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  • Oxford University Press  (3,171)
  • International Union of Crystallography (IUCr)  (1,004)
  • American Meteorological Society (AMS)
  • 1980-1984  (4,175)
  • 1981  (4,175)
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  • 1980-1984  (4,175)
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  • 101
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 145-145 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Crystal data for 5-hydroxy-7-methyl-1,4-naphthoquinone, C11H8O3, are reported. The crystal is monoclinic with space group P2, Pm or P2/m.
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  • 102
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 149-151 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The Rietveld [J. Appl. Cryst. (1969), 2, 65–71] method of structure refinement from powder diffraction patterns is widely used with neutron data and increasingly so with X-ray data. A computer program for the application of the method with X-ray data, or with neutron nuclear scattering data, has been written ab initio in an effort to make it versatile, user oriented, portable, convenient, and largely self-contained yet reasonably comprehensive. It is of modular construction to facilitate user-desired modifications, one of which may be additions to the choice of four profile functions now included. The program accommodates either one or two wavelengths (e.g. α1 and α2 or λ and λ/2). It permits simultaneous refinement of the structures of two phases and the background.
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  • 103
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 153-154 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
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  • 104
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 154-155 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
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  • 105
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 157-159 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: If a powder pattern consists of well resolved peaks, and if it is adequately described by a crystallographic model, as determined by statistical tests, the estimates of the parameters and their standard deviations will not be significantly different, in a statistical sense, whether the method of refinement uses peak profiles or integrated intensities. If the model does not fit adequately, the standard deviations cannot be calculated by statistical methods. If peaks overlap, there are correlations between the intensities of the individual peaks that are handled automatically in the profile method, but must be included explicitly in the integrated-intensity method. A background function should be included in the model, and its parameters refined. The background parameters have correlations with other parameters that become important if the pattern is complex, and therefore poorly resolved.
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  • 106
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 185-190 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A one-dimensional long-period superstructure (1d − LPS) of Au–24 at.% Cd alloy has been investigated at the atomic level with a 1 MV electron microscope. Simple images interpretable in terms of the 1d − LPS of DO23 type are observed; the cadmium atom positions appear as a regular out-of-step configuration of bright dots with the spacing of the lattice constant (4.1 Å) of the basic f.c.c. cell. This is called a superstructure image. The formation of the superstructure image is studied as functions of specimen thickness and defocus on the basis of n-beam multislice calculations.
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  • 107
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 209-210 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Indexed powder patterns of three monoclinic compounds of general formula (BH)3H3V10O28 . xH2O, (C6H8N)3H3V10O28.xH2O, where 0.5 ≤ x ≤ 2 and B = 2-methylpyridine (J2), 3-methylpyridine (J3) and 4-methylpyridine (J4), are given. The lattice parameters of the unit cells with two molecules are: J2a = 10.263 (8), b = 14.253 (7), c = 16.229 (8) Å, β = 104.36 (5)°; J3a = 13.108 (3), b = 20.633 (5), c = 8.363 (1) Å, β = 104.31 (2)°; J4a = 11.003 (3), b = 22.869 (6), c = 9.569 (3) Å, β = 98.03 (2)°.
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  • 108
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 212-213 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The structure of the phase PdAl4 is isotypic with PtAl4. The hexagonal unit-cell parameters are: a = 13.085 (1), c = 9.633 (1) Å. X-ray powder diffraction data are reported.
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  • 109
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 216-217 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
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  • 110
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 218-218 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
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  • 111
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 230-233 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The ability of the vector method to determine the complete orientation distribution function (ODF) with pole figures will be demonstrated for a particular case. A comparison of the results obtained by the vector method and the series expansion method will be presented.
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  • 112
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 383-386 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A method of deconvolution using the modulus of the continuous Fourier transform of the unit cell is described. This method differs from previous deconvolution methods in membrane diffraction in that calculations are carried out in reciprocal space. The modulus profile is obtained from the continuous intensity transform which is itself the Fourier transform of the autocorrelation function. Sampling theorem methods are used to reconstruct the continuous Fourier transform of the unit cell. The various phase choices are examined and compared. In membrane diffraction, the autocorrelation function is derived in two distinct situations: when the interference function is broad as in the case of a few unit cells and when the membrane systems contain wide regions of constant electron density. It is concluded that, in the first situation, the derived autocorrelation function contains missing information and is incorrect. On the other hand, in the second situation, the derived autocorrelation function is a good representation of the true autocorrelation function.
