岩盐Li3 +xMg 2-2xNb 1-XTi 2xO6固溶体系的晶格演化、有序变换和微波介电性能:一种新建立的伪三元相图

Xing Zhang, Xiao Zhang, Z. Fang, Hongyu Yang, Z. Xiong, Hongcheng Yang, Shuren Zhang, B. Tang
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引用次数: 3

摘要

基于Li2TiO3-Li3NbO4-MgO伪三元相图,设计了新型多组分Li3+ xm_2 - 2xnbn - xti2xo6(0≤x≤1)固溶陶瓷,并对其进行了毫米波应用研究。该陶瓷在Li3Mg2NbO6和Li2TiO3端元之间表现出全方位的固溶性。随着掺杂含量(x)的增加,我们检测到正交相、立方相和单斜相之间的相变是由成分变化驱动的,并且伴随着有序-无序-有序转变。此外,在低掺杂浓度(x=0.2)样品的电子衍射图像中观察到光滑的正交-立方相变界面,并且在正交-立方相变界面附近都可以观察到基于正交或立方结构的重构超晶格。Q×f值的变化随着超晶格的出现而显著增加,并且Q×f值的增强与包含重构超晶格的结构中晶格振动非调和性非常小有关。典型地,在1250℃烧结4 h时,x=0.2样品的介电损耗为er=16.1, Q×f=128,600 GHz (f=9.2 GHz), τf=-30.4 ppm/℃;x=0.9样品的介电损耗为er=20.4, Q×f=90,300 GHz (f=7.9 GHz), τf=2.9 ppm/℃。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Lattice Evolution, Ordering Transformation and Microwave Dielectric Properties of Rock-Salt Li3 +xMg 2-2xNb 1-XTi 2xO6 Solid-Solution System: A Newly Developed Pseudo Ternary Phase Diagram
The new types of multi-component Li3+xMg2-2xNb1-xTi2xO6 (0≤x≤1) solid-solution ceramics were designed based on the Li2TiO3-Li3NbO4-MgO pseudo ternary phase diagram and studied for millimeter-wave applications. The ceramics showed a full range of solid solubility between the Li3Mg2NbO6 and Li2TiO3 endmembers. As the doping content (x) increased, we detected the phase transitions among the orthorhombic, cubic, and monoclinic phase driven by the compositional changes, as well as accompanied with an order-disorder-order transformation. Besides, the smooth orthorhombic-cubic phase transition interfaces were observed in the electron diffraction images for the sample with the low dopant concentration (x=0.2), and the reconstructed superlattices based on the orthorhombic or the cubic structure were both observed nearby the orthorhombic-cubic phase transition interface. The change of Q×f values showed a considerable increase with the emergence of the superlattices, and the enhancement of the Q×f values was related to the very small lattice vibrational anharmonicity in the structures that contain the reconstructed superlattices. Typically, when sintered at 1250 ℃ for 4 h, the ultra-low dielectric loss was achieved in the x=0.2 sample with the properties of er=16.1, Q×f=128,600 GHz (f=9.2 GHz) and τf=-30.4 ppm/℃, and the temperature stable properties were obtained in the x=0.9 sample with er=20.4, Q×f=90,300 GHz (f=7.9 GHz), and τf=2.9 ppm/℃.
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