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在液体界面处的磁性圆柱胶体在外场中表现出其取向的非易失性切换。

Magnetic cylindrical colloids at liquid interfaces exhibit non-volatile switching of their orientation in an external field.

机构信息

Theory of Condensed Matter Group, Department of Physics and Mathematics, University of Hull, Hull, HU6 7RX, UK.

出版信息

Soft Matter. 2016 Jun 28;12(24):5285-96. doi: 10.1039/c6sm00136j. Epub 2016 May 20.

Abstract

We study the orientation of magnetic cylindrical particles adsorbed at a liquid interface in an external field using analytical theory and high resolution finite element simulations. Cylindrical particles are interesting since they possess multiple locally stable orientations at the liquid interface so that the orientational transitions induced by an external field will not disappear when the external field is removed, i.e., the switching effect is non-volatile. We show that, in the absence of an external field, as we reduce the aspect ratio α of the cylinders below a critical value (αc≈ 2) the particles undergo spontaneous symmetry breaking from a stable side-on state to one of two equivalent stable tilted states, similar to the spontaneous magnetisation of a ferromagnet going through the Curie point. By tuning both the aspect ratio and contact angle of the cylinders, we show that it is possible to engineer particles that have one, two, three or four locally stable orientations. We also find that the magnetic responses of cylinders with one or two stable states are similar to that of paramagnets and ferromagnets respectively, while the magnetic response of systems with three or four stable states are even more complex and have no analogs in simple magnetic systems. Magnetic cylinders at liquid interfaces therefore provide a facile method for creating switchable functional monolayers where we can use an external field to induce multiple non-volatile changes in particle orientation and self-assembled structure.

摘要

我们使用解析理论和高分辨率有限元模拟研究了在外部磁场中吸附在液体界面上的磁性圆柱粒子的取向。圆柱粒子很有趣,因为它们在液体界面上具有多个局部稳定的取向,因此当外部磁场移除时,由外部磁场引起的取向转变不会消失,即切换效应是非易失性的。我们表明,在没有外部磁场的情况下,随着圆柱的纵横比α降低到一个临界值(αc≈2)以下,粒子会从稳定的侧对状态自发地经历对称破缺,转变为两种等效稳定的倾斜状态之一,类似于铁磁体的自发磁化通过居里点。通过调整圆柱的纵横比和接触角,我们表明可以设计出具有一个、两个、三个或四个局部稳定取向的粒子。我们还发现,具有一个或两个稳定状态的圆柱的磁响应分别类似于顺磁体和铁磁体,而具有三个或四个稳定状态的系统的磁响应则更加复杂,在简单的磁系统中没有类似的响应。因此,液体界面上的磁性圆柱为创建可切换的功能单层提供了一种简便的方法,我们可以使用外部磁场来诱导粒子取向和自组装结构的多次非易失性变化。

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