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  • 113
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 401-416 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The measurements and calculations of the charge, spin and momentum density of the metallic elements Ti to Ni are examined. Both the Compton profiles (momentum density) and X-ray scattering factors (charge density) are shown to provide a direct determination of the cohesive energy. It generally appears that the 3d spin density is contracted relative to the free atom while the 3d charge density builds up at the Wigner–Seitz cell boundary relative to the free atom particularly near the bottom of the band. No theoretical calculation is available which evaluates charge, spin and momentum density as well as cohesive energy. In addition, a significant disparity between theory and experiment exists for the momentum and charge density anisotropies in the b.c.c. metals. Suggested areas for further work are given.
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  • 114
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 421-431 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The `microparacrystallite size' and `distortion parameter' of delignified ramie, hemp and jute have been determined – with the assumption that these materials are paracrystalline in nature – with the second and fourth central moments of X-ray diffraction line profiles. A new method of curvature correction has been developed. Background as well as non-additivity corrections have also been accounted for. Theories of determining the `microparacrystallite size' and the `distortion parameter' from single reflections independently from each of these two central moments have been developed, and described. Determination of these two parameters for several directions in the samples studied have been based on the above work. It has been shown that, in conformity with the recent findings of Hosemann & Balta Calleja [Ber. Bunsenges. Phys. Chem. (1980), 84, 91], the larger the paracrystalline distortion the smaller is the `microparacrystallite size'.
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  • 115
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 439-443 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Polar coordinates of a Kendrew model of α-chymotrypsin (α-CHT) have been measured with a surveyor's transit and a cathetometer to a high degree of accuracy and precision. Bond distances calculated independently for more than 200 independent amino-acid residues have standard deviations of 0.10 Å or less, the torsion angle ω has a standard error of 7°, and the τ angle is precise to 3°. The measured coordinates of about 1800 non-hydrogen atoms of one molecule of the α-CHT dimer fit a set of idealized polypeptide coordinates with a r.m.s. deviation of 0.17 Å, while the average deviation is 0.15 Å.
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  • 116
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 451-454 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A calculation method for the X-ray profiles from small, needle-like crystallites [Yücel, Rautureau, Tchoubar & Tchoubar (1980). J. Appl. Cryst. 13, 370–374] is applied to natural Eskisehir sepiolite mineral. By analysing the hk0 reflections, quantitative results are given on the average cross-sectional dimensions, their distribution, preferred directions of growth, lattice parameters, hydration state, and imperfections. Practical methods for the determination of the zeolitic water content and the importance of boundary effects are proposed.
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  • 117
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 464-464 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The powder data for anhydrous theophylline (1,3-dimethylxanthine), C7H8N4O2, are reported. It is orthorhombic, Pna21, with a = 24.628 (4), b = 3.833 (2), c = 8.501 (5) Å; U = 802.49 Å3; Z = 4; Dm = 1.478, Dc = 1.489 Mg m−3.
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  • 118
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 468-469 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The powder data for the title compounds are reported. They are monoclinic, Bb or B2/b, with, for 3C12H8N2.2H2SO4.2H2O, a = 20.87 (1), b = 14.581 (9), c = 11.458 (7) Å, γ = 108.32 (6)°, Z = 4, Dm = 1.58, Dc = 1.55 Mg m−3, and, for C12H8N2.2H2SO4, a = 17.39 (3), b = 15.38 (4), c = 6.85 (1) Å, γ = 124.9 (1)°, Z = 4.
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  • 119
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 191-202 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The present study presents the first small-angle neutron scattering experiment of lipid bilayers in excess water. The method of solvent contrast variation was applied. The variation of scattering intensity with the scattering angle could be analysed in terms of the Kratky–Porod model of scattering by quasi-two-dimensional systems. From this the bilayer thickness of unilamellar vesicles of dimyristoyllecithin was determined to be d = 41 ± 1 Å at 310 K. Several typical mixtures of different lecithins with varying chain lengths and of lecithin with phosphatidic acid were studied. By deuteration of one lipid component a very large contrast between segregated phases could be achieved. It was thus possible to distinguish clearly between homogeneous mixtures and mixtures which exhibit a heterogeneous lipid organization. In the latter case no intensity matching upon solvent contrast variation was possible. It is shown that phase boundaries may be determined very accurately by performing contrast variation experiments with at most two mixtures of different initial composition. The main advantage of the present method is that lateral phase separation may also be clearly studied in fluid states of the bilayer. From the average scattering-length densities one can determine the density of the lipid layers and thus the excess volumes of the mixtures. For lecithin mixtures positive excess volumes are observed.
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  • 120
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 214-215 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: An efficient computer-based procedure for randomly accessing reflection data is described.
