issue contents

Journal logoSTRUCTURAL SCIENCE
CRYSTAL ENGINEERING
MATERIALS
ISSN: 2052-5206

December 2003 issue

Highlighted illustration

Cover illustration: Orange polytypically disordered crystals of HgI2 are built from layers of corner-linked Hg4I10 supertetrahedra. The stacking disorder has been quantitatively analyzed with a Markov chain model. Two probabilities describing next-nearest-layer interactions were adjusted to observed diffuse intensity profiles extracted from image-plate detector data. Results show nearly equal volumes of the two maximum degree of order structures, with an average domain thickness of about 5 layers or 30 Å [Hostettler, Birkedal & Schwarzenbach (2002), Acta Cryst. B58, 903-913].

research papers


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An accurate charge-density analysis of the title compound is presented and compared with the procrystal topological properties.

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Rietveld refinements of the high-pressure polymorphs of GeO2 synthesized in the laboratory have been performed. The structure refinements confirm that the high-pressure phases have the α-PbO2- and pyrite-type (modified-fluorite-type) structures.

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GdS_{2-x} forms a 144-fold superstructure that is shown to result from an ordering of vacancies in the layers of S atoms. Charge balance is maintained by the presence of both S_2^{2-} dimers and S^{2-} ions in these layers.

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The incommensurately (3 + 1)-dimensional modulated structure of δ1-CoZn7.8 was solved and refined from single-crystal X-ray diffraction data. The linking of double icosahedra along the b axis is considered to be both a consequence of geometric demands and the cause of the incommensurate modulation.

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The alkali-metal clinopyroxene compound NaTiSi2O6 (sodium titanium silicate) shows a crystallographic phase transition at 197 K. The structure of the low-temperature phase was determined and the temperature-induced structural changes were investigated in detail by X-ray diffraction experiments on a single crystal between 100 and 298 K.

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The low-temperature structure of V6O13 has been re-investigated using single-crystal X-ray diffraction. The transition temperature and heat of transition have been determined using differential scanning calorimetry.

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The ab initio determinations of the crystal structures of three alkali-metal salts A[B(C2O4)2] (A = K, Na, Li) from conventional powder diffraction data are reported.

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A recently developed method for fitting a Monte Carlo computer-simulation model to observed single-crystal diffuse X-ray scattering has been used to study diffuse scattering in 4,4′-dimethoxybenzil, C16H14O4. The analysis has shown that the most prominent features of the diffraction patterns, diffuse steaks that occur normal to the {\rm [1 0 }\overline {\rm 1}] direction, are due to longitudinal displacement correlations along chains of molecules extending in this direction.

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Static disorder in the crystal structure of E-1,2-bis(3-methoxy-2-thienyl)ethene is described and attributed to a high-energy conformer of the compound.

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The structural changes in a crystal of 9-methylanthracene during the [4 + 4] photodimerization were monitored step-by-step by means of X-ray structure analysis. The results were compared with data for the [2 + 2] photodimerization.

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The protonation site and hydrogen bonding in an anhydrous and in a hydrated crystalline form of doxazosin mesylate, a commonly used antihypertensive medication, have been determined as a result of crystal structure solution from synchrotron X-ray powder diffraction data.

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The 1:2 adduct of benzene-1,2,4,5-tetracarboxylic acid and 4,4'-bipyridyl has been studied by single-crystal neutron diffraction at 20, 200 and 296 K. The structure contains two short N⋯O hydrogen bonds; the H atom in the shortest is observed to migrate across the hydrogen bond between 20 and 296 K.

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A new CBED (convergent-beam electron diffraction) method is proposed for the identification of the chirality of enantiomorphic crystals, in which asymmetry in the intensities of the reflections of Bijvoet pairs in an experimental symmetrical zone-axis CBED pattern is compared with that of a computer-simulated CBED pattern. With the present method, a single CBED pattern is sufficient and chiral identification can be made for all the possible enantiomorphic crystals that are allowed to exist in crystallography.

addenda and errata


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