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Advances in data reduction of high-pressure x-ray powder diffraction data from two-dimensional detectors: a case study of schafarzikite (FeSb2O4)

B Hinrichsen et al 2006 J. Phys.: Condens. Matter 18 S1021-S1037   doi: 10.1088/0953-8984/18/25/S09  Help

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B Hinrichsen1, R E Dinnebier1, P Rajiv1, M Hanfland2, A Grzechnik3 and M Jansen1
1 Max-Planck-Institute for Solid State Research, Heisenbergstrasse 1, D-70569 Stuttgart, Germany
2 European Synchrotron Radiation Facility, 6 rue Jules Horowitz, BP220, 38043 Grenoble Cedex, France
3 Departamento de Fisica de la Materia Condensada, Facultad de Ciencia y Technologia, Universidad del Pais Vasco, Apartado 644, E-48080 Bilbao, Spain
E-mail: r.dinnebier@fkf.mpg.de

Abstract. Methods have been developed to facilitate the data analysis of multiple two-dimensional powder diffraction images. These include, among others, automatic detection and calibration of Debye–Scherrer ellipses using pattern recognition techniques, and signal filtering employing established statistical procedures like fractile statistics.

All algorithms are implemented in the freely available program package Powder3D developed for the evaluation and graphical presentation of large powder diffraction data sets.

As a case study, we report the pressure dependence of the crystal structure of iron antimony oxide FeSb2O4 (p≤21 GPa, T = 298 K) using high-resolution angle dispersive x-ray powder diffraction. FeSb2O4 shows two phase transitions in the measured pressure range. The crystal structures of all modifications consist of frameworks of Fe2+O6 octahedra and irregular Sb3+O4 polyhedra. At ambient conditions, FeSb2O4 crystallizes in space group P42/mbc (phase I). Between p = 3.2 GPa and 4.1 GPa it exhibits a displacive second order phase transition to a structure of space group P 21/c (phase II, a = 5.7792(4) Å, b = 8.3134(9) Å, c = 8.4545(11) Å, β = 91.879(10)°, at p = 4.2 GPa). A second phase transition occurs between p = 6.4 GPa and 7.4 GPa to a structure of space group P42/m (phase III, a = 7.8498(4) Å, c = 5.7452(5) Å, at p = 10.5 GPa). A nonlinear compression behaviour over the entire pressure range is observed, which can be described by three Vinet equations in the ranges from p = 0.52 GPa to p = 3.12 GPa, p = 4.2 GPa to p = 6.3 GPa and from p = 7.5 GPa to p = 19.8 GPa. The extrapolated bulk moduli of the high-pressure phases were determined to K0 = 49(2) GPa for phase I, K0 = 27(3) GPa for phase II and K0 = 45(2) GPa for phase III. The crystal structures of all phases are refined against x-ray powder data measured at several pressures between p = 0.52 GPa, and 10.5 GPa.

Print publication: Issue 25 (28 June 2006)
Received 19 December 2005, in final form 9 February 2006
Published 8 June 2006

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