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  • International Union of Crystallography (IUCr)  (1,004)
  • 1980-1984  (1,004)
  • 1965-1969
  • 1981  (1,004)
  • 1
    Electronic Resource
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 211-219 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: For explaining diamagnetic effects observed in condensed aromatic compounds, their molecular diamagnetic anisotropies must be known. A method is proposed which, on the basis of relatively accurate structural data and of two experimental crystal anisotropies, allows the determination of molecular anisotropies in the plane and perpendicular to it. For monoclinic compounds whose magnetic tensor has no revolution symmetry, it is necessary to correct to first order the orientation of the principal magnetic axes of the crystal with respect to revolution symmetry. The proposed method is applied and discussed in the case of ten condensed aromatic compounds which crystallize in the orthorhombic and monoclinic systems. It yields, in some cases, molecular anisotropies very different from those suggested by different authors. One very simplified model produces results which fit in with the molecular anisotropies obtained as long as the arrangement of the rings is not too complex.
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  • 2
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 219-226 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Diffuse X-ray scattering in Li3N has been investigated in the range 293 to 880 K with monochromatic Mo Kα radiation. Crystal and film were fixed during the exposure. Diffuse intensity in the form of rods and discs was found. It increased with increasing temperature but without change of its features. The diffuse intensity distribution was calculated for various temperatures on the basis of an anisotropic shell model. Good agreement with the experimental results was achieved. The anharmonic effects detected in the difference electron density were studied taking into account split positions for the Li ions. This simulation leads to only minor changes in the calculated intensity distribution which indicates that the diffuse intensity of Li3N is mainly caused by harmonic lattice vibrations.
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  • 3
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 267-268 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Recent experimental measurements have revealed systematic differences between measured values of f' and those calculated by the method of Cromer & Liberman [J. Chem. Phys. (1970), 53, 1891-1898] when the incident X-ray is near to and on the long-wavelength side of an edge. The source of the discrepancy has been identified and some previously published values of f' are corrected. These corrections also apply to Table 2.3.1 in International Tables for X-ray Crystallography, Vol. IV [(1974), Birmingham: Kynoch Press].
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  • 4
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 269-269 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
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  • 5
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 335-342 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Owing to progress in lattice-dynamical computing routines, free-energy calculations for perfect molecular crystals are no longer prohibitive in the quasi-harmonic approximation. Thus the consistent derivation of an equilibrium conformation at various temperatures and pressures, and even the stability range of various phases, may become a routine possibility, starting from semi-empirical potentials only. An example of such conformational calculations is given and discussed for the tetragonal phase of adamantane at 163 and 1 K. The effect of vibrational energy (even zero-point) and entropy upon molecular orientation and position in the unit cell is shown not to be negligible by several examples. This precludes the possibility of calculating the cell parameters on free-energy grounds and the molecular coordinates by considering the minimum packing energy. For crystals with molecules fixed by symmetry, the quasi-harmonic approximation becomes particularly appropriate, since in this case for any unit cell the first derivatives of energy with respect to any molecular shift are zero. Some critical steps of such calculations are examined and discussed, especially in connection with converging processes. No particular problem is encountered in sampling the Brillouin zone, because only a limited number of points is necessary. Convergence of lattice sums to obtain packing energy is more critical, although for most practical purposes a maximum packing distance of 15 Å is sufficient. The real difficulties of these calculations consist in the need of considering many degrees of freedom at once, and also in the inadequacy of present-day semi-empirical potentials.
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  • 6
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 361-364 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: All 20 independent third-order elastic constants (TOEC) of orthorhombic calcium formate, Ca(HCOO)2, Ca2+. C2H2O2-4, space group Pcab, have been determined with the aid of stress-induced shifts of ultrasonic resonance frequencies. Longitudinal and transverse effects possess negative values indicating the high stability of calcium formate over a wide pressure range. The anisotropy of TOEC, characterized by --c111 〉 --c333 〉 --c222, corresponds with the anisotropy of second-order elastic constants (c11 〉 c33 〉 c22). The value 5.22 for the pressure derivative of the inverse bulk compressibility coincides with the quasi- invariant value of ca 5 observed in most stable cubic crystals so far investigated. There exists a pronounced departure from third-order Cauchy relations: the 'transverse' constants exceed the corresponding 'shear' components considerably in absolute magnitude in accordance with the behaviour of the second-order Cauchy relations. These effects are explained as originating from the non-centrosymmetric formate ions. A comparison of TOEC of calcium formate and cubic calcium fluoride confirms the typical contribution of the formate ions to the third-order elastic behaviour.
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  • 7
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 281-286 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A synthetic pyroxenoid of nominal composition MnFeSi2O6 has been produced in the glassy state and examined by high-resolution electron microscopy after periods of annealing of from two to sixteen hours at 1070 K. Initially highly defective structures exhibiting large chain repeat distances are produced, but on further annealing the five-tetrahedra chain repeat of rhodonite predominates. (110)-type stacking faults are frequently observed. In most eases these faults involve considerable disruption of the lattice, but in certain instances the stacking fault displacement is equal to the rhodonite lattice repeat and the faults are visible only if the chain periodicity varies. In the latter case, the structure shows a two-dimensional ability to accommodate defects, and models for this, involving chain breaking and/or chain branching, are proposed.
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  • 8
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 286-292 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: This article contains a table of the groups of combined geometrical and color-permutational symmetry operations that leave a certain kind of three-colored, three-dimensionally periodic object apparently unchanged. The asymmetric units - 'motifs' - of the object are all either geometrically congruent to, or are mirror images of, one another. Each motif has a 'color' representing a scalar quality of some kind, and three different colors of motifs are assumed to occur in the object. Two types of three-colored space groups exist: type I in which all of the geometrical lattice translations leave all the motifs unchanged in color, and type II in which at least one of the geometrical lattice translations requires a permutation of the three colors in order to restore the original appearance. There are 88 three-colored space groups of type I, and 341 of type II. Type I can belong only to the trigonal, hexagonal and cubic systems; type II can belong to any system, except the cubic. A notation for the three-colored, three-dimensional space groups is proposed. It is based on similar principles to those used in the article on colored point groups by Harker [Acta Cryst. (1976), A32, 133-139].
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  • 9
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 309-314 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The Fourier transform of a finite coiled coil containing an integral number of repeat units is evaluated analytically. The special cases where the coiled coil reduces either to a pure helix or to a toroidal helix are specifically included.
