaluated by fitting powder diffraction data from well crystallized specimens of MgO and Y3Al5O12 (YAG). Testing has also been carried out by examining the changes in the fitted values after altering various instrumental parameters (e.g. receiving-slit width, detector defocus, receiving-slit length and inclusion of a monochromator).
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  • 183
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    Applied crystallography online 25 (1992), S. 122-128 
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    Notes: Microplanar defects were observed in β-iron disilicide by transmission electron microscopy. They were identified as (100)[011]/2 intrinsic stacking faults by means of electron diffraction patterns and observed in high-resolution lattice images. A structural model of the faults is proposed here in setting the defect position at x = ¼ within the cell.
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  • 184
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    Applied crystallography online 25 (1992), S. 105-108 
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    Notes: An intrinsic Ge detector is used to analyze the energy spectrum of a well collimated X-ray beam of white radiation diffracted from powder samples of Al, Mg and Ti. Two spectra on each sample are measured at scattering angles where reflections hkl and 2h′ 2k′ 2l occur at the same energies. The Bragg reflections are separated by fitting a model for the different components of scattering to the total spectrum. The thermal-motion parameter B is determined from the intensity ratio of several pairs of reflections. Most of the uncertainties due to a non-ideal sample or errors in the experimental parameters cancel out in the expression for B. The values of B are 0.86 (2) Å2 for Al, Ba = 1.29 (8) Å2 and Bc = 1.60 (9) Å2 for Mg and Ba = 0.63 (4) Å2 and Bc = 0.73 (7) Å2 for Ti, where Ba is for directions perpendicular to the c axis and Bc for the direction of the c axis. The results are in agreement with published values of the thermal-motion parameters.
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  • 185
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    Applied crystallography online 25 (1992), S. 129-145 
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    Topics: Geosciences , Physics
    Notes: An approach for analysing neutron and X-ray specular reflectivity data from stratified media having variation in the scattering-length density near the surface is described. The method has its origin in small-angle scattering and it is composed of two steps: (i) indirect Fourier transformation [Glatter (1977). J. Appl. Cryst. 10, 415–421] giving the profile correlation function p(z) of the derivative dρ/dz of the scattering-length density; (ii) square-root deconvolution [Glatter (1981). J. Appl. Cryst. 14, 101–108] giving dρ/dz and ρ, the scattering-length-density profile. The only requirement for applying the method is that the scattering-length density varies only in a limited range. In nearly all cases the approach does not require any knowledge of the chemical composition of the surface layer and consequently incorporates a certain degree of objectivity. The method gives the smoothest profile which agrees with the experimental reflectivity data. The method is tested on simulated reflectivity data for a series of different surface profiles and subsequently used for analysing experimental data on fluorocarbon amphiphiles in water and salt solutions. The tests on simulated data show that the indirect Fourier transformation gives correlation functions agreeing very well with the corresponding functions of the original profiles. It is further demonstrated that the square-root deconvolution gives reliable results for the scattering-length-density profiles.
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  • 186
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    Applied crystallography online 25 (1992), S. 146-154 
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    Topics: Geosciences , Physics
    Notes: Area detectors have revolutionized data collection in protein crystallography, but unsubstantiated opinion as to the merits of these detectors has sometimes interfered with objective comparisons of area detector quality. Area detectors from four manufacturers were evaluated by collecting data sets on two different protein crystals, carboxypeptidase A and recombinant sperm whale myoglobin. These data sets were first compared by studying their internal consistency using Rsym measurements and as expected these Rsym values were excellent. Next, the data were studied by merging with diffractometer data sets and with each other. Finally, the myoglobin data were used to calculate anomalous difference Pattersons. Area detectors studied in this way included the Mark II from San Diego Multiwire Systems, the FAST from Enraf–Nonius, Inc., the R-AXIS II from Rigaku Corporation and the X-1000A from Siemens Analytical X-ray Instruments, Inc. Wide variations existed in the data-collection parameters chosen by the manufacturers, but all four detectors produced acceptable data as evidenced by mutual agreement and clear interpretability of anomalous difference Patterson maps based on the Fe atom in myoglobin.
