Journal of Inorganic Materials ›› 2014, Vol. 29 ›› Issue (1): 62-66.DOI: 10.3724/SP.J.1077.2014.13212

• Research Paper • Previous Articles     Next Articles

Giant Dielectric-Permittivity Property of NaCu3Ti3NbO12 and NaCu3Ti3SbO12 Ceramics and Low Dielectric Loss in NaCu3Ti3SbO12 Ceramics

HAO Wen-Tao1,2, XU Pan-Pan3, ZHANG Jia-Liang3, CAO En-Si1,2, PENG Hua1,2   

  1. (1. Key Laboratory of Advanced Transducers and Intelligent Control Systems, Taiyuan University of Technology, Taiyuan 030024, China; 2. College of Physics and Optoelectronics, Taiyuan University of Technology, Taiyuan 030024, China; 3. School of Physics, Shandong University, Jinan 250100, China)
  • Received:2013-04-15 Revised:2013-05-22 Published:2014-01-20 Online:2013-12-09

Abstract: NaCu3Ti3NbO12 and NaCu3Ti3SbO12 ceramics were prepared by the conventional solid state reaction method, and their dielectric properties and crystalline structure were investigated. It was found that they were quite similar with the CaCu3Ti4O12 ceramics, showing giant dielectric-permittivity properties with ε' larger than 7×103. Within the measuring frequency range of 40 Hz-100 MHz, a single dielectric relaxation with the characteristic frequency around 1 MHz was detected at room temperature or below whereas an additional one in low frequency region is also observed at high temperatures. Furthermore, the existence of CuO secondary phase was confirmed by X-ray diffraction. In general, the results can be explained by the similar mechanism of internal barrier layer capacitance effect which was formerly proposed for CaCu3Ti4O12 ceramics. Here, it is worthy pointing out that the tanδ of NaCu3Ti3SbO12 ceramics is lower than 0.05 in a large frequency range from 40 Hz to 7 kHz, and the tanδ at 1 kHz is lower than 0.05 in a large temperature range of -50℃ to 80℃ at 1 kHz, which is a desirable characteristic for practical applications.

Key words: NaCu3Ti3NbO12, NaCu3Ti3SbO12, giant dielectric-permittivity phenomena, internal barrier layer capacitance effect

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