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  • 10
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 324-331 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Two of the magnetic superlattice Bragg reflections of a single crystal of hematite (Fe2O3) have been measured by diffraction of X-rays produced from a conventional source, and compared to the intensities expected from the photon-spin scattering. Several orientations of the spins relative to the beams have been realized by rotating the crystal and by changing its temperature through the Morin (spin-flip) transition; in some of the measurements, the polarization produced by the monochromator was enhanced and this produced a visible asymmetry in the dependence of the intensities on the spin direction. The variations of the intensities during these changes of configuration are characteristic of magnetic scattering; the observed variations, as well as the absolute intensities, agree with the theory apart from some discrepancies. These may be due to intense multiple-scattering effects, and to some possible anomalies in the spin direction near the sample surface. As an application of this technique, changes of the direction of magnetization when a magnetic field is applied to the weakly ferromagnetic room-temperature phase have been investigated.
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  • 11
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 407-413 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: It has been found that the crystallization of oxyhaemoglobin from polyethylene glycol solutions [Grabowski et al. (1978). Biochem. J. 171, 277-279] yields at least three different forms of isomorphous crystals (P21212, a = 96.66, b = 97.88, c = 65.40 Å). 3.5 Å resolution data have been collected for two of the three identified forms. The orientations and positions of the αβ haemoglobin dimers within the asymmetric units of these crystals have been established by the molecular replacement method with computing techniques different from those used by Ward, Wishner, Lattman & Love [J. Mol. Biol. (1975), 98, 161-171] in their studies of human deoxyhaemoglobin crystals obtained from polyethylene glycol solutions. The calculations have been performed also with diffraction data from deoxyhaemoglobin and fluoromethaemoglobin + inositol hexaphosphate crystallized from polyethylene glycol by Fermi & Perutz [J. Mol. Biol. (1977), 144, 421-431]. In all cases, the individual dimers have been positioned independently and it is shown that, in the methods using a fast rotation function, three- and multidimensional residual-type translation functions may be directly applied to the structure determination of those complex structures in which the structure of only one of the two subunits present in the asymmetric unit is known. It is also shown that in all crystals studied the haemoglobin dimers are arranged in the \cal Y conformation, which seems to exclude the possibility of the full oxygenation of haemoglobin crystallized from polyethylene glycol solutions.
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  • 12
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 430-436 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A simple computer program for the simulation and analysis of X-ray back-reflection Laue photographs of a single crystal with any structure and orientation has been developed in Fortran IV. Comparison of computer plots of the calculated patterns with the photographs enables rapid identification of approximate orientation. The program may ultimately be used to index an orientation from the identification of at least three spots from the photographs. The procedure incorporating use of the program requires only minimal knowledge of crystallography or computer methods.
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  • 13
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 153-162 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Theoretical expressions for the complementary cumulative function of the Bijvoet ratio X applicable to a truncated data set are worked out for a non-centrosymmetric crystal containing P anomalous scatterers in the unit cell [P = 1 and many (MN and MC cases)] besides a large number of normal scatterers. These expressions contain the truncation limit yt as a parameter of the distribution. The results obtained are used to discuss the effect of data truncation arising from the non-observability of extremely weak reflections on the measurability of Bijvoet differences.
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  • 14
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 566-572 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Long one-dimensional magic-integer sequences are used to express the phases of 10-20 primary reflexions. The magic-integer representation of phases is extended to other secondary reflexions through strong triple- phase relationships involving one secondary and two primary reflexions. In the MAGEX procedure multiple magic-integer representations of the secondaries are sought and the error involved in their subsequent use in a conventional ψ map is much reduced. In view of the large number of primary reflexions the indices of the terms included in the ψ map are large and maps may be computed at up to 220 points. Further reflexions, in batches of ten or so, may be added to the initial set by the further use of magic integers and small-scale maps. When the base of estimated phases is sufficiently large then the phase information is extended by the controlled use of the tangent formula. Examples of the successful application of MAGEX are described.
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  • 15
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 578-584 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: FeSiF6.6H2O above 240 K is described following the structural model previously proposed for MgSiF6.6H2O above 300 K: periodic antiphase built on the ordered monoclinic cell of the low-temperature form. In the present case a progressive ordering is observed and the antiphase boundaries are no longer planar but exhibit steps which lead to a mean boundary canted with respect to the c hexagonal axis (space group P3). Above 240 K a phase transformation occurs with a threefold twinning and a significant lattice deformation. The monoclinic cell (P21/c) is described.
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  • 16
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 594-604 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A technique for improving the precision of crystal data collected on films or with electronic position-sensitive detectors is proposed. The extent of each medium or strong reflection is computed independently, after smoothing and filtering the individual intensities, producing a variable 'dynamic mask'. A method of calculating universal background profiles, which preserves the data and limits the necessary storage, is introduced. The method was applied to data collected with X-ray precession and oscillation techniques and to neutron data collected with a fiat-cone diffractometer equipped with a linear detector. In all cases substantial improvement in the precision of weaker reflections was observed. The overall quality of the data was particularly enhanced in the neutron diffraction case.
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  • 17
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 145-153 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Mixed crystals Pb3(PO4)2--Pb3(AsO4)2 are ferroelastic at low temperatures. The phase diagram contains three different phases a (paraelastic), \tt b and \tt c (both ferroelastic). The transformation \tt a-\tt b is first order for Pb3(PO4)2 and approaches second-order behaviour with increasing As content. The spontaneous strains and the birefringence follow approximately a Curie-Weiss law, with a corresponding order-parameter exponent β = ¼. The mutual high-temperature phases give diffuse X-ray reflections due to inelastic scattering. The soft-mode model is discussed for these results.
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  • 18
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A comparison of the two methods available for describing the puckering of five-membered rings - the Altona-Sundaralingam (A-S) [Altona & Sundaralingam (1972). J. Am. Chem. Soc. 94, 8205-8212] pseudorotation parameters τm, P and the Cremer-Pople (C-P) [Cremer & Pople (1975). J. Am. Chem. Soc. 97, 1354-1358] puckering parameters q, φ - shows that they are the same for all practical purposes but both have minor shortcomings. In the A-S method, the value of τm is somewhat dependent on the choice of the origin atom, while in the C-P method the normal to the mean plane, rather than being fixed, precesses as the ring puckering changes. We present here an exact procedure for obtaining the A-S parameters τm, P that correspond to the amplitude and phase of the Fourier wave of period 4π/5, thus making τm independent of the origin atom. Formulae are also given for the estimation of the standard deviations in the A-S and C-P parameters.
