用于下一代光学和传感技术的量子等离子体

M. Moaied, K. Ostrikov
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引用次数: 2

摘要

经典等离子体动力学研究主要集中在大尺寸结构上,量子力学效应对这些结构几乎没有影响。然而,最近的技术进步,特别是在纳米尺度的小型化等离子体器件上,使得想象等离子体的实验应用成为可能,其中自由电荷载流子的量子性质起着重要作用。因此,有必要利用量子力学来模拟固体等离子体纳米结构中载流子的输运。本文应用固态等离子体动力学理论中带有碰撞项的Wigner方程,建立了以电子-晶格碰撞为主要电子散射机制的介电常数非局域量子模型。利用这种非局域量子介电常数研究了超小纳米粒子的表面等离子体共振,得到了其色散关系。预计该理论将成功应用于超小型等离子体结构,如表面等离子体极化子波导、掺杂半导体、石墨烯、由金属和介电层交替组成的超材料以及量子液滴。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum plasmonics for next-generation optical and sensing technologies
Classical plasmonics has mostly focused on structures characterized by large dimension, for which the quantummechanical effects have nearly no impact. However, recent advances in technology, especially on miniaturized plasmonics devices at nanoscale, have made it possible to imagine experimental applications of plasmons where the quantum nature of free charge carriers play an important role. Therefore, it is necessary to use quantum mechanics to model the transport of charge carriers in solid state plasma nanostructures. Here, a non-local quantum model of permittivity is presented by applying the Wigner equation with collision term in the kinetic theory of solid state plasmas where the dominant electron scattering mechanism is the electron-lattice collisions. The surface plasmon resonance of ultra-small nanoparticles is investigated using this non-local quantum permittivity and its dispersion relation is obtained. The successful application of this theory in ultra-small plasmonics structures such as surface plasmon polariton waveguides, doped semiconductors, graphene, the metamaterials composed of alternating layers of metal and dielectric, and the quantum droplets is anticipated.
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