Macdonald J Ross
Department of Physics and Astronomy, University of North Carolina, Chapel Hill, North Carolina 27599-3255, USA.
J Phys Chem B. 2007 Jun 28;111(25):7064-72. doi: 10.1021/jp068470o. Epub 2007 May 27.
Ion dynamics effects and the resulting dispersed frequency response of conducting materials have often been explained in the past by a combination of the Moynihan original modulus formalism (OMF) and the Ngai coupling model (NCM). These incorrect approaches and their inappropriate conclusions are replaced by alternate, Kohlrausch-related physically reasonable conductive-system fitting and interpretation models that are then used for the analysis of both limited-range and wide-range data for the supercooled liquid 0.4Ca(NO3)2*0.6KNO3 (CKN). Detailed analysis of the limited-range 342 K data at the electric modulus immittance level shows that OMF fitting leads to an excess wing and that more appropriate models fit the data well without such a wing. Further, although such models allow estimation of the bulk dipolar dielectric constant of the material, as well as one associated only with mobile charges, they lead to implausibly small estimates of the important Kohlrausch K1 model shape parameter, beta1, and lead to an inadequate determination of its characteristic relaxation time. Therefore, wide-range CKN data sets extending to nearly 1012 Hz for the temperatures 342, 350, 356, and 361 K were very well-fitted with a more detailed composite model but one still involving K1 response. All model parameters were well-determined with no excess wings; beta1 estimates were all much closer to the universal value of 1/3; and the estimated model parameters led to a Boson peak beyond 1012 Hz, to very large thermal activation energies, and to evidence that the mobile charge concentration reached a saturation value at about 356 K. Such results do not support assumptions about variable ion-ion correlation, a mainstay of the OMF and NCM approaches. Finally, it is shown that although excess wings can sometimes be eliminated by using just an appropriate bulk fitting model and series blocking-electrode capacitor, as shown for the present narrow-range data, adequate fitting of the present wide-range data sets over their full spans of as much as 13 decades required the addition of an additional series dispersive-response model to the composite model. This addition seems likely to be required to take adequate account of the presence of more than one species of mobile charge in CKN.
过去,离子动力学效应以及导电材料由此产生的分散频率响应常常通过莫伊尼汉原始模量形式理论(OMF)和恩盖耦合模型(NCM)的组合来解释。这些错误的方法及其不恰当的结论已被与科尔劳施相关的、物理上合理的导电系统拟合和解释模型所取代,这些模型随后被用于分析过冷液体0.4Ca(NO₃)₂·0.6KNO₃(CKN)的有限范围和宽范围数据。在电模量导纳水平下对342K的有限范围数据进行的详细分析表明,OMF拟合会导致出现多余的边带,而更合适的模型能很好地拟合数据且不会出现这样的边带。此外,尽管这些模型能够估算材料的体偶极介电常数以及仅与移动电荷相关的介电常数,但它们得出的重要科尔劳施K1模型形状参数β₁的估计值小得难以置信,并且对其特征弛豫时间的确定也不充分。因此,对于342、350、356和361K温度下延伸至近10¹²Hz的宽范围CKN数据集,用一个更详细的复合模型能很好地拟合,但该模型仍涉及K1响应。所有模型参数都能很好地确定,没有多余的边带;β₁的估计值都更接近通用值1/3;估计的模型参数导致在10¹²Hz以上出现玻色子峰,得到非常大的热激活能,并证明移动电荷浓度在约356K时达到饱和值。这些结果不支持关于可变离子 - 离子相关性的假设,而这是OMF和NCM方法的主要依据。最后表明,尽管有时仅通过使用合适的体拟合模型和串联阻挡电极电容器就可以消除多余的边带,如本窄范围数据所示,但要对目前宽范围数据集在高达13个数量级的整个跨度上进行充分拟合,需要在复合模型中添加一个额外的串联色散响应模型。这种添加似乎是必要的,以便充分考虑CKN中存在不止一种移动电荷的情况。