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  • 19
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 426-430 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Rotation and translation functions in reciprocal space, commonly used to find the orientation of a known molecular fragment and/or its position in the unit cell, are all identical or closely related to the function Q(R,t) = 〈|Eh|2|Ehp(R,t)|2〉h, where |Eh| is the observed normalized structure factor and Ehp(R,t) is the normalized structure factor for the partial structure, calculated for orientation R and position t. In this paper, this function is derived from statistical considerations without referring to a Patterson synthesis. From the centrosymmetric and noncentrosymmetric probability density functions, Q(R,t) = 1 + 2p2 and Q(R,t) = 1 + p2 are obtained, respectively, where p2 is the fraction of atoms (scattering power) that has been placed in the correct orientation and position in the unit cell. Alternative search functions, for instance using |Eh|4 instead of |Eh|2, are discussed.
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  • 20
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    Acta crystallographica 37 (1981), S. 697-701 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: For b.c.c. vanadium metal the integrated intensities of 80 independent reflections were measured by using a spherically shaped single crystal 0.241 (3) mm in diameter with Ag Kα radiation. It was confirmed that there are very small differences in integrated intensities between paired reflections, and these differences can be measured significantly beyond the experimental error. The ratios of the paired reflections are small than those obtained from platy crystals [Weiss & DeMarco (1965). Phys. Rev. A. 140, 1223-1225] but are in good agreement with those recalculated recently by means of the APW method [Wakoh & Kubo (1980). J. Phys. F. 10, 2707-2715].
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  • 21
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 711-722 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: 19 absolute atomic scattering factors were measured for imperfect copper single crystals with an accuracy of the order of ±0.05 electrons for reflections with sin θ/λ ≤ 0.7 Å-1. This data set is of significantly higher accuracy than those measured earlier with X-rays for imperfect single crystals. The experimental form factors for low momentum transfer are significantly smaller than the free-atom values. The corresponding deformation density shows a small pile up of charge between nearest-neighbour atoms. At the present level of experimental accuracy, none of the available band-structure calculations provides a satisfactory description of the measured form factors over the whole range of momentum transfer where effects due to bonding can be expected.
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  • 22
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    Acta crystallographica 37 (1981), S. 625-636 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A complete list of (3 + 1)-dimensional superspace groups is presented. These groups describe the symmetry of incommensurate crystal structures with a one-dimensional modulation. A short discussion is given of applications. Extinction rules and Bravais types are tabulated in order to facilitate the determination of the superspace-group symmetry.
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  • 23
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    Acta crystallographica 37 (1981), S. 642-644 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: To overcome the disadvantages of a small starting set in MULTAN a technique is described whereby a large number of phases are given random values with low weights and then refined by a weighted tangent formula. The effectiveness of the process depends quite critically on assigning suitable weights to phase estimates and on a fairly tight control of the refinement. Examples of the application of the method are given for a number of structures, many of which are difficult to solve by direct methods.
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  • 24
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    Acta crystallographica 37 (1981), S. 636-641 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A formula has been derived for the mean-square error in the phases of crystal reflections determined through the multiwavelength anomalous scattering method. The error is written in terms of a simple function of the positions in the complex plane of the 'centres' corresponding to the different wavelengths. For the case of three centres, the mean-square error is inversely proportional to the area of the triangle formed by them. The theoretical values are in good agreement with those obtained by earlier workers from computer simulations. The present method makes it easier to optimize the number and the actual wavelengths to be employed in the multiwavelength method. The maximum benefits of this method are expected in experiments employing synchrotron radiation or neutrons.
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  • 25
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    Acta crystallographica 37 (1981), S. 645-649 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The absolute values of all the nine elastic constants of acenaphthene single crystals, C12H10, belonging to the orthorhombic system, have been determined by the photographic method from the measurement of the intensities of thermal diffuse scattering observed in a series of Laue photographs taken with monochromatized Cu Kα radiation having no higher harmonics of λKα. The direct beam was recorded photographically after being absorbed through nickel foils of known thickness, its intensity being reduced by a factor of 106. Diffuse scattering domains near the reciprocal-lattice nodes 400, 080, 004, 105, 014 and 072 were investigated extensively. The diffusely scattered intensities were corrected for the general scattering, polarization and skew factors. Corrections for absorption, divergence and second-order diffuse scattering were found negligible. The values of the elastic constants in units of GN m-2, with e.s.d.'s in parentheses, are C11 = 11.05 (50); C22 = 10.26 (30); C33 = 9.40 (23); C44 = 4.25 (08); C55 = 3.69 (07); C66 = 4.87 (10); C12 = -1.93 (20); C13 = 3.34 (12); C23 = 2.34 (13). The accuracy of experimentally determined values of the elastic constants is discussed.
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  • 26
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    Acta crystallographica 37 (1981), S. 649-652 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Most tables of space subgroups of space groups are devoted to maximal subgroups. Although available tables of maximal subgroups are complete with regard to translationengleich subgroups, they are inaccurate concerning klassengleich subgroups. As a matter of fact, these tables do not show that several klassengleich subgroups relevant to the same set of basis vectors may be distinguished by non-congruous origins.
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  • 27
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    Acta crystallographica 37 (1981), S. 658-661 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: New, finite and exact relationships between products of two normalized structure factors, with coefficients which are a function of the squared moduli of structure factors, are presented. The equations allow new linear relationships between the cosine and sine of triple-phase invariants to be set up. The meaning of the new equations is discussed in connexion with the direct calculation of cosines of triple-phase invariants and the results show, for simple one-dimensional model structures, that it is possible to obtain exact solutions.
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    Acta crystallographica 37 (1981), S. 653-658 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Two germanium polymorphs of the diamond type and the ST-12 structure were used to investigate the accuracy of extended X-ray absorption fine structure (EXAFS) analysis with a phase-difference method. This method gives similar accuracies to both conventional curve-fitting and Fourier-transform methods in determining the difference of the first- neighbor distances for these two polymorphs. The number of first-shell atoms of the ST-12 structure was determined to be 4.0 ± 0.2 with the diamond-type phase as a standard. In addition, the first-neighbor coordination of amorphous germanium was analyzed with this method. These results suggest that the phase-difference method is useful for structure analysis of materials and that it is especially useful for structure analyses under high pressure.
