Sakai Kyosuke, Nomura Kensuke, Yamamoto Takeaki, Sasaki Keiji
Research Institute for Electronic Science, Hokkaido University, Sapporo, Hokkaido, 001-0020 JAPAN.
Sci Rep. 2015 Feb 12;5:8431. doi: 10.1038/srep08431.
Localized surface plasmon resonance (LSPR) has been shown to exhibit a strong potential for nanoscale electromagnetic field manipulation beyond the diffraction limit. Particularly dark mode plasmons circumvent radiation loss and store the energy long in time, which raise the prospect of interesting plasmonics applications, for example biochemical sensing and nanoscale lasing. Here we theoretically investigate a method of exciting multipole plasmons, including dark modes, using normally incident light. By performing numerical calculations, we show that multipole plasmons in metal nanodisks can be selectively excited by circularly-polarized optical vortex beams. We study the electromagnetic fields of the beam cross-sections and their correspondence with the excited multipole plasmon modes with respect to spin and orbital angular momenta. The transfer of angular momentum between photons and plasmons is also discussed.
局域表面等离子体共振(LSPR)已被证明在超越衍射极限的纳米级电磁场操纵方面具有强大潜力。特别是暗模等离子体可避免辐射损耗并长时间存储能量,这为诸如生化传感和纳米级激光等有趣的等离子体应用带来了前景。在此,我们从理论上研究了一种使用正入射光激发包括暗模在内的多极等离子体的方法。通过进行数值计算,我们表明金属纳米盘中的多极等离子体可被圆偏振光学涡旋光束选择性激发。我们研究了光束横截面的电磁场及其与激发的多极等离子体模式在自旋和轨道角动量方面的对应关系。还讨论了光子与等离子体之间的角动量转移。