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  • 121
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 217-217 
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  • 122
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    Applied crystallography online 14 (1981), S. 219-222 
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    Topics: Geosciences , Physics
    Notes: A method for the computation of the effect of rough sample surfaces on diffraction intensities is described. Though the model used for the calculation is a special simple one, it is exact. The method is illustrated by its application to a surface whose boundary is a saw-tooth. Possible generalizations of the character of the surface roughness effect and how it depends on the dimensions of the surface irregularities are inferred from the calculation.
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  • 123
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    Applied crystallography online 14 (1981), S. 223-225 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A method to determine the exact fiber identity periods (FIP) of polyamides from the X-ray meridional reflections has been found, which is essential especially for the γ forms of polyamides with large values of the FIP. The basic concept of this method is that the γ form has two kinds of reflections, the peak positions of which are shifted from the corresponding reciprocal-lattice points to the wide- and small-angle directions, so that the true FIP is between the maximum and minimum values calculated from the former and latter kinds of reflections, respectively. For an example, this method was applied to polylauryllactam (nylon 12) and a value of 31.92±0.02 Å was obtained as a more precise FIP.
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  • 124
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    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 14 (1981), S. 241-246 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Growth defects in a natural Brazilian single-crystal of beryl have been studied by X-ray topography, optical microscopy and electron microprobe. The distribution and configuration of channels and dislocations are both very different from those previously observed in other crystals and can be correlated with a `horseshoe' growth in a pegmatic medium. This was confirmed by the analysis of inclusions which allowed us to estimate the limits of temperature and pressure ranges in the genetic medium.
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  • 125
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    Applied crystallography online 14 (1981), S. 256-260 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A new X-ray film, produced by CEAVERKEN in Sweden, has recently become available. Some properties of this film have been compared to three other films commonly used in the recording of X-ray diffraction intensities (Agfa T4, Kodak No-screen, Ilford Industrial G). The linearity of CEA film has been found to be similar to that for Agfa and Ilford. The speed of the new film is about 10% lower than Agfa or Kodak, and the film factor was measured to be 2.9 for Cu Kα radiation. The background level is significantly lower than on the other three films investigated. This combination of properties makes CEA film suitable for routine collection of X-ray diffraction data.
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  • 126
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    Applied crystallography online 14 (1981), S. 270-273 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: It is shown that the principal topotaxial relationship between hematite α-Fe2O3 and magnetite Fe3O4 during cycles of reduction and oxidation can be considered as crystallographically reversible. The precision of the mutual orientation of the two lattices decreases as the number of cycles of reduction and oxidation increases and there is a correlation between crystallographic orientation and the rate of oxidation and of reduction.
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  • 127
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    Applied crystallography online 14 (1981), S. 280-280 
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  • 128
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    Applied crystallography online 14 (1981), S. 70-71 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
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    Notes: Orthorhombic unit-cell constants for SrRE2O4 (RE = Sm, Eu, Gd, Dy, Ho, Er, Tm, Yb, Lu, In and Y) have been determined by refinement of X-ray powder diffraction data. Unit-cell volumes are plotted against the cube of the trivalent rare-earth ionic radius.
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  • 129
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    Applied crystallography online 14 (1981), S. 76-76 
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  • 130
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    Applied crystallography online 14 (1981), S. 77-78 
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  • 131
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    Applied crystallography online 14 (1981), S. 94-100 
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    Notes: A brief description of the Molecular Modeling System-X graphics system hardware is followed by an explanation of the language which has been developed to realize an `electronic Richards box'. A variety of commands permits the construction and manipulation of a protein model within an electron density distribution. Usually about ten amino-acid residues can be displayed at any one time within a box of 20 grid points on an edge. The density is changed automatically as the viewer translates the model off the edge of the screen. He can then add, subtract or modify residues as appropriate.
