首页> 外文期刊>Journal of Applied Physics >Temperature dependent Raman scattering and far-infrared reflectance spectra of MgO modified Pb0.99(Zr0.95Ti0.05)0.98Nb0.02O3 ceramics: A composition effect
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Temperature dependent Raman scattering and far-infrared reflectance spectra of MgO modified Pb0.99(Zr0.95Ti0.05)0.98Nb0.02O3 ceramics: A composition effect

机译:MgO修饰的Pb 0.99 (Zr 0.95 Ti 0.05 0.98 的温度依赖性拉曼散射和远红外反射光谱Nb 0.02 O 3 陶瓷的组成效应

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摘要

Lattice dynamics and phase transition of MgO modified Pb0.99(Zr0.95Ti0.05)0.98Nb0.02O3 (PZTN-x wt. % MgO, x = 0, 0.1, 0.2, 0.5) ceramics have been investigated by far-infrared (FIR) reflectance in the temperature range of 5.5–300 K and Raman spectra between 77 and 300 K, respectively. With the aid of above complementary methods, the structure of all ceramics was defined as low-temperature ferroelectric rhombohedral phase [ FR(LT)] at room temperature. The FIR dielectric functions were extracted from the multi-Lorentz oscillator dispersion model. The lowest frequency phonon mode, which is related to Pb-BO3 (B = Zr, Ti, Nb) vibration, mainly dominates the FIR dielectric response. With increasing MgO composition, the dielectric constants ε(0) at room temperature are estimated to 85.4, 73.4, 73.9, and 41.9, respectively. The decreasing trend can be due to the doubly ionized oxygen vacancies induced by Mg substitution for B-site. The order-disorder phase transition located around 120 K can be clearly clarified from temperature evolution of phonon frequency, damping, and intensity. It decreases slightly with increasing MgO composition, which influence the distortion due to the broken correlation chains and local permanent dipoles creation. Moreover, the transformation from antiferroelectric orthorhombic AO to [FR(LT)] phase has been observed around 250 K, which is associated with the antiferroelectric displacement of Pb atoms along 〈110〉 and coupled rotations of the corner-connected oxygen octahedral. Furthermore, the transition from [FR(LT)] to [FR(HT)] (high-temperature ferroelectric rhombohedral phase) was identified a- ound 290 K for MgO-doped PZTN ceramics. It arises from the shift of cation (Pb and Zr/Ti/Nb/Mg ions) along the 〈111〉 direction and the transition temperature slightly decreases compared to the pure ceramic.
机译:MgO修饰的Pb 0.99 (Zr 0.95 Ti 0.05 0.98 Nb 0.02的晶格动力学和相变 O 3 (PZTN-x wt。%MgO,x = 0,0.1,0.2,0.5)的陶瓷已经通过5.5的温度范围内的远红外(FIR)反射率进行了研究–300 K和拉曼光谱分别在77和300 K之间。借助于上述补充方法,将所有陶瓷的结构定义为室温下的低温铁电菱面体相[ F R(LT) ]。从多洛伦兹振荡器频散模型中提取了FIR介电函数。最低频率的声子模式与Pb-BO 3 (B = Zr,Ti,Nb)振动有关,主要决定了FIR介电响应。随着MgO组成的增加,室温下的介电常数ε(0)分别估计为85.4、73.4、73.9和41.9。下降趋势可能是由于M取代B位引起的双离子氧空位。从声子频率,阻尼和强度的温度变化可以清楚地阐明位于120 K附近的有序-无序相变。它随着MgO组成的增加而略有降低,这会影响相关链断裂和局部永久偶极子产生的畸变。此外,观察到从反铁电正交的 A O [F R(LT)] 的转变。 250 K,这与Pb原子沿
的反铁电位移以及角连接的氧八面体的耦合旋转有关。此外,从<公式> [F R(LT)] 过渡到<公式> [F R(HT)] (高MgO掺杂的PZTN陶瓷在290 K左右被确定为高温铁电菱形面相。它是由于阳离子(Pb和Zr / Ti / Nb / Mg离子)沿 〈111〉 方向移动而引起的,并且其转变温度与纯陶瓷相比略有下降。

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  • 来源
    《Journal of Applied Physics》 |2014年第9期|1-8|共8页
  • 作者单位

    Key Laboratory of Polar Materials and Devices, Ministry of Education, Department of Electronic Engineering, East China Normal University, Shanghai 200241, China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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