Department of Materials Science and Engineering, Nagoya University, Furo-cho, Chikusa, Nagoya 464-8603, Japan.
Inorg Chem. 2011 Apr 18;50(8):3281-5. doi: 10.1021/ic101916c. Epub 2011 Mar 15.
The binary skutterudite CoP(3) has a large void at the body-centered site of each cubic unit cell and is, therefore, called a nonfilled skutterudite. We investigated its room-temperature compression behavior up to 40.4 GPa in helium and argon using a diamond-anvil cell. High-pressure in situ X-ray diffraction and Raman scattering measurements found no phase transition and a stable cubic structure up to the maximum pressure in both media. A fitting of the present pressure-volume data to the third-order Birch-Murnaghan equation of state yields a zero-pressure bulk modulus K(0) of 147(3) GPa [pressure derivative K(0)' of 4.4(2)] and 171(5) GPa [where K(0)' = 4.2(4)] in helium and argon, respectively. The Grüneisen parameter was determined to be 1.4 from the Raman scattering measurements. Thus, CoP(3) is stiffer than other binary skutterudites and could therefore be used as a host cage to accommodate large atoms under high pressure without structural collapse.
具有体心位置大空穴的二元 skutterudite CoP(3) 称为非填满 skutterudite。我们使用金刚石对顶砧在氦气和氩气中研究了其室温下的压缩行为,最高压力可达 40.4 GPa。高压原位 X 射线衍射和拉曼散射测量发现,在这两种介质中,在最高压力下没有相变和稳定的立方结构。将目前的压力-体积数据拟合到第三阶 Birch-Murnaghan 状态方程,得到在氦气和氩气中的零压体弹模量 K(0) 分别为 147(3) GPa [压力导数 K(0)’为 4.4(2)] 和 171(5) GPa [其中 K(0)’= 4.2(4)]。从拉曼散射测量确定 Grüneisen 参数为 1.4。因此,CoP(3) 比其他二元 skutterudite 更硬,因此可以用作容纳高压下大原子的主体笼,而不会发生结构坍塌。