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Temperature-dependent Raman spectra of TbMnO(3) from 5 to 300 K in the spectral range of 200-1525 cm(-1) show five first-order Raman allowed modes and two high frequency modes. The intensity ratio of the high frequency Raman band to the corresponding first-order Raman mode is nearly constant and high (∼0.6) at all temperatures, suggesting an orbiton-phonon mixed nature of the high frequency mode. One of the first-order phonon modes shows anomalous softening below T(N) (∼46 K), suggesting a strong spin-phonon coupling.
No abstract is provided for this article.
No abstract is provided for this article.
Band structure calculations have indicated that in the double-Tl–O-layer cuprates, the bottom of the Tl(6s) band lies significantly below the Fermi level, while in the single-Tl–O-layer cuprates the Tl(6s) band lies well above the Fermi level. The metal chemistry of the single-Tl–O-layer cuprates is such as to create holes in the CuO2 layers. In the two-Tl–O-layer cuprates, it has been suggested that an internal oxidation-reduction reaction mechanism could be operative. Superconducting transition temperatures (Tc) of the cuprate superconductors have been correlated with a large number of structural parameters, such as in-plane Cu–O bond lengths, bond valence sums, Madelung potentials, and the electronegativity of the constituent ions. Among these, the in-plane Cu–O bond length is an important structural parameter that reflects the extent of oxidation of the CuO2 layer on doping.
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Electrical and magnetic properties of several oxide systems of K2NiF4 structure have been compared to those of the corresponding perovskites. Members of the La1−x Sr1+x CoO4 system are all semiconductors with a high activation energy for conduction unlike La1−x Sr x CoO3 (x ≥ 0.3) which is metallic; the latter oxides are ferromagnetic. La0.5Sr1.5CoO4 shows a magnetization of 0.5 μB at 0 K (compared to 1.5 μB of La0.5Sr0.5CoO3), but the high-temperature susceptibilities of the two systems are comparable. In SrO · (La0.5Sr0.5MnO3) n , both magnetization and electrical conductivity increase with the increase in n approaching the value of the perovskite La0.5Sr0.5MnO3. LaSrMn0.5Ni0.5(Co0.5)O4 shows no evidence of long-range ferromagnetic ordering unlike the perovskite LaMn0.5Ni0.5(Co0.5)O3; high-temperature susceptibility behavior of these two insulating systems is, however, similar. LaSr1−x Ba x NiO4 exhibits high electrical resistivity with the resistivity increasing proportionately with the magnetic susceptibility (note that LaNiO3 is a Pauli-paramagnetic metal). High-temperature susceptibility of LaSrNiO4 and LaNiO3 are comparable. Susceptibility measurements show no evidence for long-range ordering in LaSrFe1−x Ni x O4 unlike in LaFe1−x Ni x O3 (x ≤ 0.35) and the electrical resistivity of the former is considerably higher. Electrical resistivity of Sr2RuO4 is more than an order of magnitude higher than that of SrRuO3. Some generalizations of the properties of two- and three-dimensional oxide systems have emerged from these experimental observations.
Adsorption of N2, benzene and methanol have been studied on as-prepared single-walled carbon nanotubes (SWNT) as well as SWNTs treated with HCl and HNO3. These nanotubes are good microporous materials with total surface areas well above 400 m2/g and internal surface areas of 300 m2/g or higher. Benzene molecules are shown to be adsorbed within the pores of the SWNTs.
Amine‐templated zinc sulfates of the formulae, [Zn(SO 4 )(H 2 O) 2 (C 10 N 2 H 8 )] ( I ) and [C 3 N 2 H 12 ][Zn(SO 4 )] ( II ) both with linear structures have been prepared under hydro/solvothermal conditions. Of these, I has the chain structure formed by ZnO 4 N 2 octahedra and SO 4 tetrahedra, while II comprises ladders formed by corner‐sharing four‐membered rings. Amine‐templated thorium sulfates of the formula [HN(CH 2 ) 6 NH] 2 [Th 2 (SO 4 ) 6 (H 2 O) 2 ]·2H 2 O, ( III ) and [H 2 N(CH 2 ) 4 NH 2 ][Th 3 (SO 4 ) 7 (H 2 O) 4 ]·5H 2 O ( IV ) are also obtained under hydrothermal conditions. III has a sheet structure consisting of cages whereas IV has a two‐dimensional structure derived from the connectivity of ladders.
Electronic and ionic conductivities of silver selenide crystal (Ag 2 + δ Se) have been measured over a range of stoichiometry through the α-β transition by using solid state electrochemical techniques. In the high temperature β-phase Ag 2 Se shows metallic behaviour of electronic conductivity for high values of δ ; with decrease in δ, the conductivity of the material exhibits a transition. The magnitude of change in electronic conductivity at the α -β transition is also determined by stoichiometry. Ionic conductivity of the β-phase does not vary significantly with stoichiometry. A model to explain the observed transport properties has been suggested.
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Two stable tetravalent lead azides, triphenyl lead azide and diphenyl lead diazide have been prepared and characterized. Physical properties such as crystal morphology, infra-red spectra, X-ray diffraction, solubility and thermal behaviour are reported.