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  • 132
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    Applied crystallography online 14 (1981), S. 109-116 
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    Notes: As the use of low-energy electron diffraction (LEED) for surface structural analysis has increased, the need for accurate values of scattering amplitudes and cross sections in the angle and energy range of interest to those doing LEED work has also increased. Presently available tables of atomic scattering factors, which could serve as a standard starting point for more sophisticated LEED calculations, are unfortunately limited in angle and energy and do not include a number of elements of interest to the surface-science community. In order to calculate these scattering amplitudes as well as total elastic cross sections for atomic scattering of low-energy electrons, the Dirac equation was solved numerically. Various analytic and numerical forms for the atomic potential, including relativistic, self-consistent Hartree–Fock–Slater scattering potentials were used. The exchange of the incoming electron with the atomic electrons was neglected because this effect is negligible for atomic scattering in the ranges where this work is applicable. Care is taken to demonstrate the validity of this work for LEED calculations and the limits of its application. The complete set of data for relativisitic partial-wave phase shifts is available for H, He, Li, C, N, O, Ne, Na, Si, S, Ar, K, Ca, Sc, Cr, Fe, Co, Ni, Zn, Ge, Se, Kr, Rb, Y, Mo, Rh, Cd, Sn, Te, Xe, Cs, La, W, Ir, Hg, Pb, Po and Rn. The data covers the energy range from 15 to 305 eV in 10 eV increments. To ensure convergence of the series when calculating the atomic scattering factors and subsequently the total elastic cross section, the actual calculations were performed with 50 to 80 partial waves depending on the energy of the incident electron. Owing to space limitations the phase shifts as well as the complex atomic scattering factors and elastic cross sections are not presented in the paper. They are available from the authors on request.
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    Applied crystallography online 14 (1981), S. 134-136 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Time-variable incident intensity from synchrotron radiation sources may cause scaling errors in crystallographic data collection using integrative techniques as in rotation methods. This problem is avoided with a new technique which has been developed for computer-controlled film data collection with an Arndt–Wonacott camera. Effects of intensity fluctuations are automatically compensated by hardware on the basis of incident-beam monitoring with a small ionization chamber placed between collimator and crystal.
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  • 134
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    Applied crystallography online 14 (1981), S. 143-144 
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    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
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    Notes: The chemical preparation of (NH4)2[RhCl5(H2O)] is described; lattice parameters and an indexed X-ray powder pattern are given. Diammonium aquapentachlororhodate is orthorhombic with a = 13.738 (1); b = 9.762 (1); c = 7.0419 (4) Å. The space group is Pnma.
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  • 135
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    Applied crystallography online 14 (1981), S. 155-155 
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  • 136
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    Applied crystallography online 14 (1981), S. 155-156 
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  • 137
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    Applied crystallography online 14 (1981), S. 169-177 
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    Notes: The crystal structure of Au–Cd (30–32%) alloys has been studied at atomic level with a 1 MV electron microscope. The experimental images can be fitted well with many-beam dynamical calculations for the long-period superstructure (LPS) designated as 7a0−2H type. The structures with incommensurate periods consist of a number of domains of the 7a0−2H structure separated by antiphase boundaries which are composed of orthorhombic cells. The result demonstrates the potentiality of high-voltage, high-resolution electron microscopy for direct determination of the atomic arrangements in modulated structures of alloys.
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    Applied crystallography online 14 (1981), S. 216-216 
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    Applied crystallography online 14 (1981), S. 217-218 
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    Applied crystallography online 14 (1981), S. 261-264 
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    Notes: Cation-excess spinels with the general formula Ni2(1 + x)2 +(Si4+, Ti4+)(1 − x)O4 (0.16 ≤ x ≤ 1) can be considered as defect NiO rocksalt structures in which two octahedral metal atoms are replaced by one tetrahedrally coordinated atom. Neutron time-of-flight powder data have been collected for two members of the solid-solution series with the ZING-P′ high-resolution diffractometer at Argonne National Laboratory. Least-squares refinement, using a modified Rietveld profile analysis, confirms that all Ti4+ in Ni2.62Ti0.69O4 [R(profile) = 3.27%; R(Rietveld) = 9.06%] and Ni2.42Ti0.74Si0.05O4 [R(profile) = 3.07%; R(Rietveld) = 8.54%] partially occupies the tetrahedral site 8(a) (Fd3m). Ni2+ totally occupies the octahedral position 16(d) and partially occupies position 16(c) which is vacant in stoichiometric spinels. The presence of small amounts of Si4+ ( ̃3 mol%) in the tetrahedral site 8(a) stabilizes the structure and results in a large decrease [0.0194 (1) Å] in the a cell parameter.
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    Applied crystallography online 14 (1981), S. 280-280 
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    Applied crystallography online 14 (1981), S. 297-299 
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    Notes: Polycrystalline samples of (KxTl1 − x)2Cd2(SO4)3 have been prepared with x = 0[0.125]1.0. The phase transition temperature, liquidus and solidus temperatures, lattice parameters and unit-cell volume at 298 K have been determined for each composition. The phase transition temperature varies linearly with x for 0.125 ≤ x ≤ 1.0, and the solidus curve varies linearly with x over the entire range. Mixed crystals are cubic at 298 K for x ≤ 0.645 and are orthorhombic at higher values of x. The cubic lattice parameter varies linearly with x for 0.125 ≤ x ≤ 0.645, the lengths of the orthorhombic a, b and c axes vary linearly with xfor 0.645≤x ≤ 1.0, and the unit-cell volume varies linearly with x for 0.125≤ x≤ 1.0.
