首页> 外文OA文献 >Ferroelectric domain formation in discotic liquid crystals : Monte Carlo study on the influence of boundary conditions
【2h】

Ferroelectric domain formation in discotic liquid crystals : Monte Carlo study on the influence of boundary conditions

机译:盘状液晶中的铁电畴形成:蒙特卡罗   研究边界条件的影响

代理获取
本网站仅为用户提供外文OA文献查询和代理获取服务,本网站没有原文。下单后我们将采用程序或人工为您竭诚获取高质量的原文,但由于OA文献来源多样且变更频繁,仍可能出现获取不到、文献不完整或与标题不符等情况,如果获取不到我们将提供退款服务。请知悉。

摘要

The realization of a spontaneous macroscopic ferroelectric order in fluids ofanisotropic mesogens is a topic of both fundamental and technological interest.Recently, we demonstrated that a system of dipolar achiral disklike ellipsoidscan exhibit long-searched ferroelectric liquid crystalline phases of dipolarorigin. In the present work, extensive off-lattice Monte Carlo simulations areused to investigate the phase behavior of the system under the influences ofthe electrostatic boundary conditions that restrict any global polarization. Wefind that the system develops strongly ferroelectric slablike domainsperiodically arranged in an antiferroelectric fashion. Exploring the phasebehavior at different dipole strengths, we find existence of the ferroelectricnematic and ferroelectric columnar order inside the domains. For higher dipolestrengths, a biaxial phase is also obtained with a similar periodic array offerroelectric slabs of antiparallel polarizations. We have studied thedepolarizing effects by using both the Ewald summation and the sphericalcut-off techniques. We present and compare the results of the two differentapproaches of considering the depolarizing effects in this anisotropic system.It is explicitly shown that the domain size increases with the system size as aresult of considering longer range of dipolar interactions. The system exhibitspronounced system size effects for stronger dipolar interactions. The resultsprovide strong evidence to the novel understanding that the dipolarinteractions are indeed sufficient to produce long range ferroelectric order inanisotropic fluids.
机译:在各向异性介晶流体中实现自发的宏观铁电有序是一个基础性和技术性的课题。最近,我们证明了偶极非手性盘状椭球体的体系具有长期研究的偶极性铁电液晶相。在当前的工作中,广泛的非晶格蒙特卡洛模拟被用来研究在限制任何整体极化的静电边界条件的影响下系统的相位行为。我们发现系统以反铁电方式周期性地形成强铁电平板状磁畴。探索不同偶极强度下的相行为,我们发现在域内存在铁电向列和铁电柱状序。对于更高的偶极子强度,还可以使用反平行极化的类似周期阵列电子平板获得双轴相。我们已经通过使用埃瓦尔德求和和球形截止技术研究了去极化效应。我们提出并比较了考虑该各向异性系统中去极化效应的两种不同方法的结果。结果表明,考虑到更长的偶极相互作用范围,畴尺寸随系统尺寸的增加而增加。该系统具有突显出的系统尺寸效应,可实现更强的偶极相互作用。结果为新颖的理解提供了有力的证据,即偶极相互作用确实足以产生长距离铁电有序各向异性流体。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
代理获取

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号