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首页> 外文期刊>CERAMICS INTERNATIONAL >Phase structures, microstructures, and dielectric characteristics of high epsilon(r) (1-x-y)Bi0.5Na0.5TiO3-xLi(0.5)Sm(0.5)TiO(3)-yNa(0.5)La(0.5)TiO(3) microwave ceramic systems
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Phase structures, microstructures, and dielectric characteristics of high epsilon(r) (1-x-y)Bi0.5Na0.5TiO3-xLi(0.5)Sm(0.5)TiO(3)-yNa(0.5)La(0.5)TiO(3) microwave ceramic systems

机译:高ε(R)(1-XY)Bi0.5Na0.5TiO3-XLI(0.5)SM(0.5)TiO(3)-YNA(0.5)La(0.5)TiO(0.5)TiO(3)的相结构 微波陶瓷系统

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Ultrahigh dielectric constant (epsilon(r)) (1-x-y)Bi0.5Na0.5TiO3-xLi(0.5)Sm(0.5)TiO(3)-yNa(0.5)La(0.5)TiO(3) (BNT-LST-NLT, 0.3 <= x <= 0.7, 0.0 <= y <= 0.4) microwave ceramic systems were fabricated using a conventional solid-state reaction method, and their phase structures, microstructures, and microwave dielectric characteristics were systematically investigated. From XRD pattern analyses and refinement results, (1-x-y)BNT-xLST-yNLT (x-- 0.3-0.6 and y = 0.4-0.1) samples were crystallized into a cubic perovskite structure, and XRD peaks corresponding to the (031), (131), and (230) planes were identified as super-reflections belonging to the tilt system of orthorhombic a(-) a(-) b(+) with the Pnma space group. In particular, on the basis of the Raman spectra and microwave dielectric properties analysis results, the crystal structure of the sample (x = 0.6 and y = 0.1) sintered at 1200 degrees C for 4 h was considered to be closer to orthorhombic symmetry. In addition, solid orthorhombic perovskite-type solutions were formed together with a small amount of secondary phase Sm2Ti2O7 as x = 0.6 and y = 0.2, 0.3. However, an increase in the Sm2Ti2O7 phase content was also detected for x = 0.7 and y = 0.0, accompanied by the perovskite phase. For the microwave dielectric properties, the epsilon(r) and Q x f values strongly depended on the apparent density, ionic polarizability, phase structure, and phase composition, and also, the tau(f) value was predicted by adjusting the tolerance factor (t). The epsilon(r) and tau(f) values basically agreed with the existing models, such as the mixing rule. As a result, the (1-x-y)BNT-xLST-yNLT (x = 0.6 and y = 0.1) ceramic sample sintered at 1200 degrees C for 4 h exhibited superior microwave dielectric properties of epsilon(r) similar to 149.1, Q x f similar to 3270 GHz, and tau(f) similar to 39.1 ppm/degrees C
机译:超高介电常数(ε(R))(1-xy)Bi0.5Na0.5tio3-XLI(0.5)SM(0.5)TiO(3)-YNA(0.5)La(0.5)TiO(3)(BNT-LST-使用常规的固态反应方法制造NLT,0.3 <= x <= 0.7,0.0 <= Y <= 0.4)微波陶瓷系统,系统地研究了它们的相结构,微观结构和微波介电特性。从XRD模式分析和细化结果,(1-XY)BNT-XLST-YNLT(X-- 0.3-0.6和Y = 0.4-0.1)样品被结晶成立方钙钛矿结构,以及对应于(031)的XRD峰值(131)和(230)平面被鉴定为属于与PNMA空间组的正交A( - )A( - )B(+)的倾斜系统的超反射。特别地,基于拉曼光谱和微波介电性质分析结果,认为在1200℃下烧结4小时的样品(x = 0.6和y = 0.1)的晶体结构被认为更接近正交对称。此外,固体正交钙钛矿型溶液与少量的二次相Sm 2 O 7一起形成,为x = 0.6,y = 0.2,0.3。然而,对于X = 0.7和Y = 0.0,也检测到SM2Ti2O7相含量的增加,伴随钙钛矿相。对于微波介电性质,ε(R)和Q XF值强烈地依赖于表观密度,离子极化性,相结构和相位组成,并且还通过调节公差因子来预测TAU(F)值(T. )。 epsilon(r)和tau(f)值基本上与现有模型相同,例如混合规则。结果,在1200摄氏度下烧结的(1-XY)BNT-XLST-YNLT(x = 0.6和Y = 0.1)烧结4小时,表现出类似于149.1,Q XF的epsilon(R)的优异的微波介电性能类似于3270 GHz,和TAU(F)类似于39.1 ppm /℃

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