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26 citations found for Ma, Q

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Crystals of the title compound, 2C26H18N4O2·C7H8, were obtained from the reaction of 8-hydroxy­quinoline with 1,2-phenyl­enediamine in methanol and recrystallized from toluene. The compound contains three essentially planar ring systems: the benzimidazole ring (r.m.s. deviation = 0.039 Å) and two 8-hydroxy­quinoline rings (r.m.s. deviations of 0.0056 Å in both rings). The benzimidazole ring and one 8-hydroxy­quinoline ring are almost co-planar, forming a dihdral angle of 3.1 (2)°. The other 8-hydroxy­quinoline ring is almost perpendicular to the benzimidazole plane with a dihedral angle of 86.2 (2)°. Intra­molecular O—H...N contacts are present. The crystal structure is stabilized by inter­molecular O—H...N inter­actions. The complete toluene molecule is generated by crystallographic inversion symmetry; therefore its methyl group is disordered over two sites of equal occupancy.

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SAD phasing based primarily on sulfur anomalous scattering measured in-house led to easily interpretable maps for five standard test proteins.

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Acta Cryst. (2002). A58, c83
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Siderophore-interacting proteins (SIPs) can reduce ferric iron to ferrous iron and cause iron to be released from the ferric siderophore complex. The SIP from Vibrio anguillarum 775 has been expressed, purified and crystallized. The crystal diffracted to 1.113 Å resolution, which is the highest resolution so far observed for a member of the SIP family.

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In the title hydrated mol­ecular salt, 2C3H7N6+·HPO42−·3H2O, three of the O atoms of the hydrogen phosphate anion are disordered over two positions, with relative occupancies of 0.763 (1) and 0.237 (1). In the crystal, the components are linked by N—H...N, N—H...O and O—H...O hydrogen bonds

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An approach to fast fitting of crystal electric field parameters to any experimental data is presented. This approach is implemented in a lightweight Python-based program, CrysFieldExplorer.

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In the title compound, C8H9N2+·NO3, inter­molecular N—H...O hydrogen bonds join the mol­ecules into a chain extending along the b axis.

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The crystal structure of β-luffin at 2.0 Å resolution has been solved by the molecular-replacement method using polyalanyl trichosanthin as the search model.

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Acta Cryst. (2014). A70, C859
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In light of advances in detector technology, we revisit wide angle x-ray scattering techniques and their application to amorphous thin films that are of technological importance. For thin film materials the asymmetrical reflection geometry is employed to avoid the substrate signals. Incident x-ray angles are typically set close to the critical angles. There are various complications related to this geometry, in particular, raw scattering patterns being distorted. In addition, because these materials are typically weak scatterers due to disorder, increased data collection efficiency is always desired. Here, we report our activities using a 4-element vortex Si-drift detector for wide angle x-ray scattering experiments and present some experimental data collected on amorphous transparent conducting oxides.

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Crystals of the title compound, C10H8N2O2, were obtained from a condensation reaction of hydrazine hydrate with furfural. In the crystal structure, the mol­ecule is centrosymmetric and almost planar and the furan rings are parallel by symmetry.

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In the title compound, [Co(C6H5N4)3], the CoIII atom adopts a distorted octa­hedral CoN6 coordination geometry, arising from three N,N′-bidentate deprotonated 2,2′-biimidazole ligands. The dihedral angles between the five-membered rings of the ligands are 4.1 (2), 9.4 (2) and 10.5 (2)°. In the crystal, mol­ecules are linked by N—H...N hydrogen bonds, generating a layered network lying in (11\overline{1}).

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In the title compound, [Mn(C13H9N2O)2(CH3OH)2]Cl, the MnIII atom (site symmetry \overline{1}) is coordinated by two N,O-bidentate 2-(1H-benzimidazol-2-yl)phenolate ligands and two methanol mol­ecules, to generate a distorted trans-MnN2O4 octa­hedral geometry for the metal ion. The dihedral angle between the aromatic ring systems in the ligand is 16.0 (3)°. In the crystal structure, the complex cations and chloride anions are linked by O—H...Cl and N—H...Cl hydrogen bonds. The chloride ion lies on a crystallographic twofold axis.

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This work describes an experimental method in tackling the self-absorption effect encountered in fluorescence X-ray absorption spectroscopy and its application to surface and subsurface.

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In the title salt, [Cu(NCS)(C6H6N4)2]Cl, the CuII atom adopts a five-coordinated square-pyramidal geometry consisting of an N atom from a thio­cyanate anion and four N atoms from two chealting biimidazole ligands. The thio­cyanate ligand occupies the axial position and is, like the CuII centre, located on a mirror plane. The cation and anion are linked into a linear chain by N—H...S and N—H...Cl hydrogen bonds.

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Crystals of luffaculin, a ribosome-inactivating protein from sponge gourd seeds, have been obtained. The crystals belong to space group C2 and diffract to 2.0 Å resolution.

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The mol­ecular and crystal structure of the title triazole derivative is reported. In the crystal, mol­ecules are linked by weak C—H...O and C—H...F hydrogen bonds, forming a three-dimensional supra­molecular structure.

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In the title complex, [Zn2(C10H7NO6)2(C5H5N)2]n, the repeat unit is a centrosymmetic tetra-carboxyl­ato-O,O'-bridged dimer in which each ZnII atom is five-coordinated by four O atoms from different dianionic 4,6-dimethyl-5-nitro­iso­phthalate ligands [Zn—O = 2.0283 (18)–2.0540 (19) Å] and one N atom from a pyridine mol­ecule [Zn—N = 2.030 (2) Å] in the axial site of a slightly distorted square-pyramidal coordination sphere. The Zn...Zn separation is 2.9750 (6) Å. The complex dimers are extended into a two-dimensional polymeric structure parallel to (100) through bridges provided by the second carboxyl­ate group of the ligand.

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The structures of the PDI-related protein Wind and three mutants show the same mode of dimerization and only subtle differences in the putative Pipe-binding region, although two of the mutants completely abrogate Pipe transport.

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