TY - JOUR
T1 - Structural mechanisms underlying near-zero thermal expansion in β-eucryptite
T2 - A combined synchrotron X-ray and neutron Rietveld analysis
AU - Xu, Hongwu
AU - Heaney, Peter J.
AU - Yates, Douglas M.
AU - Von Dreele, Robert B.
AU - Bourke, Mark A.
N1 - Funding Information:
We are grateful to D.E. Cox, P.M. Woodward, and Q. Zhu for help with the synchrotron x-ray experiments. This work was supported by the National Science Foundation grants No. EAR-9418031 and No. EAR-9706143 (to P.J.H.) and the 1996 and 1997 crystallography scholarships from the International Center for Diffraction Data (ICDD) (to H.X.). Synchrotron x-ray diffraction was carried out at the National Synchrotron Light Source (NSLS), Brookhaven National Laboratory, and neutron diffraction was performed at the Manuel Lujan, Jr. Neutron Scattering Center (MLNSC), Los Alamos National Laboratory, which both are supported by the United States Department of Energy.
PY - 1999/7
Y1 - 1999/7
N2 - The structures of ordered and disordered β-eucryptite have been determined from Rietveld analysis of powder synchrotron x-ray and neutron diffraction data over a temperature range of 20 to 873 K. On heating, both materials show an expansion within the (001) plane and a contraction along the c axis. However, the anisotropic character of the thermal behavior of ordered β-eucryptite is much more pronounced than that of the disordered compound; the linear expansion coefficients of the ordered and disordered phases are αa = 7.26×10-6 K-1; αc = -16.35×10-6 K-1, and αa = 5.98×10-6 K-1; αc = -3.82×10-6 K-1, respectively. The thermal behavior of β-eucryptite can be attributed to three interdependent processes that all cause an increase in a but a decrease in c with increasing temperature: (i) Si/Al tetrahedral deformation, (ii) Li positional disordering, and (iii) tetrahedral tilting. Because disordered β-eucryptite does not exhibit tetrahedral tilting, the absolute values of its axial thermal coefficients are smaller than those for the ordered sample. At low temperatures, both ordered and disordered β-eucryptite exhibit a continuous expansion parallel to the c axis with decreasing temperature, whereas a remains approximately unchanged. Our difference Fourier synthesis reveals localization of Li ions below room temperature, and we suggest that repulsion between Li and Al/Si inhibits contraction along the a axes.
AB - The structures of ordered and disordered β-eucryptite have been determined from Rietveld analysis of powder synchrotron x-ray and neutron diffraction data over a temperature range of 20 to 873 K. On heating, both materials show an expansion within the (001) plane and a contraction along the c axis. However, the anisotropic character of the thermal behavior of ordered β-eucryptite is much more pronounced than that of the disordered compound; the linear expansion coefficients of the ordered and disordered phases are αa = 7.26×10-6 K-1; αc = -16.35×10-6 K-1, and αa = 5.98×10-6 K-1; αc = -3.82×10-6 K-1, respectively. The thermal behavior of β-eucryptite can be attributed to three interdependent processes that all cause an increase in a but a decrease in c with increasing temperature: (i) Si/Al tetrahedral deformation, (ii) Li positional disordering, and (iii) tetrahedral tilting. Because disordered β-eucryptite does not exhibit tetrahedral tilting, the absolute values of its axial thermal coefficients are smaller than those for the ordered sample. At low temperatures, both ordered and disordered β-eucryptite exhibit a continuous expansion parallel to the c axis with decreasing temperature, whereas a remains approximately unchanged. Our difference Fourier synthesis reveals localization of Li ions below room temperature, and we suggest that repulsion between Li and Al/Si inhibits contraction along the a axes.
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U2 - 10.1557/JMR.1999.0421
DO - 10.1557/JMR.1999.0421
M3 - Article
AN - SCOPUS:0032651372
SN - 0884-2914
VL - 14
SP - 3138
EP - 3151
JO - Journal of Materials Research
JF - Journal of Materials Research
IS - 7
ER -