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    Applied crystallography online 14 (1981), S. 309-314 
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    Notes: A model, belonging to the class of cell models previously introduced, is developed to calculate the small-angle X-ray scattering of random multiphase systems. This model, which is applied to supported metal catalysts, involves two cell sizes, one for the support and one for the metal. Interphase surface areas and the correlation function, related to the X-ray scattering intensity by a Fourier transform, are given in terms of these two parameters. By fitting the measured intensity I(h) to that predicted by the model, values for the metal and support surface areas are obtained.
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    Applied crystallography online 14 (1981), S. 326-328 
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    Notes: A single-stage closed-cycle helium cryorefrigerator has been installed on a conventional four-circle neutron diffractometer. The cold head together with a specially designed support and alignment unit are sufficiently compact to enable it to be mounted directly onto the φ rotation table within the χ circle in place of the normal goniometer head used for room-temperature experiments. The device has a temperature range of 50 to 300 K, is extremely simple to use, and has a low operation cost as no cryogenic liquids are consumed. There are additional restrictions on the diffractometer angles but, with care, it is possible to measure at least half the reciprocal sphere.
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    Applied crystallography online 14 (1981), S. 337-344 
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    Notes: An investigation of the M23C6 carbide (M = metal atom) precipitation induced by aging in AISI 304 stainless steel was performed with techniques of small-angle neutron scattering (SANS) and transmission electron microscopy (TEM). The samples were aged at 873 and 923 K for different times after a solution treatment at 1323 K. The coherent neutron scattering length density for each sample was calculated from the chemical composition. As the carbide composition is dependent on aging time exact chemical compositions for each sample were determined with X-ray fluorescence techniques. Coherent scattering cross-section curves were obtained for the different aged samples, from which the total surface and total volume of precipitates per unit volume of sample were determined as a function of aging time at both temperatures. Moreover, the size distribution function of M23C6 carbide was obtained for each aging time. In general, the results obtained, taking into account the difficulty of the problem, are in satisfactory agreement with the localized TEM observations.
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    Applied crystallography online 14 (1981), S. 351-352 
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    Notes: Crystal data are reported for cholesteryl cis-11-eicosenoate, C47H82O2, cis-13-docosenoate, C49H86O2, cis-15-tetracosenoate, C51H90O2, trans-9-octadecenoate, C45H78O2, trans-9-trans-12-octadecadienoate, C45H76O2, and cholestanyl octanoate, C35H62O2 dodecanoate, C39H70O2, and tetradecanoate, C41H74O2.
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    Applied crystallography online 14 (1981), S. 353-353 
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    Applied crystallography online 14 (1981), S. 354-355 
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    Applied crystallography online 14 (1981), S. 362-369 
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    Notes: At the University of Missouri Research Reactor, a γ-ray diffractometer has been constructed which uses 0.12 Å radiation produced from the decay of 153Sm. Use of this source rather than 198Au (λ = 0.03 Å), which is used at several instruments in Europe, has important advantages which are discussed. Details of the design necessary to work with 1000 Ci (37 TBq) sources at this wavelength are presented. In addition, the results of several experiments intended to test the capability of the instrument for measuring extinction-free structure factors at low angles and for measuring to high sin θ/λ ( ̃2 Å−1) are reported. These results show that it will be relatively straightforward to make absolute structure-factor determinations for light elements and to determine electron density distributions more accurately than has been done in the past with X-ray diffraction. Furthermore, determination of anharmonic thermal motion and form factors will be possible. Crystal perfection studies on small samples have also been performed and can be done routinely.
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    Applied crystallography online 14 (1981), S. 387-391 
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    Notes: The problem of assigning the phase to the first-order reflection in membrane diffraction is treated. Biological membrane assemblies with two membranes per unit cell and the special case of lipid bilayers are treated. Phase assignment is dependent on the origin value of the minus fluid or the minus lipid model and on the actual asymmetry of the membranes. The conditions for phase assignment are derived from a study of single- and three-strip electron density models.
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    Applied crystallography online 14 (1981), S. 417-420 
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    Notes: As a model for the internal structure of polymer crazes, a system of parallel cylinders with liquid-like order is proposed. X-ray diffraction curves were calculated for such a system with Monte Carlo data for the radial distribution function of the two-dimensional hard-disk fluid at different packing densities. A comparison is made between the present calculations and experimental results of crazed polycarbonate showing a very good agreement. A way of evaluating the average craze fibril diameter with the calculations is also discussed.
