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X-ray crystallographic studies of highly purified Ti2O3 show abrupt changes in the lattice parameters with temperature in the range 390–470°K. The distension of the unit cell in this temperature range is readily correlated with corresponding changes in resistivity.
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An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
Electronic absorption spectroscopy and fluorescence spectroscopy have been used to investigate the interaction of the fullerenes C60 and C70 with diethylaniline, and with aromatic solvents such as benzene. C60 interacts weakly with aromatic amines in the ground state while C70 does not interact at all. Steady state fluorescence emission and lifetime measurements show that both C60 and C70 form excited state complexes (exciplexes) with the amines in non-aromatic solvents such as methylcyclohexane, but not in benzene. In benzene, only fluorescence quenching is observed due to the interaction between the π systems of the aromatic solvent and the fullerene in the ground state. This is also borne out by the systematic study of solvent effects on the absorption and emission spectra of the fullerenes.
Graphene is a fascinating new nanocarbon possessing, single-, bi- or few- (≤ ten) layers of carbon atoms forming six-membered rings. Different types of graphene have been investigated by X-ray diffraction, atomic force microscopy, transmission electron microscopy, scanning tunneling microscopy and Raman spectroscopy. The extraordinary electronic properties of single-and bi-layer graphenes are indeed most unique and unexpected. Other properties of graphene such as gas adsorption characteristics, magnetic and electrochemical properties and the effects of doping by electrons and holes are equally noteworthy. Interestingly, molecular charge-transfer also markedly affects the electronic structure and properties of graphene. Many aspects of graphene are yet to be explored, including synthetic strategies which can yield sufficient quantities of graphene with the desired number of layers.
Giant magnetoresistance (GMR) and related properties of manganate perovskites of the general formula Lnl − xAxMnO3 (Ln = rare earth; A = divalent ion) are discussed in detail. There is a fine interplay of magnetic exchange, structural properties and electronic transport in these materials which gives rise to several novel properties. The manganates are ferromagnetic at or above a certain value of x (or Mn4+ content) and become metallic at temperatures below the curie temperature, T c . This behavior is attributed to double-exchange. GMR is generally a maximum close to T c or the insulator-metal (I-M) transition temperature, T im . The T c and %MR are markedly affected by the size of the A site cation, 〈 r A 〉, thereby affording a useful electronic phase diagram when T c or T im is plotted against 〈 r A 〉 or pressure. The commonalities and correlations found in the properties of manganates are examined along with certain unusual features in the electron-transport properties of these materials. Some of the Ln1 − xAxMnO3 compositions exhibit charge-ordering and related effects. Charge ordering is crucially dependent on 〈 r A 〉 or the eg band width and the charge-ordered insulating state transforms to a metallic ferromagnetic state on the application of a magnetic field, charge-ordering and double-exchange being competing interactions.
Bi5Ti3FeO15 and Bi7Ti3Fe3O21 which are n=4 and n=6 members of the family of oxides of the general formula (Bi2O2)2+(An−1BnO3n+1)2− show unusual superstructures, possibly due to cation ordering.
Deintercalation of amines from the layered amine adducts of WO 3 , MoO 3 and W 1‐ x Mo x O 3 has been employed as a soft chemical route to produce unusual metastable structures of the oxides. After the adducts of WO 3 , MoO 3 and W 1– x Mo x O 3 ( x = 0.25, 0.5, 0.75) with amines such as triethylamine (TEA), pyridine, n ‐butylamine and n ‐octylamine had been characterized, deintercalation was carried out thermally as well as by acid leaching. Thermal deintercalation yielded novel metastable structures of WO 3 and MoO 3 that were significantly different from the stable forms, which contain distorted metal‐oxygen octahedra. Thus, ReO 3 ‐type cubic WO 3 was obtained by the thermal deintercalation of WO 3 · 0.5 TEA. Acid leaching of the amines gave metastable phases of WO 3 , MoO 3 and W 1‐ x Mo x O 3 , which were different from those obtained thermally. All the metastable phases transformed to the corresponding stable forms at higher temperatures.
Pyrolysis of organometallic precursors such as metallocenes and iron pentacarbonyl as well as of their mixtures with hydrocarbons such as acetylene or benzene has been carried out under a variety of conditions to synthesize nanotubes. While the use of benzene as a hydrocarbon source generally yields multi-walled nanotubes, it has been possible to obtain single-walled nanotubes (∼1 nm diameter) by pyrolyzing a metallocene or a mixture of metallocenes along with acetylene under a high flow rate of Ar. These experiments show that the organometallic precursor produces small nanoparticles of ∼1 nm diameter which then catalyze the formation of the single-walled nanotubes. Copious quantities of aligned-nanotube bundles have been obtained by the pyrolysis of acetylene in the presence of high concentrations of ferrocene. Nanorods have been produced by the pyrolysis of ferrocene under vacuum. Single walled nanotubes can be filled or decorated by metals.
No abstract is provided for this article.
No abstract is provided for this article.