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Elastic colloidal monopoles and reconfigurable self-assembly in liquid crystals

机译:弹性胶体单极子和液晶中可重构的自组装

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摘要

Monopole-like electrostatic interactions are ubiquitous in biology(1) and condensed matter(2-4), but they are often screened by counter-ions and cannot be switched from attractive to repulsive. In colloidal science, where the main goal is to develop colloidal particles(2,3) that mimic and exceed the diversity and length scales of atomic and molecular assembly, electrostatically charged particles cannot change the sign of their surface charge or transform from monopoles to higher-order multipoles(4). In liquid-crystal colloids(5-7), elastic interactions between particles arise to minimize the free energy associated with elastic distortions in the long-range alignment of rod-like molecules around the particles(5). In dipolar(6,8), quadrupolar(8-12) and hexadecapolar(13) nematic colloids, the symmetries of such elastic distortions mimic both electrostatic multipoles(14) and the outermost occupied electron shells of atoms(7,15,16). Electric and magnetic switching(17,18), spontaneous transformations(19) and optical control(20) of elastic multipoles, as well as their interactions with topological defects and surface boundary conditions, have been demonstrated in such colloids(21-23). However, it has long been understood(5,24) that elastic monopoles should relax to uniform or higher-order multipole states because of the elastic torques that they induce(5,7). Here we develop nematic colloids with strong elastic monopole moments and with elastic torques balanced by the optical torques induced by ambient light. We demonstrate the monopole-to-quadrupole reconfiguration of these colloidal particles by unstructured light, which resembles the driving of atoms between the ground state and various excited states. We show that the sign of the elastic monopoles can be switched, and that like-charged monopoles attract whereas oppositely charged ones repel, unlike in electrostatics(14). We also demonstrate the out-of-equilibrium dynamic assembly of these colloidal particles. This diverse and surprising behaviour is explained using a model that considers the balance of the optical and elastic torques that are responsible for the excited-state elastic monopoles and may lead to light-powered active-matter systems and self-assembled nanomachines.
机译:单极类静电相互作用在生物学(1)和凝聚态物质(2-4)中是普遍存在的,但是它们经常被抗衡离子筛选,因此不能从吸引转变为排斥。在胶体科学中,主要目标是开发能模仿并超过原子和分子组装的多样性和长度尺度的胶体颗粒(2,3),带静电的颗粒不能改变其表面电荷的符号或从单极转变为更高的极性阶多极(4)。在液晶胶体(5-7)中,粒子之间发生弹性相互作用,以使与棒状分子在粒子周围的长距离排列中的弹性变形相关的自由能最小化(5)。在偶极(6,8),四极(8-12)和十六极(13)的向列胶体中,这种弹性变形的对称性模仿了静电多极(14)和原子的最外层电子壳(7,15,16) 。在这种胶体中已证明了弹性多极的电磁开关(17,18),自发变换(19)和光学控制(20),以及它们与拓扑缺陷和表面边界条件的相互作用(21-23)。但是,人们早就知道(5,24),因为弹性单极会产生弹性转矩(5,7),所以它们应松弛到均匀或更高阶的多极态。在这里,我们开发出具有强弹性单极矩且弹性转矩与环境光感应的光学转矩平衡的向列胶体。我们通过非结构化的光证明了这些胶体粒子的单极到四极重组,这类似于原子在基态和各种激发态之间的驱动。我们证明了弹性单极子的符号可以切换,并且带电荷的单极子会吸引而带相反电荷的单极子会排斥,这与静电学不同(14)。我们还演示了这些胶体粒子的平衡外动态组装。使用考虑了引起激发态弹性单极子的光学和弹性扭矩之间的平衡的模型来解释这种多样且令人惊讶的行为,并且可能导致光动力的主动物质系统和自组装纳米机器。

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  • 来源
    《Nature 》 |2019年第7760期| 214-218| 共5页
  • 作者单位

    Univ Colorado, Dept Phys, Boulder, CO 80309 USA;

    Univ Colorado, Dept Phys, Boulder, CO 80309 USA;

    Univ Colorado, Dept Phys, Boulder, CO 80309 USA;

    Univ Colorado, Dept Phys, Boulder, CO 80309 USA|Univ Colorado, Dept Elect Comp & Energy Engn, Boulder, CO 80309 USA|Univ Colorado, Soft Mat Res Ctr, Boulder, CO 80309 USA|Natl Renewable Energy Lab, Renewable & Sustainable Energy Inst, Boulder, CO 80309 USA|Univ Colorado, Boulder, CO 80309 USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
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  • 正文语种 eng
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