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  • 187
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    Applied crystallography online 25 (1992), S. 192-194 
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    Topics: Geosciences , Physics
    Notes: The single-crystal X-ray diffractometer installed at the PWA Laboratory in Frascati is described. The Huber four-circle goniometer is controlled by an IBM-compatible personal computer by means of a plug-in board interface based on the LSI chip Am9513. The program CS running under MS-DOS performs a wide variety of operations from random search to data collection. The angular resolution of the diffractometer is 0.0025°, while the instrumental resolution at 8 keV, with an Si(lll) monochromator, is 0.0026°. After preliminary tests, 2Zn insulin crystals were mounted on the diffractometer and reflections were measured using synchrotron radiation. The rocking curves show full widths at half-maxima (FWHM) in the range 0.013–0.031° mainly due to the mosaicity.
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  • 188
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    Notes: A new polarized target for neutron scattering has been designed by CERN and tested successfully using the reactor FRG-1 at the GKSS Research Centre. The nuclear spins are aligned with respect to the external field – parallel or antiparallel – by dynamic nuclear polarization (DNP). To avoid absorption of neutrons by 3He, the frozen solutions of biomolecules are immersed in liquid 4He which in turn is thermally coupled to the cooling mixture of 3He/4He of the dilution refrigerator. Compared with earlier experiments where the sample had been cooled directly by 3He, the rate of detectable neutrons increased by a factor of 30. Another factor of 30 is due to the installation of the cold source and the beryllium reflector in FRG-1. Polarized neutron scattering from apoferritin in deuterated solvent shows that the proton spin polarization is homogeneous in apoferritin molecules. After saturation of proton nuclear magnetic resonance (NMR), polarized neutron scattering is dominated by deuteron spin contrast. With the deuterated large subunit of E. coli ribosomes, three different basic scattering functions are derived from spin-contrast variation, reflecting the known scattering-length-density distribution of the architecture of rRNA and ribosomal proteins. The planned in situ structure determination of a mRNA fragment is discussed in the light of the present results.
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  • 189
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    Applied crystallography online 25 (1992), S. 181-191 
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    Notes: Low-resolution three-parameter models of the shape of a biopolymer in solution can be determined by a new indirect method from small-angle X-ray scattering without contrast-variation experiments. The basic low-resolution model employed is a triaxial ellipsoid – the inertia-equivalent ellipsoid (IEE). The IEE is related to the tensor of inertia of a body and the eigenvalues and eigenvectors of this tensor can be calculated directly from the atomic coordinates and from the homogeneous solvent-excluded body of a molecule. The IEE defines a mean molecular surface (like the sea level on earth) which models the molecular shape adequately if the IEE volume is not more than 30% larger than the dry volume of the molecule. Approximately 10 to 15% of the solvent-excluded volume is outside the ellipsoid; the radii of gyration of the IEE and of the homogeneous molecular body are identical. The largest diameter of the IEE is about 5 to 15% (0̃.2–0.8 nm) smaller than the maximum dimension of globular molecules with molecular masses smaller than 65000 daltons. From the scattering curve of a molecule in solution the IEE can be determined by a calibration procedure. 29 proteins of known crystal structure have been used as a random sample. Systematic differences between the axes of the IEE, calculated directly from the structure, and the axes of the scattering-equivalent ellipsoids of revolution, estimated from the scattering curve of the molecule in solution, are used to derive correction factors for the axial dimensions. Distortions of model dimensions of 20 to 40% (up to 1 nm), caused by misinterpretation of scattering contributions from electron density fluctuations within the molecule, are reduced to a quarter by applying these correction factors to the axes of the scattering-equivalent ellipsoids of revolution. In a computer experiment the axes of the inertia-equivalent ellipsoids have been determined for a further nine proteins with the same accuracy. The automated estimation of the IEE from the scattering curve of a molecule in solution is realized by the Fortran77 program AUTOIEE.
