Colossal permittivity and ultralow dielectric loss in (Nd0.5Ta0.5)xTi1-xO2 ceramics

被引:29
作者
Xu, Zhenpeng [1 ,2 ]
Li, Lingxia [1 ,2 ]
Wang, Wenbo [1 ,2 ]
Lu, Te [1 ,2 ]
机构
[1] Minist Educ, Sch Microelect, Tianjin 300072, Peoples R China
[2] Minist Educ, Key Lab Adv Ceram & Machining Technol, Tianjin 300072, Peoples R China
基金
中国国家自然科学基金;
关键词
Colossal permittivity; Ultralow dielectric loss; Activation energy; Polarization; TEMPERATURE;
D O I
10.1016/j.ceramint.2019.05.290
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
Giant permittivity ceramic is one of the most significant classes of material to realize the miniaturization and integration of a high-performance capacitor. In this paper, to realize good giant dielectric properties, the (Nd0.5Ta0.5)(x)Ti1-xO2 ceramics (NTTO x = 0.005, 0.01, 0.03, 0.05) were synthesized by a standard conventional solid-state reaction. Comparing with the previous co-doped TiO2 ceramics giant permittivity material system, NTTO ceramics perform extremely colossal permittivity and ultralow dielectric loss (1%NTTO: epsilon = 82052, tan delta = 0.008 at 1 kHz; 5%NTTO: epsilon = 170131, tan delta = 0.090 at 1 kHz). The broad distinction of the dielectric behavior between the (Nd0.5Ta0.5)(x)Ti1-xO2 ceramics can be explained by the impedance analysis and the calculated polarization activation energies. The main electron-pinned defect-dipole (denoted as EPDD) polarization corresponds to the ultralow loss, embodying in the maximum value of E-gb (the activation energy of the grain boundary), E-a2 (the EPDD polarization activation energies) and the minimum value of E-a1 (the total polarization activation energies). Though the interfacial polarization can cause the permittivity increase, it can also give rise to poor frequency stability and higher loss.
引用
收藏
页码:17318 / 17324
页数:7
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