Electric field influenced alignment of symmetrical lamellar diblock copolymers confined within polar discs.

Usama Gulzar, Inayatullah Soomro, Muhammad Javed Iqbal
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Abstract

Controlling the self-assembly of nanoscale morphologies by applying a surface field to diblock copolymers leads to potential applications in optics, sensors, nanolithography templates, and high-density media. In this paper, we predict the alignment behaviour of symmetric diblock copolymers confined in annular discs in response to an applied electric field. Investigations have focused on new trends in lamellar patterning that are influenced by variations in microphase separation, electric field strength, pore size, and disc inner radius. The cell dynamics simulation model is a discrete version of the time-dependent Ginzburg-Landau (Cahn-Hilliard-Cook) equation that captures the dynamic evolution of novel morphologies in curves, expressed in polar coordinates. The competition between electric-field-driven ordering and geometric confinement offers insight into controlling alignment in coherent lamellar morphology under local confinement. It is demonstrated that under confined domains, the electric field aligns the lamellar patterns into concentric and radial orientations associated with confinement domains. The competition between electric-field-driven ordering and geometric confinement provides insight into controlling alignment in coherent lamellar morphology under local confinement. The weak electric field is insufficient to overcome the frustration caused by thermal fluctuations and curvature. Excessively strong electric fields also drive the system into kinetically trapped metastable states with persistent defects. An intermediate electric field strength provides an optimal balance between defect relaxation and electrostatic driving, resulting in a defect-free, aligned lamellar morphology.

电场影响极性圆盘内对称层状二嵌段共聚物的排列。
通过在二嵌段共聚物熔体中使用表面场来控制自组装,可以操纵纳米尺度的形貌,在光学、传感器、纳米光刻模板和高密度介质中具有潜在的应用前景。在本文中,控制是通过预测取向行为使用电场施加到对称双嵌段共聚物熔体限制在环形圆盘。研究的重点是微相分离产生的层状图案的新方向,受电场强度、孔径和圆盘内部半径的变化的影响。细胞动力学模拟模型是时间相关的Ginzburg-Landau (Cahn-Hilliard-Cook)方程的离散版本,该方程使用极坐标系统捕获曲线域中新形态的动态演变。证明了片层诱导的电场取向,具有约束域和依赖于电场强度的同心圆取向和径向取向之间的过渡机制。电场驱动有序和几何约束之间的竞争为空间约束下相干片层形貌的取向控制提供了新的思路。观测表明,弱电场不足以克服由热波动和曲率引起的挫折。此外,过强的电场会诱导具有持续缺陷的亚稳态动力学陷阱系统。缺陷松弛和静电驱动之间的最佳平衡由中等电场强度提供,从而产生无缺陷,排列的片层形态。
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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