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    Applied crystallography online 14 (1981), S. 437-438 
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    Notes: Values of mean and anomalous absorption parameters in potassium feldspar, for operating diffraction vector g = 20{\bar 1} at an accelerating voltage of 100 kV, are reported. These values are ξg/ξ'0 = 0.35±0.05 and ξg/ξ'g = 0.27±0.07.
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    Applied crystallography online 14 (1981), S. 447-450 
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    Notes: The structure of high-pressure americium, phase III, which occurs at room temperature in the pressure range 10–15 GPa, has been determined. The material has a monoclinic lattice with a = 3.025±0.005, b = 11.887±0.019, c = 2.830±0.005 Å, and β = 106.11±0.14° at 12.5 GPa. The space group is P21/m with Z = 4. Intensity data were obtained from powder-pattern films taken at pressure with Mo Kα radiation, λ = 0.7107 Å. The structure, which can be described as a layer stacking intermediate between the lower-pressure f.c.c. and higher-pressure α-U structure types, was refined by least-squares calculations to R1 = 0.07 with 12 observed reflections. Am–Am distances of nearest neighbors range from 2.83 to 3.21 Å.
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    Applied crystallography online 14 (1981), S. 462-463 
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    Notes: Nd(MoO4) (ReO4) is monoclinic, space group P21/c; the cell dimensions are a = 6.169 (1), b = 9.822 (1), c = 13.139 (2) Å and β = 111.65 (1)°. The monoclinic compounds in the series Ln(MoO4) (ReO4), with Ln = Ce to Lu (Pm compound is not examined), are isotypic. Crystal parameters and powder diffraction data are given.
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    Applied crystallography online 14 (1981), S. 466-467 
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    Notes: X-ray and electron diffraction studies were made on the two phases of 11-aminoundecanoic acid, C11H21NO2. Phase I: dihydrate, monoclinic, C2/c, z = 8, a = 15.96±0.03, b = 4.71±0.01, c = 35.48±0.08 Å, β = 82.1±0.3°. Phase II: anhydrate, orthorhombic, P212121, z = 4, a = 7.526±0.003, b = 4.623±0.003, c = 32.42±0.01 Å.
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    Applied crystallography online 14 (1981), S. 471-472 
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    Notes: Tl2TlOH(SO4)2 is monoclinic, space group Cc or C2/c. The cell parameters are a = 7.758 (3), b = 17.587 (9), c = 7.356 (3) Å, β = 119.91 (3)°, Z = 4. Compounds in the series MI2MIIIOH(X O4)2 (with MI= K, Rb, Tl, NH4; MIII = Tl, In; X = S, Se) are isotypic. Crystal parameters and powder diffraction data are given.
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    Acta crystallographica 37 (1981), S. 584-593 
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    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: A number of theories are examined for their predictions of extinction coefficients at large values of extinction, especially as applied to polarization ratios. Although several theories give the behavior expected on the basis of physical reasoning (a polarization ratio approaching unity), the popular theories of Zachariasen [Acta Cryst. (1967), 23, 558-564] and Becker & Coppens [Acta Cryst. (1964), A30, 129-147, 148-153] do not show the correct asymptotic behavior. Although this shortcoming may be of no consequence in ordinary crystallographic applications, it is misleading in predicting the correct polarization factor to be used in connection with a crystal-monochromated apparatus, where the monochromator is usually adjusted to maximize its extinction. The importance of measuring, rather than estimating, the polarization ratio of a crystal monochromator is therefore reemphasized.
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    Acta crystallographica 37 (1981), S. 605-605 
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    Acta crystallographica 37 (1981), S. 605-605 
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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. 443-444 
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    Acta crystallographica 37 (1981), S. 441-442 
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    Notes: A Fourier representation of the distribution of the halogen atoms along c of Cd analogues of apatite should show a reduction in ripples, paid for by poorer resolution in the Rayleigh sense, if the reflexions within a cube having its triad axis along c are used, rather than all those within the observable sphere in reciprocal space [Wilson (1979). Acta Cryst. A35, 122-130, §2.7.2]. Syntheses with the data of Wilson, Sudarsanan & Young [Acta Cryst. (1977), B33, 3142-3154] show the predicted effect. The variance of such distributions is discussed.