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  • 29
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    Acta crystallographica 37 (1981), S. 754-762 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A new type of satellite has been observed in plagioclases CaxNa1 - x[Al1 + xSi3 - xO8] with 0.5 ≤ x ≤ 1. Their intensities are such that they could be observed only by applying a special focusing technique. They appear in the neighbourhood of some strong reflections with h + k = 2n, l = 2n. It is shown that the new satellites are most probably caused by a three-dimensional array of domains of two structures, differing only by small displacements of the atoms. Since the translation lattices of the two structures have the same geometry it is concluded that the two structures are twins of an acentric plagioclase correlated with a centre of symmetry. The size of the domains is 80 Å approximately. The diffraction of such submicroscopically intergrown twins is calculated for lamellae and blocks and compared qualitatively with the experimental results. The approximate periodicity of the domains could be destroyed by very long exposure to X-rays.
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  • 30
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    Acta crystallographica 37 (1981), S. 742-754 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: In a previous paper [Khachaturyan, Semenovskaya & Vainshtein (1979). Soy. Phys. Crystallogr. 24, 519- 524], the thermodynamic formulation of the procedure of crystal structure determination from the intensity array of X-ray reflections was proposed. This approach requires the introduction of analogues of such thermodynamic functions as the free energy, entropy, temperature and so on, and it is reduced to the solution of the specific 'kinetic equation'. It was shown that the equilibrium state of the system is described by the distribution of the scattering substance density which at low temperature corresponds to the true structure of the crystal. The problem of crystal structure determination is thus reduced to determination of the equilibrium distribution of the scattering substance. The Önsager equation formalism was applied to derive 'kinetic equations' describing the relaxation of the system to its equilibrium state. The test of the proposed procedure exemplified by the solution of the 'kinetic equation' to determine the crystal structure of l-proline, C5H9NO2, with 32 atoms per unit cell is considered.
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  • 31
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 764-765 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Expressions are derived for estimating the standard deviations of Cremer-Pople ring-puckering coordinates, with the assumption that the e.s.d.'s of the atomic positions are approximately isotropic.
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  • 32
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    Acta crystallographica 37 (1981), S. 767-767 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
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  • 33
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    Acta crystallographica 37 (1981), S. 765-766 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Maxima and minima are tabulated for the Bessel functions Jn(x) for values of n from 0 to 30 [i.e. zeros of J'n(x)]. The first six points are recorded for each function. The table considerably extends the range of earlier tables available in the literature. It should have applications in the interpretation of diffraction patterns from helical or wave-form structures or features, and has been used in connection with some electron microscope images.
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  • 34
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    Acta crystallographica 37 (1981), S. 684-689 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A figure of merit DELCRI, with estimates Δ3 for the absolute values of the triplet phase sums φ3, is described for the selection of numerical values of symbols used in a symbolic addition procedure. From tests with a number of structures crystallizing in polar space groups this figure of merit was found to enable the selection of enantiomorph-specific phase sets.
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  • 35
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    Acta crystallographica 37 (1981), S. 491-500 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The combination of phase information obtained by the method of isomorphous replacement with that calculated from a partial model of the structure has proved to be a powerful tool in the interpretation of the structure of horse muscle phosphoglycerate kinase. That the combined phases are an improvement on the calculated or isomorphous ones is evidenced by more readily interpretable electron density maps, which show only a low level of feedback from incorrectly located atoms. Several different types of Fourier syntheses have been calculated using the combined phase angles and an essentially qualitative evaluation of their relative merits is presented.
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  • 36
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    Acta crystallographica 37 (1981), S. 500-506 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: All complete pattern shift lattice (DSC-lattice) translations of one lattice with respect to the second lattice of a bicrystal are described as a group. It is shown that the matrix representation of this group can be used to solve topological problems connected with secondary grain boundary dislocations (SGBD's) such as finding the step in the boundary associated with the SGBD. We have formulated this problem by establishing the 'step vector' S associated with the Burgers vector b of the SGBD in a cubic bicrystal. The problem is then solved in 2D, and the way to generalize to 3D is indicated.
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  • 37
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    Acta crystallographica 37 (1981), S. 511-516 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A general theory of the diffuse scattering which has previously been developed on the basis of a microdomain model [Hashimoto (1974). Acta Cryst. A30, 792-798] is applied to the three special cases in which the microdomains have the ordered structures denoted by L12, L10 and L11. The practical intensity formula is presented in each case, which can be used to obtain, from the observed X-ray intensity distribution, the statistical nature of the microdomains; the average size, the size distribution, the number density and the spatial interdomain correlation.
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  • 38
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    Acta crystallographica 37 (1981), S. 517-525 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A set of symbols based on the minimum subset of Seitz matrices required to generate the complete symmetry may be derived for each of the three-dimensional crystallographic space groups. This has a number of desirable properties including explicit information on the choice of origin. It also leads to a simple and general algorithmic procedure for generating equivalent positions.
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  • 39
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    Acta crystallographica 37 (1981), S. 507-510 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The magnitudes of the electric field gradients at all atomic positions in Li3N are known from NQR experiments. High-temperature NQR data indicate the gradients at Li(1) and Li(2) to be of opposite sign. In this paper, we calculate the field gradients from X-ray data and refine the parameters of the multipole deformation functions together with scale, extinction and temperature factors against X-ray and NQR data simultaneously, assuming various sign combinations for the gradients at Li(1), Li(2) and N. Despite an ill-defined scale factor of the X-ray intensities, negative signs at both Li(2) and N are obtained, and the sign at Li(1) is thus positive. The same signs are obtained from an ionic point-charge model. The extinction correction is important and dependent on the assumed signs. The model deformation map for the signs +, -, - at Li(1), Li(2) and N shows nearly spherical Li ions, whereas N appears to be strongly polarized perpendicular to c. With the assumption of the incorrect negative sign at Li(1), a strongly polarized Li(1) ion but approximately the same reliability indices for the X-ray data are obtained. Inclusion of NQR data in the charge-density refinement results in a better definition of the quadrupolar components of the deformation density close to the atomic centres.
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  • 40
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    Acta crystallographica 37 (1981), S. 525-529 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A general expression for the diffracted intensities from an aggregate of partially disordered layer structures consisting of plane lattice layers displaced randomly along a and b by arbitrary fractions a/qa and b/qb has been worked out. The approach is similar to that of Wilson [X-ray Optics (1962). London: Methuen] and has been followed by Ray, De & Bhattacherjee [Clay Miner. (1980), 15, 393]. The expression is very general in nature and is suitable for studying the variation of intensities from such crystallites with any amount of displacements. Numerical computations for several cases have been carried out and results discussed. It is concluded that the peak will broaden and background increase as the magnitudes and probabilities of disorder increase.
