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富钛NaYCuTiO陶瓷的巨介电性能和麦克斯韦-瓦格纳弛豫显著改善。

Significantly Improved Colossal Dielectric Properties and Maxwell-Wagner Relaxation of TiO-Rich NaYCuTiO Ceramics.

作者信息

Saengvong Pariwat, Chanlek Narong, Putasaeng Bundit, Pengpad Atip, Harnchana Viyada, Krongsuk Sriprajak, Srepusharawoot Pornjuk, Thongbai Prasit

机构信息

Giant Dielectric and Computational Design Research Group (GD-CDR), Department of Physics, Faculty of Science, Khon Kaen University, Khon Kaen 40002, Thailand.

Synchrotron Light Research Institute (Public Organization), 111 University Avenue, Muang District, Nakhon Ratchasima 30000, Thailand.

出版信息

Molecules. 2021 Oct 5;26(19):6043. doi: 10.3390/molecules26196043.

Abstract

In this work, the colossal dielectric properties and Maxwell-Wagner relaxation of TiO-rich NaYCuTiO ( = 0-0.2) ceramics prepared by a solid-state reaction method are investigated. A single phase of NaYCuTiO is achieved without the detection of any impurity phase. The highly dense microstructure is obtained, and the mean grain size is significantly reduced by a factor of 10 by increasing Ti molar ratio, resulting in an increased grain boundary density and hence grain boundary resistance (). The colossal permittivities of ' ~ 0.7-1.4 × 10 with slightly dependent on frequency in the frequency range of 10-10 Hz are obtained in the TiO-rich NaYCuTiO ceramics, while the dielectric loss tangent is reduced to tanδ ~ 0.016-0.020 at 1 kHz due to the increased . The semiconducting grain resistance () of the NaYCuTiO ceramics increases with increasing , corresponding to the decrease in Cu/Cu ratio. The nonlinear electrical properties of the TiO-rich NaYCuTiO ceramics can also be improved. The colossal dielectric and nonlinear electrical properties of the TiO-rich NaYCuTiO ceramics are explained by the Maxwell-Wagner relaxation model based on the formation of the Schottky barrier at the grain boundary.

摘要

在本工作中,研究了通过固相反应法制备的富TiO₂的NaYCuTiO₄(x = 0 - 0.2)陶瓷的巨介电性能和麦克斯韦-瓦格纳弛豫。获得了单相的NaYCuTiO₄,未检测到任何杂质相。得到了高密度的微观结构,通过增加Ti摩尔比,平均晶粒尺寸显著减小了10倍,导致晶界密度增加,从而晶界电阻(Rgb)增大。在富TiO₂的NaYCuTiO₄陶瓷中,获得了ε' ~ 0.7 - 1.4×10³且在10² - 10⁶Hz频率范围内对频率略有依赖的巨介电常数,而由于Rgb增大,在1kHz时介电损耗正切降低至tanδ ~ 0.016 - 0.020。NaYCuTiO₄陶瓷的半导体晶粒电阻(Rg)随着x的增加而增大,这与Cu²⁺/Cu⁺比例的降低相对应。富TiO₂的NaYCuTiO₄陶瓷的非线性电学性能也得到了改善。基于晶界处肖特基势垒的形成,通过麦克斯韦-瓦格纳弛豫模型解释了富TiO₂的NaYCuTiO₄陶瓷的巨介电和非线性电学性能。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fc45/8512015/8898536bf050/molecules-26-06043-g001.jpg

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