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通过非对称波耦合到辐射模式和束缚模式在倏逝场中诱导产生的巨大太赫兹拉力。

Giant terahertz pulling force within an evanescent field induced by asymmetric wave coupling into radiative and bound modes.

作者信息

Ferrari Hernán, Zapata-Rodríguez Carlos J, Cuevas Mauro

出版信息

Opt Lett. 2022 Sep 1;47(17):4500-4503. doi: 10.1364/OL.460202.

Abstract

Manipulation of nano-scale objects by engineering the electromagnetic waves in the environment medium is pivotal for several particle handling techniques using optical resonators, waveguiding, and plasmonic devices. In this Letter, we theoretically demonstrate the possibility of engineering a compact and tunable plasmon-based terahertz (THz) tweezer using a graphene monolayer that is deposited on a high-index dielectric substrate. When a nanoparticle located in a vacuum in the vicinity of the graphene monolayer is illuminated under total internal reflection, as light is launched from the substrate, such a device is shown to be capable of inducing an enhanced rotating dipole in the nanoparticle thus enabling asymmetric, directional near-field coupling into the graphene plasmon mode and the radiative modes in the substrate. As a result of the total momentum conservation, the net force exerted on the particle points in a direction opposite to the pushing scattering force of the exciting evanescent field. Our results can contribute to novel realizations of photonic devices based on polarization-dependent interactions between nanoparticles and electromagnetic mode fields.

摘要

通过操控环境介质中的电磁波来操纵纳米级物体,对于使用光学谐振器、波导和等离子体器件的多种粒子处理技术至关重要。在本信函中,我们从理论上证明了利用沉积在高折射率介电衬底上的单层石墨烯设计一种紧凑且可调谐的基于等离子体的太赫兹(THz)镊子的可能性。当位于石墨烯单层附近真空中的纳米粒子在全内反射下被从衬底发射的光照射时,这种器件能够在纳米粒子中诱导增强的旋转偶极子,从而实现不对称的、定向的近场耦合进入石墨烯等离子体模式和衬底中的辐射模式。由于总动量守恒,施加在粒子上的净力指向与激发倏逝场的推散射力相反的方向。我们的结果有助于基于纳米粒子与电磁模式场之间偏振相关相互作用的光子器件的新型实现。

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