首页> 外文期刊>Journal of Materials Research >Structural mechanisms underlying near-zero thermal expansion in β -eucryptite: A combined synchrotron x-ray and neutron Rietveld analysis
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Structural mechanisms underlying near-zero thermal expansion in β -eucryptite: A combined synchrotron x-ray and neutron Rietveld analysis

机译:β-锂霞石中近零热膨胀的结构机理:同步加速器X射线和中子Rietveld分析

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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 (00l) 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 α_a = 7.26 x 10~(-6) K~(-1), α_c = -16.35 x 10~(-6) K~(-1), and α_a = 5.98 x 10~(-6) K~(-1); α_c = -3.82 x 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.
机译:根据粉末同步加速器X射线和中子衍射数据的Rietveld分析,在20至873 K的温度范围内,确定了有序和无序的β-锂霞石的结构。加热时,两种材料均在(00l)平面内膨胀,并且沿c轴收缩。然而,有序β-锂霞石的热行为的各向异性特征比无序化合物的热行为更加明显。有序和无序相的线性膨胀系数为α_a= 7.26 x 10〜(-6)K〜(-1),α_c= -16.35 x 10〜(-6)K〜(-1),α_a= 5.98 x 10〜(-6)K〜(-1); α_c= -3.82 x 10〜(-6)K〜(-1)。 β-锂霞石的热行为可归因于三个相互依赖的过程,这些过程都随温度的升高而导致c的增加而c的降低:(i)Si / Al四面体形变;(ii)Li位置无序;以及(iii)四面体倾斜。由于无序的β-锂霞石不表现出四面体倾斜,因此其轴向热系数的绝对值小于订购样品的绝对值。在低温下,随着温度降低,有序的和无序的β-锂霞石都表现出平行于c轴的连续膨胀,而a保持大致不变。我们的差异傅里叶合成揭示了室温以下锂离子的局限性,并且我们建议锂与Al / Si之间的排斥作用会抑制沿a轴的收缩。

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