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  • 190
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    Applied crystallography online 25 (1992), S. 195-198 
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    Notes: The application of the Laue method is extended to phase identification of single crystals. This extension is made possible by a new method of indexing Laue patterns, which is based on computerized rotation of the reciprocal axes of the crystal and a new criterion for judging true solutions. The new method and criterion have been tested successfully for crystals with various structures, including triclinic. An example is given for the phase identification of molybdenum oxide which has six structural modifications.
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  • 191
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    Applied crystallography online 25 (1992), S. 199-204 
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    Notes: High-resolution transmission electron microscopy (HRTEM) and electron diffraction were used to investigate the microstructure of natural lead oxides found in Panzhihua Mountain, China. The electron diffraction patterns showed crossing of diffraction spots along 〈110〉 directions in litharge and along 〈100〉 directions in massicot and the structural images showed the domain-like texture, probably constructed by arrays of planar defects in the fundamental structures. Based upon the structure of these oxides the possible structural models of planar defects are discussed and the orientation relationship of litharge and massicot is determined.
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  • 192
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    Applied crystallography online 25 (1992), S. 211-213 
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    Notes: The lens equation for Bragg diffraction of monochromatic X-rays and neutrons in the case of a cylindrically curved crystal is derived for the general Bragg- and Laue-case geometries. The resulting equation is identical to the formula for polychromatic focusing only in the limits of symmetrical reflection and/or in Rowland geometry.
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    Applied crystallography online 25 (1992), S. 166-180 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Structure determination of macromolecules often depends on phase improvement and phase extension by use of real-space averaging of electron density related by noncrystallographic symmetry. Although techniques for such procedures have been described previously [Bricogne (1976). Acta Cryst. A32, 832–847; Johnson (1978). Acta Cryst. B34, 576–577], modern computer architecture and experience with these methods have suggested changes and improvements. Two unit cells are considered: (1) the p-cell corresponding to the actual crystal structure(s) being determined (there would be more than one of these if the molecule crystallizes in more than one crystal form) and (2) the h-cell corresponding to the molecule in a standard orientation with respect to which the molecular symmetry axes are defined. Averaging can proceed entirely within the p-cell, referring to the h-cell only in as far as knowledge of the molecular symmetry is required. It is also possible to place the averaged molecule back into the h-cell, where it can be used to redefine the molecular envelope or for displaying a suitably chosen asymmetric unit of the molecule. Techniques are discussed for automatically selecting a molecular envelope which is consistent with packing considerations within the p-cell and which retains the symmetry of the molecular point group. The electron density map to be averaged is divided into bricks for storage in virtual memory. Roughly as many bricks as there are noncrystallographic asymmetric units per crystallographic asymmetric unit need to be retained in memory at one time. This procedure minimizes paging problems and avoids double sorting. Use of eight-point interpolation permits storing the map at grid points separated by no more than 1/2.5 of the resolution limit to obtain rapid convergence.
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  • 194
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 25 (1992), S. 214-220 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Software has been written in Fortran77 for the space-filling representation of crystal structures. It generates atomic positions starting from the asymmetric unit and taking into account the 230 possible space groups. It then computes realistic shaded images in correct perspective with the hidden part removed. The main differences from existing programs are the ability to represent thermal ellipsoids and good portability to commonly used workstations. Details are given about the organization and operation of the program and some applications.
