Dilawar Nita, Varandani Deepak, Mehrotra Shalini, Poswal Himanshu K, Sharma Surinder M, Bandyopadhyay Ashis K
Pressure & Vacuum Standards, National Physical Laboratory, Dr K S Krishnan Road, New Delhi 110012, India.
Nanotechnology. 2008 Mar 19;19(11):115703. doi: 10.1088/0957-4484/19/11/115703. Epub 2008 Feb 19.
We report Raman spectroscopic studies of the nanosized rare earth sesquioxides, namely yttrium sesquioxide (Y(2)O(3)), gadolinium sesquioxide (Gd(2)O(3)) and samarium sesquioxide (Sm(2)O(3)), under high pressure. The samples were characterized using x-ray diffraction, Raman spectroscopy and atomic force microscopy at atmospheric pressures. Y(2)O(3) and Gd(2)O(3) were found to be cubic at ambient, while Sm(2)O(3) was found to be predominantly cubic with a small fraction of monoclinic phase. The strongest Raman peaks are observed at 379, 344 and 363 cm(-1), respectively, for Y(2)O(3), Sm(2)O(3) and Gd(2)O(3). All the samples were found to be nanosized with 50-90 nm particle sizes. The high pressures were generated using a Mao-Bell type diamond anvil cell and a conventional laser Raman spectrometer is used to monitor the pressure-induced changes. Y(2)O(3) seems to undergo a crystalline to partial amorphous transition when pressurized up to about 19 GPa, with traces of hexagonal phase. However, on release of pressure, the hexagonal phase develops into the dominant phase. Gd(2)O(3) is also seen to develop into a mixture of amorphous and hexagonal phases on pressurizing. However, on release of pressure Gd(2)O(3) does not show any change and the transformation is found to be irreversible. On the other hand, Sm(2)O(3) shows a weakening of cubic phase peaks while monoclinic phase peaks gain intensity up to about a pressure of 6.79 GPa. However, thereafter the monoclinic phase peaks also reduce in intensity and mostly disordering sets in which does not show significant reversal as the pressure is released. The results obtained are discussed in detail.
我们报道了在高压下对纳米级稀土 sesquioxides(即氧化钇(Y₂O₃)、氧化钆(Gd₂O₃)和氧化钐(Sm₂O₃))的拉曼光谱研究。在常压下,使用 X 射线衍射、拉曼光谱和原子力显微镜对样品进行了表征。发现 Y₂O₃ 和 Gd₂O₃ 在室温下为立方晶系,而 Sm₂O₃ 主要为立方晶系,含有少量单斜相。对于 Y₂O₃、Sm₂O₃ 和 Gd₂O₃,分别在 379、344 和 363 cm⁻¹ 处观察到最强的拉曼峰。所有样品均为纳米级,粒径为 50 - 90 nm。使用 Mao - Bell 型金刚石对顶砧产生高压,并使用传统的激光拉曼光谱仪监测压力诱导的变化。当压力升至约 19 GPa 时,Y₂O₃ 似乎经历了从晶体到部分非晶态的转变,并伴有微量的六方相。然而,在压力释放时,六方相发展为主相。在加压时,Gd₂O₃也会发展为非晶态和六方相的混合物。然而,在压力释放时,Gd₂O₃ 没有显示任何变化,并且发现这种转变是不可逆的。另一方面,Sm₂O₃ 在约 6.79 GPa 的压力下,立方相峰减弱,而单斜相峰强度增加。然而,此后单斜相峰强度也降低,并且在压力释放时大多出现无序状态,没有明显的反转。详细讨论了所得结果。