Department of Basic Science and Mathematics, Faculty of Science, Thaksin University, Songkhla Campus, Songkhla, 90000, Thailand.
Giant Dielectric and Computational Design Research Group (GD-CDR), Department of Physics, Faculty of Science, Khon Kaen University, Khon Kaen, 40002, Thailand.
Sci Rep. 2023 Mar 21;13(1):4638. doi: 10.1038/s41598-023-31879-z.
A modified sol-gel method was used to successfully produce NaYCuTiO ceramics with high dielectric permittivity. The dielectric permittivity of NaYCuTiO ceramics reaches values larger than 10 at room temperature and 1 kHz. Moreover, these ceramics exhibit two distinct thermally induced dielectric relaxations over a broad temperature range. The loss tangent is indeed small, ~0.032-0.035. At low temperatures, dielectric relaxation was attributed to the oxygen vacancy effect, while at high temperatures, it was attributed to grain boundary and sample-electrode contact effects. Our calculations revealed that Y and Na ions are likely to occupy Ca and Cu sites, respectively. As a result, other Cu related phases, especially CuO, were observed at the grain boundaries. Based on our analysis, there is a charge compensation between Na and Y ions in NaYCuTiO. Additionally, the Cu and Ti states observed in our XPS study originate from the presence of an oxygen vacancy in the lattice. Last, the primary cause of the enormous dielectric permittivity of NaYCuTiO ceramics primarily comes from the internal barrier layer capacitor effect.
采用改进的溶胶-凝胶法成功制备了具有高介电常数的 NaYCuTiO 陶瓷。NaYCuTiO 陶瓷的介电常数在室温下和 1 kHz 时大于 10。此外,这些陶瓷在很宽的温度范围内表现出两个明显的热诱导介电弛豫。损耗角正切确实很小,约为 0.032-0.035。在低温下,介电弛豫归因于氧空位效应,而在高温下,归因于晶界和样品-电极接触效应。我们的计算表明,Y 和 Na 离子可能分别占据 Ca 和 Cu 位。因此,在晶界处观察到了其他与 Cu 相关的相,特别是 CuO。基于我们的分析,在 NaYCuTiO 中存在 Na 和 Y 离子的电荷补偿。此外,我们的 XPS 研究中观察到的 Cu 和 Ti 态源自晶格中的氧空位。最后,NaYCuTiO 陶瓷具有巨大介电常数的主要原因来自于内部势垒层电容器效应。