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  • 41
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    Acta crystallographica 37 (1981), S. 548-552 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A new relationship between products of two structure factors with coefficients calculated as the Fourier transform of a modified Patterson function is presented. The relation is alternatively expressed in terms of triple phase invariants and also a new weighted form of Sayre's equation [Sayre (1952). Acta Cryst. 5, 60-65] emerges as a special case. The advantages of the new equations with respect to Sayre's equation are discussed and, with simple one-dimensional models, examples of direct calculation of the cosines of triple-phase invariants are included.
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  • 42
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    Acta crystallographica 37 (1981), S. 529-535 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The lattice energy of isolated, regular tetrathiafulvalene (C6H4S4) and tetracyanoquinodimethane (C12H4N4) segregated and mixed stacks was minimized for four structural parameters; a longitudinal and transverse slip of neighbouring molecules relative to each other, a rotation of a neighbouring molecule perpendicular to the molecular planes and the perpendicular distance between two neighbouring molecules. The van der Waals and repulsive interactions only were calculated from atom-atom potentials. The absolute minima of the lattice energies were achieved at stack structures slipped longitudinally with all stack parameters deviating less than about 0.1 Å from their observed mid-range values. The mixed stack proved to be less stable than the segregated stack only by about some tenths of a kJ mo1-1. Additional local minima were found for the segregated tetrathiafulvalene stack and for the mixed stack, which are not (yet) observed experimentally. The eclipsed tetrathiafulvalene stack and the tetracyanoquinodimethane stack with transverse slip, both of these observed experimentally, could not be predicted within a one-dimensional isolated stack model.
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  • 43
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    Acta crystallographica 37 (1981), S. 536-547 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: If a mixed organic solvent is added to a ribosome solution and stored at 277 K in a crystallization chamber, thin lamellae of a few μm diameter can be obtained. Under the electron microscope, tetragonal face-centred macrocells of b = 40 and c = 55 nm are visible. These findings are substantiated by X-ray small- and wide-angle diffraction which leads to macrocells of b = 42 and c = 52 nm and establishes the third dimension of the macrocell with a = 42 nm. Mainly 0kl reflections appear. From their line widths, it follows that each lamella consists of at least 15 × 15 × 15 macrocells with small paracrystalline distortions gs - 1.5%, whilst their 6 × 8 × 12 subcells with a0 = 7.1, b0 = 5.3 and c0 = 4.3 nm have large fibrillary distortions in the bc plane, similar to the aggregation of microparacrystals in stretched and annealed polymers. With a new method, the folding root of the Q function projected on the b axis can be analysed. Two compounds are placed in each macrocell, each consisting of about 136 cylinders of about 2.0 nm diameter and 7 nm length. They are aligned to fibrils of different lengths orthogonal to the bc plane and occupy about 47% of the macrocell. The residual volume is filled up with an 'amorphous phase' as in semicrystalline polymers. A comprehensive study of the existing literature leads to the conclusion that the 'crystalline phase' consists of two 70S ribosome tetramers and that the cylinders are obviously parts of two-stranded helices, whilst most of the RNA proteins are in the 'amorphous phase'. The biological significance of the ribosome crystals and the paracrystalline sublattice is described in detail in the Discussion.
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  • 44
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    Acta crystallographica 37 (1981), S. 553-557 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: An efficient algebraic algorithm is described for determining unit cells. It can be directly implemented on a digital computer. Two practical examples of its use are given: the determination of a unit cell on the (hkl) plane and the enumeration of the lattice points contained in a non-primitive cell. Both examples can be performed easily by hand; when performed by computer, they achieve a considerably higher computational speed than any other known methods.
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  • 45
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    Acta crystallographica 37 (1981), S. 573-578 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: On the basis of electron-density considerations, graphic explanations are given of triplets and positive and negative quartets. It is shown that the number of useful negative relations will always be much smaller than the number of useful positive relations.
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  • 46
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    Acta crystallographica 37 (1981), S. 558-565 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The intensities of the weak superlattice reflections in the UX3 compounds, where X = Ru, Rh, Ge, and Sn, have been measured by neutron diffraction. These compounds have the ordered AuCu3 structure. Excellent fits to the observed intensities are obtained by introducing anisotropic second-order and fourth-order (anharmonic) terms to describe the probability distribution function at the X atom site. The ratio of the magnitude of the mean-square thermal vibration parallel to and perpendicular to the unique tetragonal axis of the X atom appears to depend on whether p bonding (UGe3, USn3) or d bonding (URu3, URh3) occurs with the U electrons. In UGe3 data out to Q = 13 Å-1 show the need to include a fourth-order anharmonic term. The form of this anharmonicity suggests an attractive potential between the nearest- neighbor U-X atoms.
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    Acta crystallographica 37 (1981), S. 851-856 
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    Notes: Within the Debye approximation the temperature-dependent correlations of atomic vibrations are shown to involve essentially a single integral which is a function of two parameters. A tabulation of this integral is presented, together with high- and low-temperature expansions. A comparison with much more elaborate calculations for real crystals suggests that the simple method described might be accurate to 2̃0%.
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  • 48
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    Acta crystallographica 37 (1981), S. 848-850 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Authoritative values for the parameters of harmonic thermal motion have been used as criteria for various least-squares refinements of the structure model for beryllium metal. A change in the absolute scale of Brown [Philos. Mag. (1972), 26, 1377-1394] improves the correspondence of the associated data with the true thermal parameters. Contraction of the core-electron distribution upon bonding is a possible implication of the rescaled data.
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  • 49
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    Acta crystallographica 37 (1981), S. 863-871 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: TDS profiles convoluted with the instrument resolution were obtained by forming differences between diffraction profiles measured with neutrons of wavelength 0.60 Å on three perfect Si crystals of different thickness. The profiles were measured with two detector apertures for the reflections 022, 004, 044, 026, 008 and 066. From these measurements TDS correction factors α and hence a correction term ΔB for the temperature parameter of Si were derived. The temperature parameter of Si was determined for two temperatures, 92 and 292 K, as B92 = 0.212 (3) Å2 and B292 = 0.422 (3) Å2, respectively, from the refinement of 100 symmetry-inequivalent reflections measured with neutrons of wavelength 0.53 Å on an imperfect Si crystal.
