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Polarization Properties and Polarization Depth Profiles of (Cd:Zn)S/P(VDF-TrFE) Composite Films in Dependence of Optical Excitation

机译:(Cd:Zn)S / P(VD​​F-TrFE)复合膜的偏振特性和偏振深度分布

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摘要

The influence of optical excitation intensity on the electrical, ferroelectric and pyroelectric properties of ferroelectric-semiconductor-composites was investigated. For this purpose, composite thin films consisting of poly(vinylidene fluoride-co-trifluoroethylene) and 10 vol % (Cd:Zn)S particles with a thickness of 34 µm were fabricated. The samples were used to measure the absolute pyrocoefficient and to determine the relative pyroelectric depth profile using Laser Intensity Modulated Method. It was shown that a polarization of the samples without an optical excitation at the utilized relatively small peak-to-peak voltages could not be verified by the Sawyer–Tower circuit and the measurement setup of the pyroelectric coefficient, respectively. Both remanent polarization and pyroelectric coefficients increased with increasing optical excitation intensity during poling as well as increasing peak-to-peak voltage. The pyrocoefficient shows a temporal decay in the first hours after poling. The specific heat and thermal conductivity or the thermal diffusivity are required for the calibration of the pyroelectric depth profile. Rule of mixture and photo-acoustic investigations proved that the thermal properties of the utilized composites do not differ significantly from those of the pristine polymer. Based on the pyroelectric depth profile which is proportional to the polarization profile, the existing “three phase model” has been extended to generate a replacement circuit diagram, explaining the local polarization due to the optical excitation dependency for both local resistivity and local field strength.
机译:研究了光激发强度对铁电半导体复合材料的电,铁电和热电性质的影响。为此,制造了由聚偏二氟乙烯-三氟乙烯共聚物和10%(体积)(Cd:Zn)S颗粒组成的复合薄膜,其厚度为34μm。使用激光强度调制方法,将样品用于测量绝对热解系数并确定相对热解深度分布。结果表明,在所利用的相对较小的峰峰电压下,没有光激发的样品的极化分别无法通过Sawyer-Tower电路和热释电系数的测量装置来验证。极化过程中,剩余极化和热电系数都随光激发强度的增加以及峰峰值电压的增加而增加。热极化系数在极化后的最初几小时内显示出时间衰减。比热和热导率或热扩散率是热电深度分布的校准所必需的。混合规则和光声研究证明,所用复合材料的热性能与原始聚合物的热性能没有显着差异。基于与极化分布成比例的热释电深度分布,现有的“三相模型”已扩展为生成替换电路图,解释了由于光激发对局部电阻率和局部场强的依赖性而引起的局部极化。

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