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Optical binding between polar particles

机译:极性颗粒之间的光学绑定

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Optical binding is a phenomenon that is exhibited by micro-and nano-particulate systems, suitably irradiated with offresonance laser light. Recent quantum electrodynamical studies have shown that the optomechanical effect owes its origin to a radiative intervention with the Casimir-Polder dispersion force. The potential energy surfaces for optically induced inter-particle coupling reveal unexpected features of considerable intricacy, and when several particles are present, the effect can result in the formation of geometrically varied non-contact assemblies. In general, previous studies have been restricted to considering only the dynamic electromagnetic coupling between particles, where the latter are considered to be non-polar and centrosymmetric. However, when optical binding between non-polar particles takes place, other forms of interaction need to be entertained – more especially so, since any presence of a permanent dipole moment necessarily also admits a non-zero hyperpolarizability. Consequently, amongst the static contributions to the interaction between any pair of particles, a coupling between the electric dipole of one and the hyperpolarizability of the other must also be considered. In this paper we study these static contributions to the overall optical binding, comparing their effect with other inter-particle interactions, particularly the prominent electric dipole-dipole coupling. The results suggest that static coupling between polar particles can significantly modify the observed optical binding.
机译:光学绑定是通过微颗粒系统表现出的现象,其适当地用偏心激光照射。最近的量子电动研究表明,光学力学效应归因于具有Casimir-Bolder色散力的辐射干预。用于光学诱导的颗粒偶联的潜在能量表面揭示了相当杂色的意外特征,并且当存在几个颗粒时,效果可以导致几何变化的非接触组件的形成。通常,以前的研究仅限于仅考虑颗粒之间的动态电磁耦合,后者被认为是非极性和亚里索的。然而,当发生非极性颗粒之间的光学结合时,需要娱乐其他形式的相互作用 - 更尤其是因此,由于任何永久偶极矩的存在必然也承认了非零超极化性。因此,在任何一对颗粒之间的相互作用的静态贡献中,也必须考虑在另一对颗粒之间的偶极子之间的耦合和另一对的偶极性。在本文中,我们将这些静态贡献研究了整体光学结合,比较了它们与其他颗粒间相互作用的影响,特别是突出的电偶极偶极偶联。结果表明,极性颗粒之间的静态耦合可以显着改变观察到的光学结合。

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