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141.
Using oyster shell, single-crystalline Na2Ti6O13 and Na2W4O13 one-dimensional nanostructures (ODNS) were simply synthesized from granular TiO2 and WO3 particles by thermal heating at 700 °C. The oyster shell was used as a source of both sodium and carbon dioxide, which have an effect on unidirectional growth of single-crystalline Na2Ti6O13 and Na2W4O13 from TiO2 and WO3. The growth of sodium metal oxide ODNS from metal oxide particles was reproduced by replacing oyster shell with chemical reagents (NaCl, CaCO3) or gas (CO2), allowing identification of the main factors for the growth of ODNS. The characteristics of biological material (i.e., oyster shell) lend certain advantages in the fabrication of sodium metal oxide ODNS: (a) low processing temperature with high yield; (b) an eco-friendly method; and (c) no requirement of additional processes such as separation or washing. This work suggests a new approach for using biological material for the crystal growth of nanostructured materials.  相似文献   
142.
Hexa-alkylphosphorus triamides and trifluoromethyl bromide react to give trifluoromethyltris(dialkylamino)phosphonium bromides which were used for the trifluoromethylation of benzaldehyde and copper(I) iodide in the presence of fluoride anions with different counterions; tris(diethylamino)difluorophosphorane proved to be a masked fluoride anion donor. The structures of [CF3P(NMe2)3]+Br and [CF3P(NEt2)3]+Br have been determined by single-crystal X-ray investigations and shown to exhibit a distorted tetrahedral bond configuration with a rather long (F3)C---P bond of 1.866(9) or 1.896(6) Å, respectively.  相似文献   
143.
We performed the single-crystal X-ray diffraction study of a perovskite-type gold mixed-valence compound, Cs2AuIAuIIICl6, under high pressures up to 18 GPa by using a diamond-anvil-cell with helium gas as an ideal hydrostatic pressure-transmitting medium. The lattice parameters and the variable atomic positional parameters were obtained with reasonable accuracy at various pressures. A structural phase transition at ca. 12.5 GPa from I4/mmm to Pm3m was found. The lattice parameters a0 and c0, denoted in the tetragonal cell setting, result in the relationship 21/2a0=c0, and the superstructure reflections h k l (l is odd), caused by the shift of the Cl ions from the midpoint of the Au ions, disappeared at pressures above the phase transition. Both elongated [AuIIICl6] and compressed [AuICl6] octahedra in the low-pressure phase smoothly approach regular octahedra with increasing pressure. Above the structural phase transition at 12.5 GPa, all the [AuCl6] octahedra are crystallographically equivalent, which shows that the tetragonal-to-cubic phase transition accompanies the valence transition from the AuI/AuIII mixed-valence state to the AuII single-valence state.  相似文献   
144.
The crystal structure of Ca(IO3)2·6H2O (Fdd2, Z = 8, a = 1485.9(1) pm, b = 2301.8(2) pm, and c = 639.44(5) pm, RW = 4.7%) has been refined by single-crystal neutron diffraction studies on the basis of 1150 reflections using the Becker and Coppens formalism for refinement of the extinction parameters. The X-ray structure reported in the literature has been confirmed and the positions of the six crystallographically different hydrogen atoms have been established for the first time. The HO distances of the hydrogen bonds formed are 167.8, 177.8, 180.2, 191.8, 194.8, and 198.0 pm, which correspond to the six uncoupled OD stretching modes (2307, 2378, 2409, 2488, 2516, and 2526 cm−1, 90 K) in the infrared and Raman spectra of isotopically dilute samples. For assignment of the observed bands to the hydrogen positions of the structure we performed single-crystal Raman studies on partially deuterated samples, as proposed in 1984. The limits of this procedure and those of other methods for assigning water bands and the relationship of the strengths of the hydrogen bonds with spectroscopic and structural data, including bond valences and I---OH bond angles, are discussed.  相似文献   
145.
A new mixed metal oxalate Cd3In2(C2O4)6·9H2O, with an open-framework structure, has been prepared from a precipitation method at room temperature. Its crystal structure has been solved from single-crystal diffraction data. The compound crystallizes with space group P6422 and the cell parameters are a=8.566(5)Å, c=37.811(5) Å, V=2403(2) Å3, and Z=3 (R1=0.036). The three-dimensional structure is built from three types of MO8 (M=Cd, In) polyhedra, i.e., triangular dodecahedra, bicapped trigonal prisms and an undefined distorted eight-fold cadmium polyhedron. Relationships with the structures of the related cadmium zirconium oxalates are discussed. The structure overview suggests the possibility to conceive new oxalate-based materials with open-framework structures. The thermal behavior of the new compound is described in details from temperature-dependent X-ray powder diffraction and thermogravimetry measurements. The dehydration process of the precursor is reversible in its stability temperature range. The final product consists of a mixture of nanocrystalline CdIn2O4 and the simple oxides.  相似文献   
146.
