铁电纳米复合材料畴切换诱发的近室温大电致发光效应

Zeqing Yu, X. Hou, Sizheng Zheng, Chen Bin, Jieying Wang
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引用次数: 0

摘要

基于铁电材料电积效应(ECE)的固态制冷技术具有效率高、易于微型化等优点,因此被视为蒸汽压缩系统的一种有前途的替代技术。然而,铁电材料的绝热温度变化(ATC)小和工作温度范围窄是其 ECE 制冷实际应用的主要障碍。为了提高铁电聚合物聚偏氟乙烯 [P(VDF-TrFE)] 的 ECE 性能,本文引入了极化度较大的 PbZr1-xTixO3 (PZT) 纳米粒子,形成铁电纳米复合材料。相场模拟用于研究铁电纳米复合材料的动态磁滞环和相应的畴演化。利用基于麦克斯韦关系的间接方法计算了随温度变化的 ATC 值。在填充了 PbZr0.1Ti0.9O3 纳米颗粒的 P(VDF-TrFE)纳米复合材料[P(VDF-TrFE)-PZT0.9]中观察到了双磁滞环的出现,这主要是由于微观畴由单畴转变为极性漩涡引起的。与 P(VDF-TrFE)相比,P(VDF-TrFE)-PZT0.9 中与畴转变相关的 ATC 值得到了增强,优异 ECE 的温度范围也得到了有效拓宽。此外,随着填充的 PZT 纳米粒子的分量 x 的增加以跨越各向形态相边界(MPB),最大 ATC 值也显著增加。本文的研究结果不仅解释了 P(VDF-TrFE)-PZT 纳米复合材料的畴转变诱导优异 ECE 的机理,而且对今后通过引入铁电纳米填料增强 P(VDF-TrFE)ECE 的研究具有启发意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Large electrocaloric effect near room temperature induced by domain switching in ferroelectric nanocomposites
The solid-state refrigeration technique based on the electrocaloric effect (ECE) of ferroelectric materials has been regarded as a promising alternative to vapor compression systems due to its advantages of high efficiency and easy miniaturization. However, the small adiabatic temperature change (ATC) and narrow operating temperature range of ferroelectric materials are key obstacles for their practical applications of ECE refrigeration. To improve the ECE performance of ferroelectric polymer poly(vinylidene fluoride) [P(VDF-TrFE)], PbZr1−xTixO3 (PZT) nanoparticles with larger polarization is herein introduced to form ferroelectric nanocomposites. The phase-field simulation is employed to investigate the dynamic hysteresis loops and corresponding domain evolution of the ferroelectric nanocomposites. The temperature-dependent ATC values are calculated using the indirect method based on the Maxwell relation. The appearance of the double hysteresis loop is observed in P(VDF-TrFE) nanocomposite filled with PbZr0.1Ti0.9O3 nanoparticles [P(VDF-TrFE)–PZT0.9], which is mainly caused by a microscopic domain transition from single domain to polar vortex. Compared to the P(VDF-TrFE), enhanced ATC values associated with the domain transition are unveiled in P(VDF-TrFE)–PZT0.9, and the temperature range of excellent ECE is also effectively broadened. In addition, as the component x of filled PZT nanoparticles increases to cross the morphotropic phase boundary (MPB), the maximum ATC value shows a significant increase. The results presented in this work not only explain the mechanism of domain transition induced excellent ECE in the P(VDF-TrFE)–PZT nanocomposite, but also stimulate future studies on enhancing ECE of P(VDF-TrFE) by introducing ferroelectric nanofillers.
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