Mineral Physics Institute, Stony Brook University, Stony Brook, NY 11794, USA.
J Phys Condens Matter. 2014 Jan 22;26(3):035104. doi: 10.1088/0953-8984/26/3/035104. Epub 2013 Nov 28.
The structural behavior of GeO2 glass has been investigated up to 64 GPa using results from x-ray absorption spectroscopy in a diamond anvil cell combined with previously reported density measurements. The difference between the nearest Ge-O distances of glassy and rutile-type GeO2 disappears at the Ge-O distance maximum at 20 GPa, indicating completion of the tetrahedral-octahedral transition in GeO2 glass. The mean-square displacement σ(2) of the Ge-O distance in the first Ge-O shell increases progressively to a maximum at 10 GPa, followed by a substantial reduction at higher pressures. The octahedral glass is, as expected, less dense and has a higher compressibility than the corresponding crystalline phase, but the differences in Ge-O distance and density between the glass and the crystals are gradually eliminated over the 20-40 GPa pressure range. Above 40 GPa, GeO2 forms a dense octahedral glass with a compressibility similar to that of the corresponding crystalline phase (α-PbO2 type). The EXAFS and XANES spectra show evidence for subtle changes in the dense glass continuing to occur at these high pressures. The Ge-O bond distance shows little change between 45-64 GPa, and this may reflect a balance between bond shortening and a gradual coordination number increase with compression. The density of the glass is similar to that of the α-PbO2-type phase, but the Ge-O distance is longer and is close to that in the higher-coordination pyrite-type phase which is stable above ∼60 GPa. The density data provide evidence for a possible discontinuity and change in compressibility at 40-45 GPa, but there are no major changes in the corresponding EXAFS spectra. A pyrite-type local structural model for the glass can provide a reasonable fitting to the XAFS spectra at 64 GPa.
采用金刚石对顶压腔中的 X 射线吸收光谱学与之前报道的密度测量相结合的方法,研究了 GeO2 玻璃在高达 64 GPa 的压力下的结构行为。玻璃态和金红石型 GeO2 的最近 Ge-O 距离之差在 20 GPa 时的 Ge-O 距离最大值处消失,表明 GeO2 玻璃中的四面体-八面体转变已经完成。第一壳层中 Ge-O 距离的均方根位移 σ(2)在 10 GPa 时逐渐增大到最大值,然后在更高的压力下大幅减小。正如预期的那样,八面体玻璃的密度较低,压缩性较高,但其与相应的晶体相之间的 Ge-O 距离和密度差异在 20-40 GPa 的压力范围内逐渐消除。在 40 GPa 以上,GeO2 形成了一种高密度的八面体玻璃,其压缩性与相应的晶体相(α-PbO2 型)相似。EXAFS 和 XANES 谱表明,在这些高压下,致密玻璃中仍存在细微变化的证据。Ge-O 键长在 45-64 GPa 之间几乎没有变化,这可能反映了键缩短和配位数随压缩逐渐增加之间的平衡。玻璃的密度与α-PbO2 型相相似,但 Ge-O 距离较长,接近于在较高配位的黄铁矿型相,在约 60 GPa 以上稳定。密度数据为 40-45 GPa 时可能出现的不连续性和压缩性变化提供了证据,但相应的 EXAFS 谱没有发生重大变化。玻璃的黄铁矿型局部结构模型可以为 64 GPa 时的 XAFS 谱提供合理的拟合。