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Slim P-E hysteresis loop and anomalous dielectric response in sol-gel derived antiferroelectric PbZrO_3 thin films

机译:溶胶-凝胶反铁电PbZrO_3薄膜中的细P-E磁滞回线和异常介电响应

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摘要

Sol-gel derived PbZrO_3 (PZ) thin films have been deposited on Pt(111)/Ti/SiO_2/Si substrate and according to the pseudotetragonal symmetry of PZ, the relatively preferred (110), oriented phase formation has been noticed. The room temperature P-E hysteresis loops have been observed to be slim by nature. The slim hysteresis loops are attributed to the [110], directional antiparallel lattice motion of Pb ions and by the directionality of the applied electric field. Pure PZ formation has been characterized by the dielectric phase transition at 235 ℃ and antiferroelectric P-E hysteresis loops at room temperature. Dielectric response has been characterized within a frequency domain of 100 Hz-1 MHz at various temperatures ranging from 40 to 350 ℃. Though frequency dispersion of dielectric behaves like a Maxwell-Wagner type of relaxation, ω~2 dependency of ac conductivity indicates that there must be G-C equivalent circuit dominance at high frequency. The presence of trap charges in PZ has been determined by Arrhenius plots of ac conductivity. The temperature dependent n (calculated from the universal power law of ac conductivity) values indicate an anomalous behavior of the trapped charges. This anomaly has been explained by strongly and weakly correlated potential wells of trapped charges and their behavior on thermal activation. The dominance of circuit/circuits resembling Maxwell-Wagner type has been investigated by logarithmic Nyquist plots at various temperatures and it has been justified that the dielectric dispersion is not from the actual Maxwell-Wagner-type response.
机译:溶胶凝胶衍生的PbZrO_3(PZ)薄膜已沉积在Pt(111)/ Ti / SiO_2 / Si衬底上,并且根据PZ的拟四边形对称性,已经注意到相对优选的(110)取向相形成。室温下的P-E磁滞回线已被观察到是细长的。细长的磁滞回线归因于[110],Pb离子的定向反平行晶格运动以及所施加电场的方向性。纯PZ的形成具有235℃的介电相变和室温下反铁电P-E磁滞回线的特征。在40至350℃的各种温度下,介电响应的特征是在100 Hz-1 MHz的频域内。尽管电介质的频率色散表现得像麦克斯韦-瓦格纳(Maxwell-Wagner)型弛豫一样,但交流电导率的ω〜2依赖性表明在高频下必须有G-C等效电路优势。 PZ中陷阱电荷的存在已通过交流电导率的Arrhenius图确定。与温度相关的n(根据交流电导率的通用幂定律计算)值表示捕获的电荷的异常行为。这种异常已通过被困电荷的势阱和它们在热激活下的行为之间的强弱相关来解释。已经通过在不同温度下的对数奈奎斯特图研究了类似于麦克斯韦-瓦格纳类型的电路的主导地位,并且已经证明介电色散不是来自实际的麦克斯韦-瓦格纳类型响应。

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  • 来源
    《Journal of Applied Physics》 |2008年第2期|636-646|共11页
  • 作者单位
  • 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);
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  • 正文语种 eng
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