Influence of Zn nonstoichiometry on the phase structure, microstructure and microwave dielectric properties of Nd(Zn0.5Ti0.5)O3 ceramics

被引:8
|
作者
Li, Jiamao [1 ,2 ,3 ]
Fan, Chuangang [1 ]
Cheng, Zhenxiang [2 ]
Ran, Songlin [3 ]
机构
[1] Anhui Univ Technol, Sch Mat Sci & Engn, Maanshan 243032, Peoples R China
[2] Univ Wollongong, Inst Superconducting & Elect Mat, Wollongong, NSW 2500, Australia
[3] Anhui Univ Technol, Minist Educ, Key Lab Met Emiss Reduct & Resources Recycling, Maanshan 243002, Peoples R China
关键词
Ceramics; Perovskite; Microstructure; Microwave dielectric properties; TEMPERATURE;
D O I
10.1016/j.jallcom.2019.04.195
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The double perovskites Nd(Zn0.5+xTi0.5)O-3 (x = 0.05, 0.03, 0.01, 0, -0.01, -0.03 and -0.05) have been prepared successfully by conventional route for mixing oxides. The influences of Zn nonstoichiometry on the phase composition, microstructure and microwave dielectric properties have been systematically discussed. A small amount of Zn nonstoichiometry (-0.01 <= x <= 0.03) did not change the phase composition but a large amount of Zn excess (x = 0.05) and deficient (x = -0.03 and -0.05) caused the appearances of secondary phases Zn2TiO4 and Nd2Ti2O7, respectively. A significant difference in grain size could be observed in the Zn nonstoichiometry ceramics. The sinterability and density were reduced due to the presence of the impurity phase Nd2Ti2O7 for the Zn-deficient ceramics, while Nd2Ti2O7 could adjust temperature coefficient of resonant frequency (tau(f)) to near-zero. The tau(f) of the Nd(Zn0.5+xTi0.5)O-3 (x = -0.05-0.05) ceramics was significantly affected by the Zn nonstoichiometry. After sintered at 1360 degrees C for 4 h, the nonstoichiometric Zn0.51+xTi0.5)O-3 ceramics showed favorable microwave dielectric properties: dielectric constant epsilon(r) = 36.41, quality factor Q x f = 182650 GHz, and tau(f )= -26.5 ppm/degrees C and the Zn0.47+xTi0.5)O-3 ceramics possessed a near-zero tau(f )value of -5.6 ppm/degrees C, accompanying by a high epsilon(r) and a moderate Q x f (epsilon(r) = 27.75, Q x f = 47820 GHz ). (C) 2019 Elsevier B.V. All rights reserved.
引用
收藏
页码:385 / 392
页数:8
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