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    Acta crystallographica 37 (1981), S. 857-863 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A procedure for joint refinement of X-ray and neutron data is described in which structural, charge density and extinction parameters are adjusted simultaneously in order to arrive at the best least-squares solution with respect to all available diffraction data. This X + N refinement is applied to previously collected low-temperature data on oxalic acid dihydrate, C2H2O4.2H2O, and results are compared with the X-ray-only refinement, and an X-ray refinement with neutron values for the hydrogen structural parameters. The X + N model deformation density shows higher peak heights in the lone-pair regions than the X- ray-only model density and resembles more closely the X-N deformation maps. Though the X + N maps are more strongly model dependent, they contain less noise, provide an analytical description of the deformation density and, unlike the X-N density, can be obtained in principle with a less than complete data set. The estimate of the goodness-of-fit for each of the data sets requires an apportioning of the joint parameters, which in this study is based on the relative magnitude of the least-squares derivatives.
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    Acta crystallographica 37 (1981), S. 899-903 
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    Notes: The structure factor of librating or orientationally disordered molecules with isotropic Gaussian distribution functions is calculated exactly by numerical integration. The computer program with an example is described. The results are compared with approximation methods which correspond to a cumulant expansion of the structure factor. The application to the refinement of the plastic phases of C2Cl6 and SF6 is shown. The influence of anharmonic distributions is considered. The method is compared to the analysis with spherical cubic harmonics.
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    Acta crystallographica 37 (1981), S. 876-889 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Multiple simultaneous Bragg diffraction effects of X-rays in quaternary III-V liquid-phase epitaxial thin layers are investigated with both photographic and counter detection methods. For the photographic investigation, a divergent source is used. The geometric aspects of this type of diffraction, affected by lattice mismatch between epitaxial layers and substrates, are discussed for cases involving five-, six- and eight-beam reflections. The lattice mismatches in directions parallel and perpendicular to the interface normal of InGaAsP/ InP, determined from a single divergent-beam photograph, are obtained. For the counter detection study, a collimated incident beam and several single and double heterojunction samples, with large lattice mismatches are used. A kinematical treatment for a general n-beam diffraction, from double- and triple-layer systems, is derived to account for the measured intensities.
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    Acta crystallographica 37 (1981), S. 871-875 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The rate and mechanisms of growth and the final quality of crystals are related to lattice disorders and can be studied from the analysis of X-ray diffraction patterns. Crystals of proteins and other biological macromolecules display features which are different from those of inorganic crystals. In this work the long-range order of protein crystals is probed via the mosaic spread, with a special camera constructed for this purpose. The very small mosaic spread measured indicates almost perfect long-range order in the crystal, suggesting the absence of dislocations. This is compatible with the weak binding energies and mechanical softness of protein crystals. If indeed such crystals do not incorporate dislocations, accumulation of strain may be a possible mechanism for the cessation of growth of protein crystals. Microscopic observations of crystal growth support this idea.
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    Acta crystallographica 37 (1981), S. 889-899 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: In the most general case the orientation distribution of crystals in a polycrystalline sample is to be described by a function of orthogonal transformations which splits up into two functions of rotations corresponding to right- and left-handed crystals. The properties of these functions are influenced by crystal and sample symmetry. The rotational subgroup of crystal symmetry leads to symmetry relations which may be written in the form of selection rules. Elements of the second kind of the crystal symmetry give rise to a determinability condition, according to which the texture function may be split into a part \tilde{f}(g) which can be determined from polycrystal diffraction experiments and a part \tilde{\tilde{f}}(g) which cannot. The determinability condition may take on three different forms according to whether the crystal symmetry contains a centre of inversion, a mirror plane or a \bar 4 inversion axis. In the case of normal scattering the Laue symmetry is to be considered instead of the true crystal symmetry. The sample symmetry is to be described by a black-white or Shubnikov group containing four kinds of elements which give rise to four kinds of symmetry conditions in the function f(g). The sample symmetry may be a conventional one consisting of one-to-one relationships between crystal orientations. It may, however, also be a non-conventional one defined by an integral relation between an infinite number of crystal orientations.
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    Acta crystallographica 37 (1981), S. 908-913 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Three semiempirical atom-atom potential functions suggested by different authors to describe non-bonded Cl...Cl interactions are examined via calculation of some thermodynamic properties of hexachloro- benzene, C6Cl6, and p-dichlorobenzene, C6H4Cl2, crystals. All thermodynamic quantities are evaluated with the cell model as a statistical mechanical basis. The calculation results provide some evidence to support the existence of positional disorder in the high-temperature phases of p-dichlorobenzene.
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    Acta crystallographica 37 (1981), S. 913-915 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Simple inspection of the reduced form of a unit cell can fail to detect the correct lattice symmetry, because of the effects of measurement errors, computer rounding errors and uncertainties in interpretation of almost equal numbers. A procedure which is insensitive to these effects consists of the generation of a list of lattice vectors sorted on length, together with angles between pairs of them. The list includes the edges, face diagonals and body diagonals of the reduced cell, and the sums and differences of any of these which are similar in length. The correct unit cell is easily recognized in the vector list.
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    Acta crystallographica 37 (1981), S. 904-908 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Bragg intensity data extracted from energy-integrated neutron measurements were treated by a conventional split-atom model, with a series expansion in cubic harmonic functions, and by a Gaussian approximation for the molecular librations. The trigonal molecular axes are found to be smeared out close to cubic [111] axes with the Cl atoms near the [100] axes. With the three models mentioned consistent data are obtained for the root-mean-square translational amplitude: 0.4 Å, and the librational amplitude: 19.6°; both at 423 K. Data and results for three different temperatures are given.
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    Acta crystallographica 37 (1981), S. 916-920 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Accurate neutron-diffraction data from a highly perfect crystal of SrTiO3 have been used to assess the extinction model of Becker & Coppens [Acta Cryst. (1974), A30, 129-147, 148-153; Acta Cryst. (1975), A31, 417--425] in refining reliable thermal parameters from data very strongly affected by extinction. The model incorporates approximations not evidently reasonable in this case - namely, the (usual) kinematical approximation and the mosaic-block description of crystal microstructure. However, it is shown that a careful choice of parameterization within the overall motel (e.g. between a Gaussian and a Lorentzian function for the distribution of mosaic-block orientations) can yield a uniformly good description of the extinction per se - except for reflections extinguished by more than about 90% on intensity. The refined thermal parameters are in remarkably good agreement with values obtained independently from lattice-dynamical calculations.
