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Dipolar interactions and constant dielectric loss spectra

机译:偶极相互作用和恒定介电损耗谱

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Frequency-independent dielectric loss spectra constitute an ubiquitous phenomenon in strongly disordered materials. The degree of universality of this effect calls for a microscopic model that takes into account interactions and structural disorder, but otherwise requires only minimal assumptions. Under this point of view we review and further investigate the cooperative relaxation behaviour in an assembly of defect centres at frozen random positions. These centres carry an internal dipolar degree of freedom and interact by dipole-dipole forces. Such a description essentially amounts to studying the cooperative dynamics of interacting "asymmetric double well potential" (ADWP)-like centres, without invoking an ad hoc barrier distribution. Kinetic Monte Carlo simulations of an associated random dipolar lattice model show a transition from Debye to constant dielectric loss behaviour upon lowering the temperature. These results are interpreted with the help of analytic theories that focus on slow relaxation within strongly interacting nearest neighbour pairs of defects. Finally, a collective mode representation of the dielectric response derived from stochastic field theory is presented.
机译:与频率无关的介电损耗谱在强烈无序的材料中普遍存在。这种效应的普遍程度要求建立一个微观模型,该模型考虑到相互作用和结构紊乱,但在其他方面仅需极少的假设。根据这种观点,我们回顾并进一步研究了在冻结的随机位置处的缺陷中心集合中的协同松弛行为。这些中心具有内部偶极自由度,并通过偶极-偶极力相互作用。这样的描述实质上等于研究相互作用的“非对称双阱势能”(ADWP)样中心的合作动力学,而无需调用临时的障碍物分布。相关的随机偶极子晶格模型的动力学蒙特卡洛模拟显示,降低温度后,从德拜转变为恒定的介电损耗行为。这些结果借助分析理论来解释,这些理论关注于在相互作用强烈的最近邻缺陷对中的缓慢弛豫。最后,提出了由随机场理论导出的介电响应的集体模式表示。

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