IBM T. J. Watson Research Center, Yorktown Heights, New York 10598, United States.
Nano Lett. 2012 Jul 11;12(7):3766-71. doi: 10.1021/nl3016335. Epub 2012 Jun 13.
We present infrared spectroscopy study of plasmon excitations in graphene in high magnetic fields. The plasmon resonance in patterned graphene disks splits into edge and bulk plasmon modes in magnetic fields. Remarkably, the edge plasmons develop increasingly longer lifetimes in high fields due to the suppression of backscattering. Moreover, due to the linear band structure of graphene, the splitting of the edge and bulk plasmon modes develops a strong doping dependence, which differs from the behavior of conventional semiconductor two-dimensional electron gas (2DEG) systems. We also observe the appearance of a higher order mode indicating an anharmonic confinement potential even in these well-defined circular disks. Our work not only opens an avenue for the investigation of the properties of Dirac magnetoplasmons but also supports the great potential of graphene for tunable terahertz magneto-optical devices.
我们呈现了在高磁场中石墨烯等离子体激元激发的红外光谱研究。在磁场中,图案化石墨烯盘中的等离子体共振分裂为边缘和体等离子体模式。值得注意的是,由于背散射的抑制,边缘等离子体在高场中表现出越来越长的寿命。此外,由于石墨烯的线性能带结构,边缘和体等离子体模式的分裂表现出强烈的掺杂依赖性,这与传统半导体二维电子气(2DEG)系统的行为不同。我们还观察到高阶模式的出现,这表明即使在这些定义良好的圆形盘中,也存在非谐约束势。我们的工作不仅为研究狄拉克磁等离子体激元的性质开辟了道路,而且还支持了石墨烯在可调谐太赫兹磁光器件中的巨大潜力。