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    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 921-921 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: In Hall [Acta Cryst. (1981). A37, 517-525] there are two errors in Table 7 on page 524. The proposed notation for proposed orders 144 and 157 should be P\bar 3 and \bar P32.
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    Acta crystallographica 37 (1981), S. 921-921 
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    Acta crystallographica 37 (1981), S. 921-921 
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    Notes: In Table 2 of Parthasarathy & Ponnuswamy [Acta Cryst. (1981), A37, 153-162], for every value of k, the row against yt = 0.3 for P = 1 and the row against yt = 0.3 for P = MC are to be interchanged. All relevant information is given in the Abstract.
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    Acta crystallographica 37 (1981), S. 922-941 
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    Acta crystallographica 37 (1981), S. 943-944 
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    Acta crystallographica 37 (1981), S. 943-943 
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    Acta crystallographica 37 (1981), S. 942-943 
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    Acta crystallographica 37 (1981), S. 944-944 
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    Acta crystallographica 37 (1981), S. 944-944 
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    Acta crystallographica 37 (1981), S. 944-944 
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    Acta crystallographica 37 (1981), S. 92-96 
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    Notes: The energy dependence of the integrated intensities Ih(ω) and Ih(ω) and of their ratio rh(ω), around an absorption edge, are greatly affected by thermal vibrations of atoms. This has been experimentally shown by the present energy-dispersive diffractometry for a mosaic crystal of CuI, for which thermal vibrations are especially large even at room temperature. The temperature factor values BCu = 3.3 ± 0.1 and B1 = 2.0 ± 0.1 Å2 have been determined in the following way: the f”Cu(ω) curve has been determined from the absorption curve, and therefrom the f'Cu(ω) curve has been calculated by the dispersion relation. By the use of these curves, the intensity curves I555(ω) and I{\bar 5}{\bar 5}{\bar 5}(ω) were obtained, and then the temperature factors were determined by finding the best fit between the above I(ω) curves and the observed one. Also, the experimental fine structure of the Friedel ratio r5(ω) is shown as a function of energy and compared with the calculated values.
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    Acta crystallographica 37 (1981), S. 135-137 
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    Notes: A straightforward method using Legendre series enables the orientation distribution in a specimen with uniaxial symmetry to be derived from the azimuthal profile of a single arbitrary reflection. Moreover, the moments of the distribution (P2n(cosα) can be obtained directly from the azimuthal profile without needing to calculate the complete distribution.
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    Acta crystallographica 37 (1981), S. 138-138 
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    Acta crystallographica 37 (1981), S. 141-141 
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    Acta crystallographica 37 (1981), S. 143-143 
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    Acta crystallographica 37 (1981), S. 144-144 
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    Acta crystallographica 37 (1981), S. 97-104 
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    Notes: X-ray diffraction of plastic crystals is investigated by using the decomposition of the orientational average density of the atoms on symmetry-adapted functions. For a cubic lattice, the molecular librational amplitude is related to the order of the cubic harmonics to be used. For a rigid molecule with 3m symmetry in a cubic lattice, the symmetry-adapted functions and the rotator functions are given up to order 12. The plastic phase structure of 1-cyanoadamantane, C11H15N, which is f.c.c., Z = 4 and a = 9.813 (3) Å, has been studied in the Fm3m space group. The orientational average density of the cyano group has a very sharp maximum in the [001] directions not completely describable (Rw = 15.4%) with cubic harmonics of order only up to 12. All the results obtained with this method agree very well with the corresponding ones from the Frenkel model structure of this compound.
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    Acta crystallographica 37 (1981), S. 242-249 
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    Notes: Summation of the components of interactomic vectors, rn, normal to a crystallographic plane, (hkl), divided by the area of the periodic repeat unit over which the vectors operate, provides a quantity, σn, (hkl), defined as an interaction factor. If all values of σn for a given interatomic vector are plotted in the directions normal to all planes in the structure, the result is a structural quadric, with geometric properties analogous to representation quadrics for single-crystal properties. All the atomic interactions in a crystal can thus be represented by a group of quadrics having common semiaxes. It is proposed that crystal properties are a function or functions of the structural quadrics and calculations incorporating some simplifying assumptions are presented to indicate possible applications of the concept.
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    Acta crystallographica 37 (1981), S. 139-140 
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    Acta crystallographica 37 (1981), S. 142-142 
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    Acta crystallographica 37 (1981), S. 143-144 
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    Acta crystallographica 37 (1981), S. 144-144 
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    Acta crystallographica 37 (1981), S. 162-169 
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    Notes: An a priori approach to the prediction of required neutron beam time for single-crystal analysis of biological structures is presented. Time economy is determined by several main features: (i) tolerable inaccuracy of the Fourier map, (ii) method of extracting phase information, (iii) data-collection technique. Phasing by anomalous scattering at two wavelengths is considered. An expression is derived for the error in scattering density arising from experimental intensity errors. Application of the theoretical probability distributions for the intensities leads to an equation for the expected total counting time. Conditions are established for which the time expenditure is a minimum. Tables which aid easy application of the results are given as well as a numerical example.
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    Acta crystallographica 37 (1981), S. 184-189 
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    Notes: Crystallographic data concerning geometric properties of hexagonal lattices of Cα, Zn, Beα, Tiα, Zrα, Mg and Cd are obtained from two different computation techniques. These properties are related to the relative orientations of identical hexagonal lattices 1 and 2 which superimpose two multiple cells M1 and M2 within a given small deformation. These orientations are listed for ratios Σ = | volume of cells M1 (or M2)/volume of the unit cell | varying from 1 to 25. Their number are limited by choosing all the principal strains transforming M1 into M2 less than or equal to 1%.
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    Acta crystallographica 37 (1981), S. 314-324 
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    Notes: The calculation of the amplitude of X-rays scattered by a magnetically ordered substance, carried out in the relativistic quantum theory (i.e. taking the spin into account), is detailed. The effect of the orbital momentum is described in an appendix. The practical formulae dealing with the polarization of the beams are given both in a simple form for the usual experiments and in a complete form, using the Stokes vectors, for the most general case. The experiments show a change in the intensity of the X-rays diffracted by a ferromagnetic (pure iron) or a ferrimagnetic (zinc-substituted magnetite) powder when the magnetization, perpendicular to the diffraction plane, is reversed. The relative values of these intensity changes range from 10-4 to 5 x 10-3 and agree in sign and magnitude with the predictions. They are proportional to the spin-density structure factor multiplied by the imaginary part of the charge- density structure factor; the large anomalous scattering of the Cu Kα radiation in the iron-containing samples is used in the present experiments.
