首页> 外文OA文献 >Raman spectroscopy study of internal dynamics in Pb(Zn_{1/3}Nb_{2/3})O_{3} and 95.55%Pb(Zn_{1/3}Nb_{2/3})O_{3}-4.5%PbTiO_{3} crystals
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Raman spectroscopy study of internal dynamics in Pb(Zn_{1/3}Nb_{2/3})O_{3} and 95.55%Pb(Zn_{1/3}Nb_{2/3})O_{3}-4.5%PbTiO_{3} crystals

机译:拉曼光谱研究内部动力学   pb(Zn_ {1/3} Nb_ {2/3})O_ {3}和95.55%pb(Zn_ {1/3} Nb_ {2/3})O_ {3} -4.5%pbTiO_ {3}   晶体

摘要

Pb(Zn$_{1/3}$Nb$_{2/3}$)O$_{3}$ is one of the simplest representatives of thelead ferroelectric relaxors. Its solid solution with PbTiO$_{3}$, atconcentrations near the morphotropic phase boundary, is especially important.In this paper, we apply the tested earlier on Pb(Mg$_{1/3}$Nb$_{2/3}$)O$_{3}$approach, to analyze the light scattering from both, nominally purePb(Zn$_{1/3}$Nb$_{2/3} $)O$_{3}$ crystal and a crystal containing 4.5% ofPbTiO$_{3}$, measured in a broad temperature range from 1000 to 100 K. Wepropose a comprehensive picture of the temperature evolution of the latticedynamics in these crystals and associated structural transformations. We show,that in PZN, like in PMN, short-lived dynamic lattice distortions exist even atthe highest measured temperatures. With cooling down, these distortions developin Fm$\bar{3}$m clusters and R3m polar nanoregions that are still capable ofreorientational motion. From the Burns temperature T$_{d}$, this motion becomesprogressively restricted. The freezing process starts at the temperatureT$^{*}$ and continues down to T$_{d0}$. The major Raman lines in all thesematerials behave very similarly. However, the temperature behavior of a weakline E in each case is essentially different. Its splitting can serve as ameasure of the order parameter of the system.
机译:Pb(Zn $ _ {1/3} $ Nb $ _ {2/3} $)O $ _ {3} $是铅铁电弛豫器的最简单代表之一。在固溶相边界附近的浓度下,它的固溶态PbTiO $ _ {3} $非常重要。在本文中,我们将较早的测试结果应用于Pb(Mg $ _ {1/3} $ Nb $ _ {2 / 3} $)O $ _ {{3} $方法,以分析名义上为纯Pb(Zn $ _ {1/3} $ Nb $ _ {2/3} $)O $ _ {3} $的光散射晶体和含有4.5%PbTiO $ _ {3} $的晶体,在1000至100 K的较宽温度范围内进行了测量。我们提出了这些晶体的晶格动力学及其相关的结构转变的温度演化的综合图。我们证明,在PZN中,就像在PMN中一样,即使在最高的测量温度下,也存在短暂的动态晶格畸变。随着冷却,这些变形会在Fm $ \ bar {3} $ m团簇和R3m极性纳米区域中发展,这些区域仍然能够进行定向运动。从伯恩斯温度T $ _ {d} $,该运动逐渐受到限制。冻结过程开始于温度T $ ^ {*} $,然后继续下降到T $ _ {d0} $。所有这些材料中的主要拉曼谱线表现得非常相似。但是,在每种情况下,弱线E的温度行为本质上是不同的。它的拆分可以作为系统顺序参数的一种度量。

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