Optimizing plasmonic resonance properties in the near-IR

D. Look
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Abstract

Surface plasmon polaritons (SPPs) are electromagnetic waves that arise when a plasmon wave1–5 (i.e., a coordinated swarm of electrons) interacts strongly with a light wave of a similar frequency (!), and together they are confined to, and propagate along, an air/metal interface. SPPs are of substantial interest because it is possible to control and modify them with the use of normal circuit elements, to allow the SPP to be ejected as pure light. In addition, the dimensions of SPPs are much smaller in metals than in air, and so the usual diffraction limit of light in air does not apply. The confinement property of SPPs—which can lead to intense electric fields and enhanced light emission—is thus exploited in a number of applications, including surfaceenhanced Raman spectroscopy (which has a higher resolution than standard Raman spectroscopy). The metals that are generally used in plasmonic applications (gold and silver), however, are not ideal for all energy ranges. Although these materials have high electron concentration (n) values (mid1022cm 3), and work well in the UV (3–12eV) and visible (1.5– 3eV) ranges (because !p n1=2), they experience heavy losses in the near-IR region (0.5–1.5eV). This is because the loss is proportional to n/! (where is electron mobility), and the high value of n cannot be avoided. In response to this problem, it has previously been proposed1–3 that highly doped semiconductors, with smaller n values, may be better plasmonic materials (than the standard gold and silver) in the near-IR (NIR) region. Fortunately— mainly because of the need for transparent electrodes in LEDs, display circuits, and solar cells—the field of highly doped semiconductors is well developed.6 However, the goal in transparent electrode design is generally to have the highest possible n, whereas in plasmonic applications, it is to have the lowest possible n, but that is still high enough to produce the desired resonance wavelength ( res). The best possible material is thereFigure 1. Experimentally measured plasmonic resonant wavelength ( res) of gallium-doped zinc oxide (GZO) as a function of annealing temperature (TA).
优化近红外等离子体共振特性
表面等离子激元极化子(SPPs)是一种电磁波,当等离子激元波1 - 5(即一群协调的电子)与频率相似的光波(!)强烈相互作用时产生,它们一起被限制在空气/金属界面上,并沿着该界面传播。SPP非常重要,因为可以使用普通电路元件来控制和修改它们,以允许SPP以纯光的形式发射。此外,spp在金属中的尺寸比在空气中的小得多,因此通常的光在空气中的衍射极限不适用。spps的约束特性——可能导致强电场和增强的光发射——因此在许多应用中得到了利用,包括表面增强拉曼光谱(比标准拉曼光谱具有更高的分辨率)。然而,通常用于等离子体应用的金属(金和银)并非适用于所有能量范围。虽然这些材料具有很高的电子浓度(n)值(中间1022cm 3),并且在UV (3 - 12ev)和可见光(1.5 - 3eV)范围内工作良好(因为!p n1=2),但它们在近红外区域(0.5-1.5eV)遭受严重损失。这是因为损耗正比于n/!(其中为电子迁移率),且n的高值不可避免。为了解决这个问题,之前有人提出1 - 3,在近红外(NIR)区域,具有较小n值的高掺杂半导体可能是更好的等离子体材料(比标准金和银)。幸运的是——主要是因为led、显示电路和太阳能电池对透明电极的需要——高掺杂半导体领域得到了很好的发展然而,透明电极设计的目标通常是具有尽可能高的n,而在等离子体应用中,它是具有尽可能低的n,但仍然足够高以产生所需的共振波长(res)。最好的材料就在那里。实验测量了掺镓氧化锌(GZO)等离子体共振波长(res)随退火温度(TA)的变化规律。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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