4.7 Article

Evolution of the structure, dielectric and ferroelectric properties of Na0.5Bi0.5TiO3-added BaTiO3-Bi(Mg2/3Nb1/3)O3 ceramics

期刊

CERAMICS INTERNATIONAL
卷 46, 期 16, 页码 25392-25398

出版社

ELSEVIER SCI LTD
DOI: 10.1016/j.ceramint.2020.07.007

关键词

Energy storage; BaTiO3; Na0.5Bi0.5TiO3; Relaxor ferroelectric

资金

  1. Natural Science Foundation of China [51702196, 51702197]
  2. Research Starting Foundation of Shaanxi University of Science and Technology [BJ16-07]
  3. China Postdoctoral Science Foundation [2017M620435]

向作者/读者索取更多资源

Via a traditional sintering process, (1-x) [0.85BaTiO(3)-0.15Bi(Mg2/3Nb1/3)O-3] - x Na0.5Bi0.5TiO3 (x = 0, 0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1) (BT-BMN-NBT) ceramics were synthesized. The sintering temperature and density of the BT-BMN-NBT ceramics decreased with the increasing NBT content. All samples exhibited a pseudocubic phase and formed stable solid solutions with dense microstructures. The crystal structure of the BT-BMN-NBT ceramics gradually transformed from BT to NBT with increasing NBT content. The introduction of NBT with a high maximum polarization (P-max) could not only enhance the relaxor ferroelectric (RFE) characteristics of the BT-based RFE, but also compensate for the reduction in P-max of BT-based RFE that is due to the enhanced RFE characteristics. The temperature that corresponds to the maximum dielectric constant increases monotonously with the NBT content. P-max of the BT-BMN-NBT ceramics increases significantly as the NBT content increases. The best energy storage (ES) performances (x = 0.3) of a releasable energy density (W-rec) of 2.91 J/cm(3) and 85.55% efficiency were realized at 200 kV/cm. Compared with the unmodified BT-BMN ceramics (1.67 J/cm(3)), W-rec was improved by 1.48 times, which originated from the NBT modification induced increase in P-max (39.5 mu C/cm(2)) to 2.34 times the nominal BT-BMN value (16.9 mu C/cm(2)). The results prove that the addition of NBT could improve the ES performances of BT-based relaxor ferroelectrics at low-field by increasing the polarization.

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