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ANOMALOUS EXPRESSIONS FOR THE NONLINEAR HARMONIC COMPONENTS OF THE ELECTRIC POLARIZATION

机译:用于电极化非线性谐波分量的异常表达

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In view of having a better interpretation of experimental data of complex liquids which are not well described by usual Debye-like models, we propose to introduce a fractional approach applied to noninertial rotational diffusion of polar molecules. This leads to solve a fractional Smoluchowski equation (in configuration space only) characterized by an anomalous exponent a varying in the interval ]0,l] corresponding to a slow relaxation process (subdiffusion). More precisely, we consider the problem of the nonlinear dielectric response due to the application of a strong electric field in the form of either a pure ac field or a strong dc bias field superimposed on a weak ac field. For both cases, we derive in the frequency domain analytical expressions for the electric susceptibilities valid up to the third order in the field strength. This yields harmonic components varying at the fundamental angular frequency ω and in 3ω To illustrate the results so obtained for the stationary regime, dispersion and absorption spectra are plotted for each harmonic component in order to show the significant departure from the classical Brownian behavior (a= 1) as a → 0. Cole-Cole diagrams are also presented allowing one to see how the arcs become more and more flattened as a → 0, which corresponds to a broadening of the absorption peaks as effectively observed in most of complex liquids. The theoretical model is in good enough agreement compared (i) with experimental data of the third-order nonlinear susceptibility of a ferroelectric liquid crystal and (ii) data of the third-order nonlinear relative dielectric permittivity of a polymer. The present work represents an extension of previous theories in nonlinear dielectric relaxation by Coffey and Paranjape, here applied to the harmonic dielectric responses in disordered media.
机译:鉴于具有不能很好地描述通常的复杂液体的实验数据的更好的诠释的德拜状模型,我们建议引入分数的方法施加到极性分子的非惯性旋转扩散。这导致解决的分数维Smoluchowski方程(在仅配置空间),其特征在于异常指数在对应于缓慢弛豫过程(次扩散)的间隔] 0,1]一个而变化。更确切地说,我们考虑非线性介质响应的问题,由于强电场的是纯交流电场或叠加在弱交流领域的强大直流偏置场的形式应用。对于这两种情况,我们在频域推导出电动敏感性有效期至三阶场强的解析表达式。这产生高次谐波成分在基波角频率ω和在3ω变化为了说明用于固定制度,分散和吸收光谱绘制在为了显示从古典布朗行为显著离开每个谐波分量,从而所获得的结果(A = 1)也被呈现一个→0科尔 - 科尔图允许人们看到弧如何变得越来越扁平作为→0,这对应于在大多数的复杂液体有效地观察到的吸收峰的加宽。理论模型是足够好的协议(i)与所述第三阶非线性的聚合物的相对介电常数的铁电液晶和(ii)数据的三阶非线性极化率的实验数据进行比较。目前的工作表示由科菲和Paranjape非线性介电弛豫以前的理论的延伸,这里应用于无序介质的电介质谐响应。

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