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  • 195
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 25 (1992), S. 205-210 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Ambiguities in amino acid sequences are a potential problem in X-ray crystallographic studies of proteins. Amino acid side chains often cannot be reliably identified from the electron density. Many protein crystal structures that are now being solved are simple variants of a known wild-type structure. Thus, cloning artifacts or other untoward events can readily lead to cases in which the proposed sequence is not correct. An example is presented showing that mass spectrometry provides an excellent tool for analyzing suspected errors. The X-ray crystal structure of an insertion mutant of Staphylococcal nuclease has been solved to 1.67 Å resolution and refined to a crystallographic R value of 0.170 [Keefe & Lattman (1992). In preparation]. A single residue has been inserted in the C-terminal α helix. The inserted amino acid was believed to be an alanine residue, but the final electron density maps strongly indicated that a glycine had been inserted instead. To confirm the observations from the X-ray data, matrix-assisted laser desorption mass spectrometry was employed to verify the glycine insertion. This mass spectrometric technique has sufficient mass accuracy to detect the methyl group that distinguishes glycine from alanine and can be extended to the more common situation in which crystallographic measurements suggest a problem with the sequence, but cannot pinpoint its location or nature.
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  • 196
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 25 (1992), S. 221-230 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A generalized formalism on multiple small-angle scattering is proposed to investigate the nature of the extractable structural information on inhomogeneities from the multiple-scattering profile. It is found that the statistical nature of the medium can broaden as well as narrow the scattering profile depending upon the characteristics of the medium. The nature and the extent of the effect of the various approximations on analysing the multiple-scattering data are discussed.
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  • 197
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 25 (1992), S. 237-243 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Even the best least-squares algorithm to extract intensities from a powder diagram will not be able to determine the separate intensities of completely overlapping peaks. In this paper a new method (DOREES) is presented to determine these intensities more accurately by applying relations between structure factors derived from direct methods and the Patterson function. The intensities obtained from the least-squares fit are used as a starting set for DOREES. Comparative tests on both artificially generated and real data show that DOREES improves the intensity set considerably.
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  • 198
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 25 (1992), S. 244-250 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A design is presented of apparatus suitable for energy-dispersive diffuse X-ray scattering in which the sample is oriented on a three-circle cradle within a vacuum chamber. The apparatus alignment procedures are discussed and a method given for finding the relevant orientation matrix under the conditions of Laue scattering to a fixed detector. The method also finds the zero positions of the orienter and is not confined to diffuse-scattering applications.
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  • 199
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 25 (1992), S. 268-273 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Construction and performance of a spectrometer based on a high-voltage generator and W-anode X-ray tube are described. W Kα1 radiation is monochromated using a bent Ge (400) crystal. The obtained monochromatic flux is 107 photons s−1 and the beam size at the focal point 15 × 0.5 mm. Comparison is made with a 241Am γ-ray source, which has an almost equal photon energy. The W Kα1 beam does not exhibit the low-energy tail typical for the γ-ray source but, on the other hand, a small contribution of doublet energy was observed. Directional Compton profiles of pyrolytic graphite were measured with both sources and essentially the same features were found.
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  • 200
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 25 (1992), S. 259-267 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The orientation distribution function (ODF) of the crystallites of polycrystalline materials can be calculated from experimentally measured pole density functions (pole figures). This procedure, called pole-figure inversion, can be achieved by the series-expansion method (harmonic method). As a consequence of the (hkl)-({\bar h}{\bar k}{\bar l}) superposition, the solution is mathematically not unique. There is a range of possible solutions (the kernel) that is only limited by the positivity condition of the distribution function. The complete distribution function f(g) can be split into two parts, \tilde {f}(g) and \tildes {f}(q), expressed by even- and odd-order terms of the series expansions. For the calculation of the even part \tilde {f}(g), the positivity condition for all pole figures contributes essentially to an `economic' calculation of this part, whereas, for the odd part, the positivity condition of the ODF is the essential basis. Both of these positivity conditions can be easily incorporated in the series-expansion method by using several iterative cycles. This method proves to be particularly versatile since it makes use of the orthogonality and positivity at the same time. In the previous paper in this series [Dahms & Bunge (1989) J. Appl. Cryst. 22, 439–447] a general outline of the method was given. This, the second part, gives details of the system of programs used as well as typical examples showing the versatility of the method.
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