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Plasmonic Laser Antennas and Related Devices

机译:等离子激光天线及相关设备

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This paper reviews recent work on device applications of optical antennas. Localized surface plasmon resonances of gold nanorod antennas resting on a silica glass substrate were modeled by finite difference time-domain simulations. A single gold nanorod of length 150 or 550 nm resonantly generates enhanced near fields when illuminated with light of 830 nm wavelength. A pair of these nanorods gives higher field enhancements due to capacitive coupling between them. Bowtie antennas that consist of a pair of triangular gold particles offer the best near-field confinement and enhancement. Plasmonic laser antennas based on the coupled nanorod antenna design were fabricated by focused ion beam lithography on the facet of a semiconductor laser diode operating at a wavelength of 830 nm. An optical spot size of few tens of nanometers was measured by apertureless near-field optical microscope. We have extended our work on plasmonic antenna into mid-infrared (mid-IR) wavelengths by implementing resonant nanorod and bowtie antennas on the facets of various quantum cascade lasers. Experiments show that this mid-IR device can provide an optical intensity confinement 70 times higher than that would be achieved with diffraction limited optics. Near-field intensities $sim$$1;{rm GW/cm}^2$ were estimated for both near-infrared and mid-IR plasmonic antennas. A fiber device that takes advantage of plasmonic resonances of gold nanorod arrays providing a high density of optical “hot spots” is proposed. Results of a systematic theoretical and experimental study of the reflection spectra of these arrays fabricated on a silica glass substrate are also presented. The family of these proof-of-concept plasmonic devices that we present here can be potentially useful in many applications including near-field optical microscopes, high-density optical data storage, surface enhanced Raman spectroscopy, heat-assisted magneti-n-nc recording, and spatially resolved absorption spectroscopy.
机译:本文回顾了有关光学天线设备应用的最新工作。通过时域有限差分模拟对金纳米棒天线放置在石英玻璃基板上的局部表面等离子体共振进行建模。当用830 nm波长的光照射时,长度为150或550 nm的单个金纳米棒共振产生增强的近场。一对这些纳米棒由于它们之间的电容耦合而具有更高的场增强。由一对三角形金颗粒组成的领结天线可提供最佳的近场限制和增强效果。通过聚焦离子束光刻在工作于830 nm波长的半导体激光二极管的端面上,制造了基于耦合纳米棒天线设计的等离子激光天线。通过无孔近场光学显微镜测量了几十纳米的光斑尺寸。通过在各种量子级联激光器的各个面上实现谐振纳米棒和领结天线,我们将等离子天线的工作扩展到了中红外(mid-IR)波长。实验表明,这种中红外设备可提供的光强度限制比衍射受限的光学器件要高70倍。估计了近红外和中红外等离激元天线的近场强度$ sim $$ 1; {rm GW / cm} ^ 2 $。提出了利用金纳米棒阵列的等离子体共振提供高密度的光学“热点”的光纤装置。还介绍了在石英玻璃基板上制造的这些阵列的反射光谱的系统理论和实验研究的结果。我们在此展示的这些概念验证的等离激元设备系列可能在许多应用中潜在地有用,包括近场光学显微镜,高密度光学数据存储,表面增强拉曼光谱,热辅助磁-n-nc记录,以及空间分辨吸收光谱。

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