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    Acta crystallographica 37 (1981), S. 442-443 
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    Notes: Cadmium sulphide thin films have been found to exhibit the occurrence of polytypism. The polytypes are formed when amorphous cadmium sulphide thin films undergo an amorphous to crystalline transformation. The single-crystal regions correspond to different polytypes. Two types of polytypic modifications were found to occur most frequently. One of these, the low-temperature modification, had a = 4.15 and c = 6.72 Å and corresponded to the known crystallographic variant 2H. The observed polytypes based on this phase were 4H (a = 4.15; c = 13.44 Å) and 6H (a = 4.15; c = 20.16 Å). In addition, a disordered long-period polytype has also been observed. The other common type found was a high-temperature modification with a = 5.12 and c = 8.62 Å. This new type has been designated as 2H1. The observed polytype based on this modification corresponded to 5H1 (a = 5.12; c = 21.50 Å).
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    Acta crystallographica 37 (1981), S. 445-446 
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    Acta crystallographica 37 (1981), S. 446-446 
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    Acta crystallographica 37 (1981), S. 446-447 
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    Acta crystallographica 37 (1981), S. 447-448 
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    Acta crystallographica 37 (1981), S. 943-943 
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    Acta crystallographica 37 (1981), S. 944-944 
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    Acta crystallographica 37 (1981), S. 238-241 
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    Notes: Structurally forbidden Bragg maxima in the X-ray diffraction pattern of V3Si have been observed. These reflections are excited by nonspherical electron distributions and anharmonic and anisotropic thermal motion. The forbidden reflections which are accessible to such excitation are correctly predicted by theory. Further studies of such maxima both with neutrons and X-rays should provide insights into the electronic and thermal behaviour of A15 compounds.
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    Acta crystallographica 37 (1981), S. 266-266 
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    Notes: Fig. 1 of Bevan, Greis & Strähle [Acta Cryst. (1980). A36, 889-890] has been printed upside-down. The legend is correct.
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    Acta crystallographica 37 (1981), S. 267-268 
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    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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    Acta crystallographica 37 (1981), S. 269-269 
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    Acta crystallographica 37 (1981), S. 269-269 
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  • 177
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    Acta crystallographica 37 (1981), S. 270-270 
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    Acta crystallographica 37 (1981), S. 271-271 
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    Acta crystallographica 37 (1981), S. 270-271 
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    Acta crystallographica 37 (1981), S. 272-272 
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  • 181
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    Acta crystallographica 37 (1981), S. 273-280 
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    Notes: The feasibility of direct structure imaging of pyroxenoid chain silicates by high-resolution electron microscopy at 500 kV is demonstrated both experimentally and theoretically for the minerals wollastonite, CaSiO3, and rhodonite, MnSiO3. Image simulations with a simplified multi-slice approach indicated that the crystal projection most suitable for direct observation of the tetrahedral chain arrangement corresponded to the overlap of the metal cations with the tetrahedral sites, a situation which occurs in all pyroxenoids. Electron micrographs were also obtained, with bright- field axial illumination at 500 kV, which could be closely matched with the simulated images, at least for very thin crystal regions. The implications of these results, in particular for studies at the atomic level of solid-state transformations involving the pyroxenoids, are briefly discussed.
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  • 182
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    Acta crystallographica 37 (1981), S. 281-286 
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    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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  • 183
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    Acta crystallographica 37 (1981), S. 286-292 
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    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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  • 184
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    Acta crystallographica 37 (1981), S. 293-301 
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    Notes: Nonbonded O...O potential parameters of the (exp - 6) type were derived from five selected oxohydrocarbon crystal structures, which do not have hydrogen bonds: β-oxygen, carbon dioxide (CO2), trioxane (C3H6O3), tetroxocane (C4H8O4) and succinic anhydride (C4H4O3). Previously established hydrocarbon H and C nonbonded parameters were transferred. Net atomic charges were calculated separately by obtaining a least-squares fit to the molecular electric field calculated by the ab initio self-consistent-field molecular-orbital method. The resulting O...O nonbonded potential was found to transfer well to the structures of pentoxecane (C5H10O5), 1,4- cyclohexanedione (C6H8O2) and diglycolic anhydride (C4H4O4). The potential did not transfer well to the structures of p-benzoquinone (C6H4O2) and furan (C4H4O). The addition of an approximate weak hydrogen-bonding potential for a C-H... O hydrogen bond improved the fit to the latter two structures.
