Structural effects on the magnetic and transport properties of perovskite 0.30)
Physical Review B - Condensed Matter and Materials Physics 56:13 (1997) 8265-8276
Abstract:
The evolution of the structural properties of (Formula presented) was determined as a function of temperature, average (Formula presented)-site radius (Formula presented) and applied pressure for the “optimal” doping range (Formula presented) 0.30, by using high-resolution neutron powder diffraction. The metal-insulator transition, which can be induced both as a function of temperature and of (Formula presented) was found to be accompanied by significant structural changes. Both the paramagnetic charge-localized phase, which exists at high temperatures for all values of (Formula presented) and the spin-canted ferromagnetic charge-ordered phase, which is found at low temperatures for low values of (Formula presented) are characterized by large metric distortions of the (Formula presented) octahedra. These structural distortions are mainly incoherent with respect to the space-group symmetry, with a significant coherent component only at low (Formula presented) These distortions decrease abruptly at the transition into the ferromagnetic metal phase. These observations are consistent with the hypothesis that, in the insulating phases, lattice distortions of the Jahn-Teller type, in addition to spin scattering, provide a charge-localization mechanism. The evolution of the average structural parameters indicates that the variation of the electronic bandwidth is the driving force for the evolution of the insulator-to-metal transition at (Formula presented) as a function of “chemical” and applied pressure. © 1997 The American Physical Society.Structural instability around Tc observed in Hg-1201 by neutron powder diffraction and EXAFS
Physica C: Superconductivity and its Applications 282-287:PART 2 (1997) 1081-1082
Abstract:
The structure of HgBa2CuO4+∂ is studied as function of temperature by neutron diffraction and Cu-Kedge EXAFS on the same powder sample with Tc=97K. Both techniques reveal the presence of an anomalous behaviour of the Cu-O in-plane bond length starting at ≈ 140K.Crystal chemistry and electronic properties of the N=2 Ruddlesden-Popper manganates: Unconventional CMR materials
MATER RES SOC SYMP P 453 (1997) 331-336
Abstract:
The crystallography and electronic properties of the Ln(2-x)Sr(1+x)Mn(2)O(7) manganese oxides adopting the n = 2 Ruddlesden-Popper (RP) structure are discussed, focusing on the structural phase diagrams and electronic properties in the vicinity of the Mn + 3.5 oxidation slate and in particular the ease of synthesis of single phases of these materials.Cs3H(SeO4)(2) at 300 K by high-resolution neutron powder diffraction
ACTA CRYSTALLOGRAPHICA SECTION C-CRYSTAL STRUCTURE COMMUNICATIONS 53 (1997) 1529-1531
Hysteresis of the pressure-induced Jahn-Teller switch in deuterated ammonium copper(II) Tutton salt, (ND4)(2)[Cu(D2O)(6)](SO4)(2)
INORGANIC CHEMISTRY 36:15 (1997) 3382-&