Structure and bulk modulus of Ln-doped UO2 (Ln = La, Nd) at high pressure

被引:13
|
作者
Rittman, Dylan R. [1 ]
Park, Sulgiye [1 ]
Tracy, Cameron L. [1 ]
Zhang, Lei [2 ,3 ,4 ]
Palomares, Raul I. [5 ]
Lang, Maik [5 ]
Navrotsky, Alexandra [2 ,3 ,4 ]
Mao, Wendy L. [1 ,6 ]
Ewing, Rodney C. [1 ]
机构
[1] Stanford Univ, Dept Geol Sci, Stanford, CA 94305 USA
[2] Univ Calif Davis, Peter A Rock Thermochem Lab, Davis, CA 95616 USA
[3] Univ Calif Davis, NEAT ORU, Davis, CA 95616 USA
[4] Univ Calif Davis, Dept Chem Engn & Mat Sci, Davis, CA 95616 USA
[5] Univ Tennessee, Dept Nucl Engn, Knoxville, TN 37996 USA
[6] SLAC Natl Accelerator Lab, Stanford Inst Mat & Energy Sci, Menlo Pk, CA 94025 USA
基金
美国国家科学基金会;
关键词
MECHANICAL-PROPERTIES; THERMAL-CONDUCTIVITY; ELASTIC PROPERTIES; URANIUM-DIOXIDE; DIFFRACTION; OXIDES; OXYGEN;
D O I
10.1016/j.jnucmat.2017.04.007
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The structure of lanthanide-doped uranium dioxide, Ln(x)U(1-x)O(2-0.5x+y) (Ln = La, Nd), was investigated at pressures up to similar to 50-55 GPa. Samples were synthesized with different lanthanides at different concentrations (x similar to 0.2 and 0.5), and all were slightly hyperstoichiometric (y similar to 0.25-0.4). In situ high-pressure synchrotron X-ray diffraction was used to investigate their high-pressure phase behavior and determine their bulk moduli. All samples underwent a fluorite-to-cotunnite phase transformation with increasing pressure. The pressure of the phase transformation increased with increasing hyper-stoichiometry, which is consistent with results from previous computational simulations. Bulk moduli are inversely proportional to both the ionic radius of the lanthanide and its concentration, as quantified using a weighted cationic radius ratio. This trend was found to be consistent with the behavior of other elastic properties measured for Ln-doped UO2, such as Young's modulus. (C) 2017 Elsevier B.V. All rights reserved.
引用
收藏
页码:28 / 33
页数:6
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