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  • 185
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    Acta crystallographica 37 (1981), S. 51-61 
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    Notes: The defect blocks formed in β''-alumina by electron irradiation are examined by 1 MV high-resolution electron microscopy. In order to explain the fact that two distinctly different types of defect images appear even in a single 1 MV micrograph, a new structural model is constructed in place of the two models so far reported. In the model proposed, two spinel-like blocks on either side of the eliminated conduction plane are directly combined by the vectors including x, y components to form cubic close packing of oxygen layers in the resultant defect blocks. The arrangements of cations in the defect block are slightly different from those expected from the spinel structure.
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  • 186
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    Acta crystallographica 37 (1981), S. 61-65 
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    Notes: As an extension of Table 7.1.5B of International Tables for X-ray Crystallography [(1967), Vol. II. Birmingham: Kynoch Press], the possible stacking variants up to ten layers are arranged according to the percentage of hexagonal stacking. A method is given which allows one to calculate the number of possible stacking variants for any number of layers.
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  • 187
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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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  • 188
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    Acta crystallographica 37 (1981), S. 324-331 
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    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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  • 189
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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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  • 190
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    Acta crystallographica 37 (1981), S. 335-342 
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    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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  • 191
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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. 342-353 
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    Notes: Probability functions, moments and cumulative distributions of the normalized intensity z = |E|2, depending on the space-group symmetry of the crystal and its chemical composition, have been investigated. The probability functions were reduced to a simple, unified representation, by reconsidering some mathematical properties of the corresponding asymptotic expansions. A subsequent unified derivation of the first four even moments of |E|, in terms of symmetry and composition, leads to (i) simple and readily computable expressions for (|E|4), (|E|6) and (|E|8) and (ii) a significant simplification of the expansion coefficients which appear in the above asymptotic expansions. The convergence of these expansions is discussed and illustrated by a numerical example. It is shown that the Edgeworth arrangement of these asymptotic expansions is superior to the frequently given Gram-Charlier one. The dependence of the fourth moment of |E| on atomic heterogeneity and the generalized cumulative distribution functions N(|E|) are illustrated for all the symmorphic space groups. The results of this study are directly applicable to practical intensity statistics for structures containing all the atoms in general positions.
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    Acta crystallographica 37 (1981), S. 361-364 
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    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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  • 194
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    Acta crystallographica 37 (1981), S. 374-377 
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    Notes: Self force constants φijαβ \Bigl \matrix { l l \cr \kappa \kappa} \Bigr, that are needed in lattice dynamical calculations making use of external-mode formalism, are obtained. There is a need to include quadratic components in angular displacements (of clusters) while computing atomic displacements. In particular, the rotation-rotation self force constant φrrαβ \Bigl \matrix { l l \cr \kappa \kappa} \Bigr derives an extra term because of the quadratic terms. Implications of this term in lattice dynamical calculations are discussed.
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    Acta crystallographica 37 (1981), S. 369-373 
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    Notes: The mathematical model described in part I [Urbanowicz (1981). Acta Cryst. A37, 364-368] has been verified by measurements performed on the Bond diffractometer constructed in the author's institute. A computer program has been written allowing the synthesis of the diffraction profile h(ω) for an arbitrary original function f(ω), distribution of tube-focus emissivity is(x), collimator length L2, and for given widths d1, d2 of collimator slits. The calculations have been performed to estimate systematic errors related to the collimation conditions, caused by insufficient accuracy (shift Δs) of the collimator setting in relation to the focus centre and asymmetry function φ of the distribution of tube-focus emissivity. A simplified formula is given for fast estimation of the errors caused by overlapping of the Kα1-Kα2 doublet and by the Lp factor.
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    Acta crystallographica 37 (1981), S. 378-382 
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    Notes: A general procedure for the calculation of radii of gyration and scattering intensities of hollow triaxial bodies is proposed. By this method, equations for the radii of gyration and the scattering intensities of hollow bodies, i.e. isosceles triangular, rectangular and regular polygonal prisms, elliptic cylinder and ellipsoid, are obtained. Existing models are expressed as the limited case of present results. The scattering curves of regular polygonal prisms of more than six sides are practically the same as that of a column. The curves have a tendency to become less undulant according to the decrease in isotropy of the body shape and the size of the hollow.
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  • 197
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    Acta crystallographica 37 (1981), S. 645-649 
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    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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    Acta crystallographica 37 (1981), S. 684-689 
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    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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    Acta crystallographica 37 (1981), S. 692-697 
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    Notes: The structure of a vacuum-deposited polycrystalline film of zinc phthalocyanine, C32H16N8Zn, has been investigated by high-resolution electron microscopy. With the aid of a minimum-dose system, the molecular arrangements in crystals were observed and the existence of at least three polymorphs were confirmed in the film.
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    Acta crystallographica 37 (1981), S. 139-140 
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