NTT Basic Research Laboratories, NTT Corporation, 3-1 Morinosato-Wakamiya, Atsugi, Kanagawa 243-0198, Japan.
Nat Commun. 2013;4:1363. doi: 10.1038/ncomms2353.
Plasmons, which are collective charge oscillations, could provide a means of confining electromagnetic field to nanoscale structures. Recently, plasmonics using graphene have attracted interest, particularly because of the tunable plasmon dispersion, which will be useful for tunable frequency in cavity applications. However, the carrier density dependence of the dispersion is weak (proportional to n(1/4)) and it is difficult to tune the frequency over orders of magnitude. Here, by exploiting electronic excitation and detection, we carry out time-resolved measurements of a charge pulse travelling in a plasmon mode in graphene corresponding to the gigahertz range. We demonstrate that the plasmon velocity can be changed over two orders of magnitude by applying a magnetic field B and by screening the plasmon electric field with a gate metal; at high B, edge magnetoplasmons, which are plasmons localized at the sample edge, are formed and their velocity depends on B, n and the gate screening effect.
等离子体激元是一种集体电荷振荡,可以将电磁场限制在纳米结构中。最近,利用石墨烯的等离子体激元引起了人们的兴趣,特别是因为其等离子体激元色散是可调谐的,这对于腔应用中的可调谐频率很有用。然而,色散对载流子密度的依赖性较弱(与 n(1/4)成正比),并且很难在数量级上调节频率。在这里,我们通过利用电子激发和探测,对在石墨烯中的等离子体模式中传播的电荷脉冲进行了太赫兹范围内的时间分辨测量。我们证明,通过施加磁场 B 和用栅极金属屏蔽等离子体电场,可以将等离子体速度改变两个数量级;在高 B 下,形成了局域在样品边缘的边缘磁等离子体激元,其速度取决于 B、n 和栅极屏蔽效应。