The reaction of the hypho-[6,7-C2B6H13] anion (1) with nickelocene and an excess of ‘proton sponge’ (1,8-bis-(dimethylamino-naphthalene)) in boiling acetonitrile leads to the formation of a pair of isomeric trimetallic nickel-boron clusters, [6,7,8-(CpNi)3-1-CB5H6] (2) and [6,7,8-(CpNi)3-2-CB5H6] (3), in a combined yield of 55%. Isomer (2) had been previously prepared from nido-2-CB5H9 but in much lower yield. Isomer (3) is without precedent and has been characterized using multi-nuclear NMR spectroscopy and mass spectrometry. Isomer (3) undergoes conversion to (2) via heating in boiling toluene. In addition to this isomeric pair, an interesting nido dimetallacarborane of constitution [6,6′-(CpNi)2-7,7′-C2B6H8] (4) has been isolated from the same reaction in 5% yield and characterized by single-crystal X-ray diffraction analysis.  相似文献   
147.
The high-temperature polymorphs of two photocatalytic materials, BiNbO4 and BiTaO4 were synthesized by the ceramic method. The crystal structures of these materials were determined by single-crystal X-ray diffraction. BiNbO4 and BiTaO4 crystallize into the triclinic system P1¯ (No. 2), with a=5.5376(4) Å, b=7.6184(3) Å, c=7.9324(36) Å, α=102.565(3)°, β=90.143(2)°, γ=92.788 (4)°, V=326.21 (5) Å3, Z=4 and a=5.931 (1) Å, b=7.672 (2) Å, c=7.786 (2) Å, α=102.94 (3)°, β=90.04 (3)° γ=93.53 (3)°, V=344.59 (1) Å3 and Z=4, respectively. The structures along the c-axis, consist of layers of [Bi2O2] units separated by puckered sheets of (Nb/Ta)O6 octahedra. Photocatalytic studies on the degradation of dyes indicate selectivity of BiNbO4 towards aromatics containing quinonic and azo functional groups.  相似文献   
148.
Single crystals of new quaternary compounds Sr8Cu3In4N5 and Sr0.53Ba0.47CuN were prepared, respectively, from a Sr–Cu–In–Na melt under 7 MPa of N2 and from a Sr–Ba–Cu–In–Na melt under 0.5 MPa of N2 by slow cooling from 1023 to 823 K. The crystal structures were determined by single-crystal X-ray diffraction. Sr8Cu3In4N5 has an orthorhombic structure (space group, Immm, Z=2, a=3.8161(5) Å, b=12.437(2) Å, c=18.902(2) Å), and is isostructural with Ba8Cu3In4N5. It contains nitridocuprates of isolated units 0[CuN2] and one-dimensional linear chains 1[CuN2/2] and one-dimensional indium clusters 1[In2In2/2]. Sr0.53Ba0.47CuN crystallizes in an orthorhombic cell, space group Pbcm, Z=4, a=5.4763(7) Å, b=9.2274(12) Å, c=9.0772(12) Å. The structure contains infinite zig-zag chains 1[CuN2/2] which kink at every second nitrogen atom.  相似文献   
149.
150.
The atomic structure of ( La 1 - y Pr y ) 0.7 Ca 0.3 MnO 3 compound with 0.5≤ y ≤1 has been systematically studied by neutron powder diffraction in the temperature range from 15 to 293 K. For composition with y = 0.75, the structural analysis was performed on two samples, one containing the natural mixture of oxygen isotopes and the other one 75% enriched by 18 O. The room temperature structural characteristics of the series, including cell volume, average Mn-O bond distance, and average Mn-O-Mn bond angle, are the linear functions of the < r A >. Temperature dependencies of these parameters are quite smooth, except for the point T = T FM , where a jump like changes occur. The isotope enriched samples have been found identical in crystal and magnetic structure down to the temperature of transition of the sample with 16 O into the metallic ferromagnetic phase. It confirms that different transport and magnetic properties of the samples with 16 O and 18 O at low temperature are driven by the different oxygen atoms dynamics solely. Temperature dependencies of the CO and AFM diffraction peak intensities and of the peak widths for compositions close to the metal-insulator boundary ( y ≈ 0.75) indicate the macroscopically phase separated AFM-dielectric + FM-metallic state below T FM . Received 28 April 2000  相似文献   
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