Total scattering studies of silica polymorphs: similarities in glass and disordered crystalline local structure
Mineralogical Magazine Mineralogical Society 64:3 (2000) 447-457
Neutron and X-ray scattering studies of magnetism in non-superconducting PrBa2Cu3O6+x
J ALLOY COMPD 303 (2000) 489-497
Abstract:
I give a short review of neutron and X-ray scattering experiments undertaken to study the magnetic properties of non-superconducting PrBa2Cu3O6+x. The measurements have confirmed the magnetic ordering of the Pr sublattice at temperatures below T-Pr approximate to 20 K, and have revealed an incommensurate magnetic structure with a long period (similar to 600 Angstrom) involving both the Pr and Cu spins. The Cu spins in this Pr ordered phase are found to be non-collinear. Taken as a whole, the results provide strong evidence for a substantial magnetic coupling of the pseudodipolar type between the Pr and Cu ions. The effect of this coupling is also evident in the spectrum of low energy magnetic excitations determined by neutron inelastic scattering. (C) 2000 Elsevier Science S.A. All rights reserved.Structural characterization of the betatoalpha superionic transition in Ag2HgI4 and Cu2HgI4
Journal of Physics Condensed Matter IOP Publishing 12:16 (2000) 3751
An x-ray diffraction and Raman spectroscopy investigation of A-site substituted perovskite compounds: The (Na1-x Kx )0.5 Bi0.5 TiO3 (0 ≤ x ≤ 1) solid solution
Journal of Physics Condensed Matter 12:14 (2000) 3267-3280
Abstract:
The (Na1-xKx)0.5Bi0.5TiO3 perovskite solid solution is investigated using x-ray diffraction (XRD) and Raman spectroscopy in order to follow the structural evolution between the end members Na0.5Bi0.5TiO3 (rhombohedral at 300 K) and K0.5Bi0.5TiO3 (tetragonal at 300 K). The Raman spectra are analysed with special regard to the hard modes and suggest the existence of nano-sized Bi3+TiO3 and (Na1-2xK2x)+TiO3 clusters. The complementary use of XRD and Raman spectroscopy suggests, in contrast to previous reported results, that the rhombohedral ↔ tetragonal phase transition goes through an intermediate phase, located at 0.5 ≤ x ≤ 0.80. The structural character of the intermediate phase is discussed in the light of sub- and super-group relations. © 2000 IOP Publishing Ltd.Images of absolute retardance L.Deltan, using the rotating polariser method.
J Microsc 198 (Pt 1) (2000) 1-9