Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
11020057 | Solid State Communications | 2019 | 14 Pages |
Abstract
In the study, Zr0.5Hf0.5V2âxPxO7 (0â¯â¤â¯xâ¯â¤â¯1.2) was prepared by solid state method and then the microstructure of synthesized samples was investigated. The microstructure, coefficient of thermal expansion (CTE) and phase transition of Zr0.5Hf0.5V2âxPxO7 (0â¯â¤â¯xâ¯â¤â¯1.2) were investigated with thermal dilatometry, x-ray diffraction (XRD) and Raman spectroscopy. The results showed that the samples were single cubic phase with the space group of Pa3¯ in the crystal structure. When the substitution rate of P5+ was higher than 0.6, the 3â¯Ãâ¯3â¯Ãâ¯3 superstructure disappeared. The expansion coefficient of Zr0.5Hf0.5V1.2P0.8O7 was calculated to be â0.53â¯Ãâ¯10â6â¯Kâ1 under the linear thermal expansion in a very wide temperature range from 300 to 573â¯K. With the increase of P5+ content, the temperatures of positive-to-negative thermal expansion of Zr0.5Hf0.5V2âxPxO7 firstly even decreased below room temperature and then increased. The synthesized Zr0.5Hf0.5V2âxPxO7 exhibited near zero thermal expansion behavior in a wide temperature range around room temperature.
Related Topics
Physical Sciences and Engineering
Materials Science
Materials Science (General)
Authors
Junping Wang, Qingdong Chen, Sailei Li, Yanjun Ji, GaoJie Zeng, Youwen Liu, Erjun Liang,