A Compact Furnace for Synchrotron Powder Diffraction Experiments up to 1800 K

A new electric furnace has been designed and fabricated for measurements of the high-resolution synchrotron radiation powder diffraction profiles from materials at high temperatures up to 1807 K in air, suitable for the multiple-detector system installed at the BL-4B2 experimental station of the Photon Factory, Tsukuba, Japan. In the present study, at 1703 K in air, the whole powder pattern of National Institute of Standard and Technology ceria powder was step scanned at a step interval of 0.004° in 2θ, by the counting time of 1.5 s/step and with a monochromatized 1.205363(5) A X-ray, in just 7 h. The full width at half-maximum of the 111 reflection of the ceria was narrow (0.0139°). The δd/d resolution of the ceria ranged from 0.058% to 0.126% at 1703 K, where d and δd are the lattice spacing and peak width, respectively. Precise unit-cell parameter 5.51259(1) A and the atomic displacement parameters were refined by the Rietveld analysis of the powder data measured at 1703 K. An electron-density map of ceria at 1703 K was obtained by the maximum-entropy method.

[1]  M. Yashima,et al.  Crystal structure and the structural disorder of ceria from 40 to 1497 °C , 2006 .

[2]  M. Yashima,et al.  A compact furnace for synchrotron powder diffraction measurements up to 1807 K , 2005 .

[3]  J. Schneider,et al.  In situ, high-temperature, synchrotron, powder diffraction studies of oxide systems in air, using a thermal-image furnace , 2005 .

[4]  M. Yashima,et al.  Performance of a new furnace for high‐resolution synchrotron powder diffraction up to 1900 K: application to determine electron density distribution of the cubic CaTiO3 perovskite at 1674 K , 2004 .

[5]  Masatomo Yashima,et al.  Positional disorder of oxygen ions in ceria at high temperatures , 2004 .

[6]  M. Yashima,et al.  High-temperature neutron powder diffraction study of cerium dioxide CeO2 up to 1770 K , 2003 .

[7]  M. Yashima,et al.  Dependence of the accuracy of a continuous phase transition temperature on angular resolution in powder diffractometry , 2003 .

[8]  M. Yashima In Situ observations of phase transition using high-temperature neutron and synchrotron X-ray powder diffractometry , 2003 .

[9]  M. Yashima,et al.  High-temperature synchrotron X-ray powder diffraction study of the orthorhombic-tetragonal phase transition in lanthanum titanate perovskite La0.68(Ti0.95, Al0.05)O3 , 2002 .

[10]  H. Yoshioka,et al.  High-Temperature Synchrotron X-Ray Powder Diffraction Study of the Orthorhombic–Tetragonal Phase Transition in La0.63(Ti0.92,Nb0.08)O3 , 2002 .

[11]  H. Graafsma,et al.  A 1000°C furnace for in situ X-ray diffraction , 2001 .

[12]  F. Izumi,et al.  A Rietveld-Analysis Programm RIETAN-98 and its Applications to Zeolites , 2000 .

[13]  R. Cernik,et al.  New high- and low-temperature apparatus for synchrotron polycrystalline X-ray diffraction. , 1998, Journal of synchrotron radiation.

[14]  H. Toraya,et al.  A new powder diffractometer for synchrotron radiation with a multiple-detector system. , 1996, Journal of synchrotron radiation.

[15]  F. Frey,et al.  Structure refinements of .BETA.-Si3N4 at temperatures up to 1360.DEG.C. by X-ray powder investigation. , 1994 .

[16]  T. C. Huang,et al.  Intensity Enhancement in Asymmetric Diffraction with Parallel-Beam Synchrotron Radiation , 1993 .

[17]  M. Hart,et al.  Lattice-parameter determination for powders using synchrotron radiation , 1990 .

[18]  M. Sakata,et al.  Accurate structure analysis by the maximum‐entropy method , 1990 .

[19]  F. Marumo,et al.  Diffractometer for synchrotron radiation structural studies of high temperature melts , 1989 .

[20]  P. Aldebert Neutron and X-ray experiments at high temperature , 1984 .

[21]  J. Faber,et al.  Defect characterization in CeO2−x at elevated temperatures—II: Neutron diffraction , 1976 .

[22]  J. Faber,et al.  Defect characterization in CeO2−x at elevated temperatures—I: X-Ray diffraction , 1976 .