Department of Chemistry, University of Toronto , Toronto, Ontario M5S 3H6, Canada.
ACS Nano. 2014 Nov 25;8(11):11305-12. doi: 10.1021/nn504093g. Epub 2014 Nov 3.
Boron nitride (BN) is considered to be a promising substrate for graphene-based devices in part because its large band gap can serve to insulate graphene in layered heterostructures. At mid-infrared frequencies, graphene supports surface plasmon polaritons (SPPs), whereas hexagonal-BN (h-BN) is found to support surface phonon polaritons (SPhPs). We report on the observation of infrared polaritonic coupling between graphene SPPs and boron nitride nanotube (BNNT) SPhPs. Infrared scattering type scanning near-field optical microscopy is used to obtain spatial distribution of the two types of polaritons at the nanoscale. The observation suggests that those polaritons interact at the nanoscale in a one-dimensional/two-dimensional (1D/2D) geometry, exchanging energy in a nonplanar configuration at the nanoscale. Control of the polaritonic interaction is achieved by adjustment of the graphene Fermi level through voltage gating. Our observation suggests that boron nitride nanotubes and graphene can interact at mid-infrared frequencies and coherently exchange their energies at the nanoscale through the overlap of mutual electric near field of surface phonon polaritons and surface plasmon polaritons. Such interaction enables the design of nano-optical devices based on BNNT-graphene polaritonics in the mid-infrared range.
氮化硼(BN)被认为是一种有前途的基于石墨烯器件的衬底,部分原因是其较大的带隙可以在层状异质结构中隔离石墨烯。在中红外频率下,石墨烯支持表面等离激元(SPP),而六方氮化硼(h-BN)则支持表面声子极化激元(SPhP)。我们报告了在石墨烯 SPP 和硼氮纳米管(BNNT) SPhP 之间观察到的红外极化激元耦合。红外散射型扫描近场光学显微镜用于在纳米尺度上获得两种极化激元的空间分布。观察表明,这些极化激元在一维/二维(1D/2D)几何形状中在纳米尺度上相互作用,在纳米尺度上以非平面配置交换能量。通过栅极电压调节石墨烯费米能级来控制极化激元相互作用。我们的观察表明,在中红外频率下,硼氮纳米管和石墨烯可以相互作用,并通过表面声子极化激元和表面等离激元的相互电近场的重叠,在纳米尺度上相干地交换能量。这种相互作用使得能够设计基于 BNNT-石墨烯极化激元的中红外范围内的纳米光学器件。