Structure and thermal expansion of Lu2O3 and Yb2O3 up to the melting points

被引:42
作者
Pavlik, Alfred, III [1 ,2 ]
Ushakov, Sergey V. [1 ,2 ]
Navrotsky, Alexandra [1 ,2 ]
Benmore, Chris J. [3 ]
Weber, Richard J. K. [3 ,4 ]
机构
[1] Univ Calif Davis, Peter A Rock Thermochem Lab, One Shields Ave, Davis, CA 95616 USA
[2] Univ Calif Davis, NEAT ORU, One Shields Ave, Davis, CA 95616 USA
[3] Argonne Natl Lab, Xray Sci Div, Adv Photon Source, 9700 S Cass Ave, Lemont, IL 60439 USA
[4] Mat Dev Inc, 3090 Daniels Court, Arlington Hts, IL 60004 USA
基金
美国国家科学基金会;
关键词
HIGH-TEMPERATURE LIQUIDS; RARE-EARTH SESQUIOXIDES; ENERGY X-RAY; NEUTRON-SCATTERING; AERODYNAMIC LEVITATION; CRYSTAL-STRUCTURES; HAUTE TEMPERATURE; DES SESQUIOXYDES; OXIDES; UO2;
D O I
10.1016/j.jnucmat.2017.08.031
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Knowledge of thermal expansion and high temperature phase transformations is essential for prediction and interpretation of materials behavior under the extreme conditions of high temperature and intense radiation encountered in nuclear reactors. Structure and thermal expansion of Lu2O3 and Yb2O3 were studied in oxygen and argon atmospheres up to their melting temperatures using synchrotron X-ray diffraction on laser heated levitated samples. Both oxides retained the cubic bixbyite C-type structure in oxygen and argon to melting. In contrast to fluorite-type structures, the increase in the unit cell parameter of Yb2O3 and Lu2O3 with temperature is linear within experimental error from room temperature to the melting point, with mean thermal expansion coefficients (8.5 +/- 0.6).10(-6) K-1 and (7.7 +/- 0.6).10(-6) K-1, respectively. There is no indication of a superionic (Bredig) transition in the C-type structure or of a previously suggested Yb2O3 phase transformation to hexagonal phase prior to melting. (C) 2017 Elsevier B.V. All rights reserved.
引用
收藏
页码:385 / 391
页数:7
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