欢迎登录材料期刊网

材料期刊网

高级检索

研究了尖晶石型CuAl2O4掺杂对CaCu3Ti4O12陶瓷显微结构、介电性能以及松弛特征和缺陷结构的影响。在频率为10-1~107 Hz、温度为153~453 K的条件下测量了样品的介电性能。研究表明,适量添加CuAl2O4,使样品晶粒尺寸减小并趋于均匀,击穿场强从CaCu3Ti4O12陶瓷样品的3.0 kV/cm提高到13.0 kV/cm,低频介电损耗减小。介电松弛中的高频松弛过程起源于晶粒本征缺陷的电子松弛过程,其活化能~0.10 eV基本不变;随着CuAl2O4含量增加,与界面相关的松弛活化能从0.50 eV减小到0.22 eV,可能与CuAl2O4在样品中引入杂质及更复杂的界面有关;电导活化能从0.66 eV增至0.86 eV,归因于CuAl2O4第二相抑制了晶界处的载流子跳跃,提高了Schottky势垒高度。CuAl2O4掺杂量大于100mol%,过量CuAl2O4会导致样品晶界势垒崩塌,样品失去非欧姆特性和巨介电性能。

The influences of CuAl2O4 doping on the microstructure and dielectric relaxation of CaCu3Ti4O12 (CCTO) ceramics were investigated. The dielectric properties were measured in the frequency from 10-1 Hz to 107 Hz under the temperature from 153 to 453 K. It was found that reduced CCTO grains as well as improved microstruc-ture were achieved by addition of 30mol%–50mol% CuAl2O4. When sintered at 1100℃ for 4 h, enhanced electric breakdown field of 13 kV/cm was obtained with 50mol% CuAl2O4 addition, while its dielectric loss at low fre-quency was greatly suppressed. Three energy levels of dielectric relaxation processes were found. It is suggested that energy level 1 eV of ~0.10 eV, corresponding to high frequency relaxation and barely varied with CuAl2O4 ad-dition, is attributed to the intrinsic electronic relaxation. Energy level 2 decreased from 0.50 eV to 0.22 eV with in-creased additional CuAl2O4, possibly resulted from multi impurities and boundaries. The energy level of conduction process rose from 0.66 eV to 0.86 eV with increased CuAl2O4 addition, which can be attributed to the block effect of more grain boundaries. In addition, the excessive content CuAl2O4 resulted in collapse of grain boundary barrier, leading to the vanish of non-ohmic properties and high dielectric constant.

参考文献

[1] Subramanian MA.;Duan N.;Reisner BA.;Sleight AW.;Li D..High dielectric constant in ACu(3)Ti(4)O(12) and ACu(3)Ti(3)FeO(12) phases[J].International Journal of Quantum Chemistry,20002(2):323-325.
[2] Extrinsic models for the dielectric response of CaCu_(3)Ti_(4)O_(12)[J].Journal of Applied Physics,20035(5):3299-3306.
[3] Sung-Yoon Chung;Il-Doo Kim;Suk-Joong L.Kang.Strong nonlinear current-voltage behaviour in perovskite-derivative calcium copper titanate[J].Nature materials,200411(11):774-778.
[4] Yuan-Hua Lin;Jingnan Cai;Ming Li;Ce-Wen Nan;Jinliang He.High dielectric and nonlinear electrical behaviors in TiO_(2)-rich CaCu_(3)Ti_(4)O_(12) ceramics[J].Applied physics letters,200617(17):172902-1-172902-3-0.
[5] Liu Y;Withers RL;Wei XY.Structurally frustrated relaxor ferroelectric behavior in CaCu3Ti4O12[J].Physical review, B. Condensed matter and materials physics,200513(13):4104-1-4104-4-0.
[6] Krohns S;Lunkenheimer P;Ebbinghaus SG;Loidl A.Colossal dielectric constants in single-crystalline and ceramic CaCu3Ti4O12 investigated by broadband dielectric spectroscopy[J].Journal of Applied Physics,20088(8):84107-1-84107-9-0.
[7] 郝文涛;张家良;谭永强;郑鹏;王春雷.CaCu3Ti4O12陶瓷高介电性的起因机制[J].无机材料学报,2011(10):1058-1062.
[8] Xiao Jing Luo;Chang Ping Yang;Xue Ping Song.Slow Relaxation Processes in CCTO Detected by Capacitance Versus Voltage Curves[J].Journal of the American Ceramic Society,20131(1):253-258.
[9] Timothy B. Adams;Derek C. Sinclair;Anthony R. West.Giant Barrier Layer Capacitance Effects in CaCu_3Ti_4O_(12) Ceramics[J].Advanced Materials,200218(18):1321-1323.
[10] Wen-Xiang Yuan;S.K. Hark.Investigation on the origin of the giant dielectric constant in CaCu_3Ti_4O_(12) ceramics through analyzing CaCu_3Ti_4O_(12)-HfO_2 composites[J].Journal of the European Ceramic Society,20122(2):465-470.
[11] Jiancong Yuan;Yuan-Hua Lin;Huafei Lu.Dielectric and Varistor Behavior of CaCu_3Ti_4O_(12)-MgTiO_3 Composite Ceramics[J].Journal of the American Ceramic Society,20117(7):1966-1969.
[12] 贾然;顾访;吴珍华;赵学童;李建英.简化共沉淀法制备CaCu3Ti4O12陶瓷及其介电性能研究[J].物理学报,2012(20):466-472.
[13] Lei Zhang;Zhong-Jia Tang.Polaron relaxation and variable-range-hopping conductivity in the giant-dielectric-constant material CaCu_3Ti_4O_(12)[J].Physical review, B. Condensed matter and materials physics,200417(17):174306.1-174306.6.
[14] 周小莉;杜丕一.CaCu3Ti4O12的制备及其对巨介电性能的影响[J].无机材料学报,2005(2):484-488.
[15] Li-Then Mei;Hsing-I Hsiang;Tsang-Tse Fang.Effect of Copper-Rich Secondary Phase at the Grain Boundaries on the Varistor Properties of CaCu_3Ti_4O_(12) Ceramics[J].Journal of the American Ceramic Society,200811(11):3735-3737.
[16] Li, J.;Jia, R.;Tang, X.;Zhao, X.;Li, S..Enhanced electric breakdown field of CaCu_3Ti_4O _(12) ceramics: Tuning of grain boundary by a secondary phase[J].Journal of Physics, D. Applied Physics: A Europhysics Journal,201332(32):325304-1-325304-6.
[17] Ran Jia;Xuetong Zhao;Jianying Li.Colossal breakdown electric field and dielectric response of Al-doped CaCu_3Ti_4O_(12) ceramics[J].Materials Science & Engineering, B. Solid-State Materials for Advanced Technology,2014:79-85.
[18] Shao SF;Zhang JL;Zheng P;Zhong WL;Wang CL.Microstructure and electrical properties of CaCu3Ti4O12 ceramics[J].Journal of Applied Physics,20068(8):84106-1-84106-11-0.
[19] 杨雁;李盛涛;李晓;吴高林;王谦;鲍明晖.CaCu3Ti4O12陶瓷深陷阱松弛特性研究[J].无机材料学报,2012(11):1185-1190.
[20] Jianying Li;Xuetong Zhao;Fang Gu;Shengtao Li.Defects and dc electrical degradation in CaCu_(3)Ti_(4)O_(12) ceramics: Role of oxygen vacancy migration[J].Applied physics letters,201220(20):202905-1-202905-4.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%