Change in compressibility of -AlOOH and -AlOOD at high pressure: A study of isotope effect and hydrogen-bond symmetrization

压缩性 环境压力 化学 静水压力 体积模量 各向异性 衍射 氢键 高压 压缩(物理) 结晶学 热力学 材料科学 复合材料 物理 分子 有机化学 光学 量子力学
作者
Asami Sano–Furukawa,Hiroyuki Kagi,Takaya Nagai,Satoshi Nakano,Satoshi Fukura,Daichi Ushijima,Riko Iizuka,Eiji Ohtani,T. Yagi
出处
期刊:American Mineralogist [Mineralogical Society of America]
卷期号:94 (8-9): 1255-1261 被引量:82
标识
DOI:10.2138/am.2009.3109
摘要

The compression behaviors of δ-AlOOH and δ-AlOOD were investigated under quasi-hydrostatic conditions at pressures up to 63.5 and 34.9 GPa, respectively, using results from synchrotron X-ray diffraction experiments conducted at ambient temperature. Because of the geometric isotope effect, at ambient pressure, the a and b axes of δ-AlOOD, which define the plane in which the hydrogen bond lies, are longer than those of δ-AOOH. Under increasing pressure, the a and b axes of δ-AlOOH stiffen at 10 GPa, although the c axis shows no marked change. Identical behavior was found in δ-AlOOD, but the change in compressibility was observed at a slightly higher pressure of 12 GPa. Axial ratios a/c and b/c first decrease rapidly with increasing pressure, then begin to increase at pressures >10 GPa in δ-AlOOH and >12 GPa in δ-AlOOD. At these pressures, the pressure dependence of a/b also changes from increasing to decreasing. The unit-cell volumes of δ-AlOOH and δ-AlOOD become slightly less compressible at high pressures. Assuming K0′ = 4, the calculated bulk moduli of δ-AlOOH below and above 10 GPa are 152(2) and 219(3) GPa, respectively. Those of δ-AlOOD below and above 12 GPa are 151(1) and 207(2) GPa, respectively.

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