15 research outputs found

    Cubic lead perovskite PbMoO3 with anomalous metallic behavior

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    A previously unreported Pb-based perovskite PbMoO3_3 is obtained by high-pressure and high-temperature synthesis. This material crystallizes in the Pm3ˉmPm\bar{3}m cubic structure at room temperature, making it distinct from typical Pb-based perovskite oxides with a structural distortion. PbMoO3_3 exhibits a metallic behavior down to 0.1 K with an unusual TT-sub linear dependence of the electrical resistivity. Moreover, a large specific heat is observed at low temperatures accompanied by a peak in CP/T3C_P/T^3 around 10 K, in marked contrast to the isostructural metallic system SrMoO3_3. These transport and thermal properties for PbMoO3_3, taking into account anomalously large Pb atomic displacements detected through diffraction experiments, are attributed to a low-energy vibrational mode, associated with incoherent off-centering of lone pair Pb2+^{2+} cations. We discuss the unusual behavior of the electrical resistivity in terms of a polaron-like conduction, mediated by the strong coupling between conduction electrons and optical phonons of the local low-energy vibrational mode.Comment: 5 pages, 5 figure

    Random Fan-Out State Induced by Site-Random Interlayer Couplings

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    We study the low-temperature properties of a classical Heisenberg model with site-random interlayer couplings on the cubic lattice. This model is introduced as a simplified effective model of Sr(Fe1x_{1-x}Mnx_{x})O2_2, which was recently synthesized. In this material, when x=0.3x=0.3, (πππ)(\pi\pi\pi) and (ππ0)(\pi\pi0) mixed ordering is observed by neutron diffraction measurements. By Monte Carlo simulations, we find an exotic bulk spin structure that explains the experimentally obtained results. We name this spin structure the "random fan-out state". The mean-field calculations provide an intuitive understanding of this phase being induced by the site-random interlayer couplings. Since Rietveld analysis assuming the random fan-out state agrees well with the neutron diffraction pattern of Sr(Fe0.7_{0.7}Mn0.3_{0.3})O2_2, we conclude that the random fan-out state is reasonable for the spin-ordering pattern of Sr(Fe0.7_{0.7}Mn0.3_{0.3})O2_2 at the low-temperature phase.Comment: 13 pages, 12 figure

    Pressure-induced amorphization of a dense coordination polymer and its impact on proton conductivity

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    The proton conductivity of a dense coordination polymer (CP) was investigated under high-pressure conditions. Impedance measurements under high pressures revealed that the proton conductivity of the CP decreased more than 1000-fold at pressures of 3–7 GPa and that the activation energy for proton conduction almost doubled compared with that at ambient pressure. A synchrotron X-ray study under high pressure identified the amorphization process of the CP during compression, which rationally explains the decrease in conductivity and increase in activation energy. This phenomenon is categorized as reversible pressure-induced amorphization of a dense CP and is regarded as a demonstration of the coupling of the mechanical and electrical properties of a CP

    Infinite-layer iron oxide with a square-planar coordination

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    簡便な手法により、化学の常識を覆す鉄酸化物を発見. 京都大学プレスリリース. 2007-12-13.Conventional high-temperature reactions limit the control of coordination polyhedra in transition-metal oxides to those obtainable within the bounds of known coordination geometries for a given transition metal. For example, iron atoms are almost exclusively coordinated by three-dimensional polyhedra such as tetrahedra and octahedra. However, recent works have shown that binary metal hydrides act as reducing agents at low temperatures, allowing access to unprecedented structures. Here we show the reaction of a perovskite SrFeO3 with CaH2 to yield SrFeO2, a new compound bearing a square-planar oxygen coordination around Fe2+. SrFeO2 is isostructural with 'infinite layer' cupric oxides, and exhibits a magnetic order far above room temperature in spite of the two-dimensional structure, indicating strong in-layer magnetic interactions due to strong Fe d to O p hybridization. Surprisingly, SrFeO2 remains free from the structural instability that might well be expected at low temperatures owing to twofold orbital degeneracy in the Fe2+ ground state with D4h point symmetry. The reduction and the oxidation between SrFeO2 and SrFeO3 proceed via the brownmillerite-type intermediate SrFeO2.5, and start at the relatively low temperature of 400 K, making the material appealing for a variety of applications, including oxygen ion conduction, oxygen gas absorption and catalysis

    Theoretical band structure of the superconducting antiperovskite Sr₃₋ₓ SnO

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    In order to investigate the position of the strontium deficiency in superconductive Sr₃₋ₓ SnO, we synthesized and measured X-ray-diffraction patterns of Sr₃₋ₓ SnO (x ~ 0.5). Because no clear peaks originating from superstructures were observed, strontium deficiency is most likely to be randomly distributed. We also performed first-principles band-structure calculations on Sr₃₋ₓ SnO (x = 0, 0.5) using two methods: full-potential linearized-augmented plane-wave plus local orbitals method and the Korringa-Kohn-Rostoker Green function method combined with the coherent potential approximation. We revealed that the Fermi energy of Sr₃₋ₓ SnO in case of x ~ 0.5 is about 0.8 eV below the original Fermi energy of the stoichiometric Sr₃SnO, where the mixing of the valence p and conduction d orbitals are considered to be small
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