Structures of K(0.05)Na(0.95)NbO3 (50-300 K) and K(0.30)Na(0.70)NbO3 (100-200 K).

Acta Crystallogr B 65:Pt 3 (2009) 291-299

Authors:

N Zhang, AM Glazer, D Baker, PA Thomas

Abstract:

Rietveld refinement using neutron powder diffraction data is reported for the potential lead-free piezoelectric material K(x)Na(1-x)NbO3 (x = 0.05, x = 0.3) at low temperatures. The structures were determined to be of rhombohedral symmetry, space group R3c, with the tilt system a(-)a(-)a(-) for both compositions. It was found that some of the structural parameters differ significantly in the two structures, and particularly the NbO6 octahedral strains as a function of temperature. The 300 K profile for K(0.05)Na(0.95)NbO3 shows the coexistence of rhombohedral and monoclinic phases, which indicates that the phase boundary is close to room temperature; the phase boundary for K(0.30)Na(0.70)NbO3 is found to be at approximately 180 K.

Circularly polarised X-rays as a probe of non-collinear magnetic order in multiferroic TbMnO3

(2009)

Authors:

F Fabrizi, HC Walker, L Paolasini, F de Bergevin, AT Boothroyd, D Prabhakaran, DF McMorrow

Low-temperature interactions of magnetic excitons in LaCoO3

Physical Review B - Condensed Matter and Materials Physics 79:17 (2009)

Authors:

SR Giblin, I Terry, D Prabhakaran, AT Boothroyd, C Leighton

Abstract:

The low-temperature magnetic behavior of LaCoO3, containing oxygen vacancies, is reported. Magnetic-susceptibility measurements made in the temperature range of 0.5-35 K on a single crystal and a polycrystalline sample provide strong evidence for the existence of magnetic excitons as fundamental entities within the bulk of the material system. Specifically, two distinct types of excitons form, isolated and interacting excitons, both of which are associated with oxygen vacancies. Isolated magnetic excitons act as high-spin paramagnetic particles while the interacting excitons appear to be coupled antiferromagnetically. It is proposed that the interaction arises from the overlap of magnetic excitons as a consequence of the statistical clustering of oxygen vacancies. The striking similarity of these results with those of the lightly doped La0.97 Sr0.03 CoO3 suggests that the observed excitons are a precursor to magneto-electronic phase separation and supports the idea that phase separation is initiated by disorder in the material system. © 2009 The American Physical Society.

A high resolution, hard x-ray photoemission investigation of La_(2-2x)Sr_(1+2x)Mn_2O_7 (0.30

(2009)

Authors:

S de Jong, F Massee, Y Huang, M Gorgoi, F Schaefers, J Fink, AT Boothroyd, D Prabhakaran, JB Goedkoop, MS Golden

ChemInform Abstract: Structure and Superconductivity of LiFeAs.

ChemInform Wiley 40:10 (2009) no-no

Authors:

Michael J Pitcher, Dinah R Parker, Paul Adamson, Sebastian JC Herkelrath, Andrew T Boothroyd, Richard M Ibberson, Michela Brunelli, Simon J Clarke