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Frequency and voltage dependence dielectric properties, ac electrical conductivity and electric modulus profiles in Al/Co3O4-PVA/p-Si structures

机译:Al / Co3O4-PVA / p-Si结构中与频率和电压相关的介电特性,交流电导率和电模量曲线

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摘要

In this research a simple microwave-assisted method have been used for preparation of cobalt oxide nanostructures. The as-prepared sample has been investigated by UV vis spectroscopy, X-ray diffraction (XRD), scanning electron microscopy (SEM). On the other hand, frequency and voltage dependence of both the real and imaginary parts of dielectric constants (epsilon', epsilon '') and electric modulus (Mf and M ''), loss tangent (tan delta), and ac electrical conductivity (sigma(ac)) values of Al/Co3O4-PVA/p-Si structures were obtained in the wide range of frequency and voltage using capacitance (C) and conductance (G/co) data at room temperature. The values of epsilon, epsilon '' and tan delta were found to decrease with increasing frequency almost for each applied bias voltage, but the changes in these parameters become more effective in the depletion region at low frequencies due to the charges at surface states and their relaxation time and polarization effect. While the value of sigma is almost constant at low frequency, increases almost as exponentially at high frequency which are corresponding to sigma(dc) and sigma(ac), respectively. The M' and M '' have low values at low frequencies region and then an increase with frequency due to short-range mobility of charge carriers. While the value of M '' increase with increasing frequency, the value of M '' shows two peak and the peaks positions shifts to higher frequency with increasing applied voltage due to the decrease of the polarization and N-ss effects with increasing frequency. (C) 2016 Elsevier B.V. All rights reserved.
机译:在这项研究中,一种简单的微波辅助方法已用于制备氧化钴纳米结构。制备的样品已通过紫外可见光谱,X射线衍射(XRD),扫描电子显微镜(SEM)进行了研究。另一方面,介电常数的实部和虚部(epsilon',epsilon”)和电模量(Mf和M”),损耗角正切(tanδ)和交流电导率(使用室温下的电容(C)和电导(G / co)数据,可以在很宽的频率和电压范围内获得Al / Co3O4-PVA / p-Si结构的σ(ac)值。发现对于每个施加的偏置电压,ε值,ε值和tanδ值都随频率的增加而减小,但是由于表面状态下的电荷及其电荷,这些参数的变化在低频下的耗尽区更有效。弛豫时间和极化效应。虽然sigma的值在低频下几乎恒定,但在高频下几乎成倍增加,分别对应于sigma(dc)和sigma(ac)。 M'和M''在低频区域具有较低的值,然后由于电荷载流子的短程迁移率而随频率增加。虽然M''的值随频率增加而增加,但M''的值显示两个峰值,并且由于极化的减小和N-ss效应随频率的增加,随着施加电压的增加,峰值位置移至较高的频率。 (C)2016 Elsevier B.V.保留所有权利。

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