Interacting dipole charges in non-linear dielectrics: a Monte Carlo simulation

H. Kliem, N. Farag
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Abstract

Numerical calculations of the electrostatic dipole-dipole interaction and the resulting effects on the dielectric polarization are performed. Dipoles of finite length, which are randomly distributed in space, decrease the polarization of the whole dipole system due to their interaction. Dipoles on cubic lattice sites increase the polarization due to the interaction, as predicted by the Lorentz model. When the dipoles are shifted from their regular sites, the polarization decreases with the degree of disorder. If the length of lattice dipoles is increased, the interaction decreases the polarization too. Both lattice and disordered dipole systems exhibit hysteresis loops of their polarization. The remanent polarization of lattice dipoles drops sharply and for disordered dipoles it drops smoothly with temperature. The interaction results in distribution of activation energies for the dipoles.
非线性介质中相互作用的偶极子电荷:蒙特卡罗模拟
对静电偶极-偶极相互作用及其对介质极化的影响进行了数值计算。有限长度的偶极子在空间上随机分布,它们之间的相互作用降低了整个偶极子系统的极化。正如洛伦兹模型所预测的那样,立方点阵上的偶极子由于相互作用而增加了极化。当偶极子从其规则位置移动时,极化随无序程度而减小。如果晶格偶极子的长度增加,相互作用也会降低极化。晶格和无序偶极子系统都表现出极化的滞后回路。晶格偶极子的剩余极化随温度的升高而急剧下降,无序偶极子的剩余极化随温度的升高而平稳下降。这种相互作用导致了偶极子的活化能分布。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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