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    Acta crystallographica 37 (1981), S. 391-397 
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    Notes: The reflecting and transmitting powers of a plane-parallel crystal composed of mosaic blocks of varying orientation and thickness are derived from dynamical theory in the symmetrical transmission case. The assumptions necessary to arrive at results coinciding with those obtained from Darwin's transfer equations are discussed in detail. The influence of a secondary reflexion is studied by solving the Darwin equations in the three-beam case. Numerical criteria to estimate the conditions under which the effect of secondary reflexion is negligible are presented.
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    Acta crystallographica 37 (1981), S. 398-406 
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    Notes: A new translation function T(t) is defined, whose main peak is expected to give directly the absolute position t = t0 of a known molecular configuration (the isostructural model) of known orientation in an unknown crystal structure. T(t) combines all required information: crystal symmetry, molecular steric properties of the model and experimental data (observed structure factors Fo) leading to more reliable results: T(t) = TO(t)/O(t), where TO(t) measures the degree of agreement between Fo and Fc(t), while O(t) is a function measuring intermolecular overlap. TO and O can both be computed efficiently by the possibility of their expansion in Fourier series, and the use of FFT. A theoretical study followed by application to a simple synthetic structure cast light upon ambiguities and failures [e.g. Bott & Sarma (1976). J. Mol. Biol. 106, 1037-1046] encountered in using translation functions previously described [e.g. Crowther & Blow (1967). Acta Cryst. 23, 544-548]. The crystal structure of the high-temperature form of hen-egg-white lysozyme was determined at 6 Å resolution by the application of this fast translation function and compared with the equivalent structure obtained by the isomorphous replacement method.
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    Acta crystallographica 37 (1981), S. 332-335 
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    Notes: Multipole interactions arising out of the interband and intraband transitions of electrons occupying d shells are analysed classically. The ion-ion and volume interactions are modified and an equilibrium condition is derived on simple and realistic lines. A model incorporating these features is employed to discuss the dispersion relations in b.c.c. transition metals like tantalum and vanadium.
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    Acta crystallographica 37 (1981), S. 353-360 
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    Notes: Abstract Theoretical expressions for R2 and RN2, indicator functions used in automated structure analysis, are given for space groups P1 and P\bar 1 as a function of σ21 = ΣPj = 1 f2j/ΣNj = 1 f2f (P is the number of atoms in the tentative structural model) and of a threshold a on the intensity data. It appears that R2 is only slightly dependent, RN2, however, is strongly dependent on a. If low-intensity reflections are eliminated from the data set, R2, and not RN2, thus remains a useful control function in testing the reliability of atomic positions Theory and experiment are shown to be in good agreement.
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    Acta crystallographica 37 (1981), S. 143-143 
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    Acta crystallographica 37 (1981), S. 144-144 
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    Acta crystallographica 37 (1981), S. 438-438 
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    Notes: Two misprinted equations in International Tables for X-ray Crystallography, Vol. IV [(1974). Birmingham: Kynoch Press], should be corrected.
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    Acta crystallographica 37 (1981), S. 437-437 
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    Notes: The anisotropic functional form previously suggested for the variation of reflexion peak width in reciprocal space does not adequately deal with cases of high anisotropy when measurements are made at different azimuthal angles. A small modification procedures considerable improvement.
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    Acta crystallographica 37 (1981), S. 443-444 
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    Acta crystallographica 37 (1981), S. 439-440 
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    Notes: The polarization ratio is expressed by |cos 2θ|n, where 2θ is the angle between the incident and the diffracted rays. For a perfect uniblock single crystal, n is usually taken to be equal to 1. For an ideally imperfect crystal, n is taken to be 2. Any other value of n is attributed to the extent of mosaicity. Numerical computation of the polarization ratio for a perfect nonabsorbing single crystal of infinite lateral extension but finite thickness shows that n, instead of having the constant value of 1, may have any value between 1 and 2, depending on the thickness of the slab, the structure factor of the reflecting plane, the volume of the unit cell and the angle of scattering. The numerical computations are based on Zachariasen's theory of diffraction of X-rays by perfect crystals [Zachariasen (1945). Theory of X-ray Diffraction by Crystals. New York: John Wiley].
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    Acta crystallographica 37 (1981), S. 445-445 
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    Acta crystallographica 37 (1981), S. 446-446 
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    Acta crystallographica 37 (1981), S. 448-448 
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    Acta crystallographica 37 (1981), S. 447-448 
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    Acta crystallographica 37 (1981), S. 819-826 
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    Notes: Disorder in both allotropic phases of pure single-crystalline cobalt was studied by elastic neutron scattering in order to separate bulk from surface effects and to remove diffuse inelastic contributions. The intensity variation along 10l, measured at different temperatures, was analysed quantitatively in terms of Jagodzinski's disorder theory. The values found for the degree of disorder in the h.c.p. phase were lower than those reported before for powder samples and remain nearly unaffected when approaching the transition temperature. The f.c.c. phase is always (below and above the transition) well ordered. However, the temperature behaviour of the f.c.c. and the h.c.p. precursor regimes in the h.c.p. and the f.c.c. modifications, respectively, is different. The connection between disorder and the martensitic h.c.p.-f.c.c. transformation is discussed.
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    Electronic Resource
    Electronic Resource
    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 37 (1981), S. 826-837 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: X-ray structure factors of MgF2 were derived from accurate measurement of single-crystal diffraction intensities. The crystal charge density was analyzed in terms of multipole expansions centered at the ionic sites. Separation of electronic and dynamic deformations was effected by using, in the difference series calculations, anisotropic Debye-Waller factors obtained in the neutron diffraction study of Vidal- Valat, Vidal, Zeyen & Kurki-Suonio [Acta Cryst. (1979), B35, 1584-1590]. The charge density was found to be composed of well defined local Mg2+ ions and slightly enlarged and more diffuse F- ions with 0.50 electrons distributed more widely in the unit cell. Nonspherical deformations of electronic origin were found significant up to fourth order, with the exception of the vanishing dipole moment of fluorine. These deformations emphasize the ionic nature of the crystal by violating the symmetry of the immediate surroundings and by decreasing the charge density in all of the octahedral bonding directions of Mg2+ down to typical ionic values.
    Type of Medium: Electronic Resource
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