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Radiative effects in plasmonic aluminum and silver nanospheres and nanorods

机译:等离子体铝和银纳米球和纳米棒中的辐射效应

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We explore localized surface plasmon resonances in small (5-30 nm radius) aluminum and silver nanoparticles using classical electrodynamics simulations, focusing on radiative (farfield scattering) effects and the unique characteristics of aluminum as a plasmonic material. In Al spheres, higher-order plasmon resonances (e.g. quadrupoles) are significant at smaller sizes (> 15 nm) than in Ag spheres. Additionally, although the plasmon width is minimized at a radius of about 15 nm for both materials, the Al plasmon linewidth (similar to 1.4 eV) for the dipole mode is much larger than that observed in Ag (similar to 0.3 eV). The radiative contribution to damping dominates over non-radiative effects for small (5-20 nm) Al spheres (> 95%) whereas for similar size Ag spheres damping is almost entirely attributed to the bulk dielectric function (non-radiative). For Al nanorods the linewidths can be narrowed by increasing aspect ratio such that for an aspect ratio of 4.5, the overall Al (0.75 eV) linewidth is reasonably close to that of the same size Ag rod (0.35 eV). This narrowing arises from frequency dispersion in the real part of the Al dielectric function, and is associated with a 65% (1.5 to 0.5 eV) decrease in the radiative contribution to the linewidth for Al. Concurrently, an increase in the non-radiative width occurs as the aspect ratio increases and the plasmon tunes to the red. This demonstrates that anisotropy can be used as a parameter for controlling Al plasmon dephasing where the composition of the plasmon linewidth (radiative or non-radiative) can be tailored with aspect ratio. Overall, these data suggest that localized surface plasmon resonance dephasing mechanisms in Al nanostructures are inherently different from those in the noble metals, which could allow for new applications of plasmonic materials, tunable plasmon lifetimes, and new physics to be observed.
机译:我们使用经典的电动力学模拟探索在小(半径为5-30 nm)的铝和银纳米颗粒中的局部表面等离子体共振,重点是辐射(场散射)效应和铝作为等离子体材料的独特特性。在铝球中,与银球相比,较小尺寸(> 15 nm)的高阶等离振子共振(例如四极)显着。此外,尽管两种材料的等离激元宽度在半径约15 nm处均最小,但偶极子模式的Al等离激元线宽(类似于1.4 eV)比在Ag中观察到的大(约0.3 eV)。对于较小的(5-20​​ nm)铝球(> 95%),辐射对阻尼的贡献超过非辐射效应,而对于类似尺寸的银球,阻尼几乎完全归因于整体介电函数(非辐射)。对于Al纳米棒,可以通过增加长宽比来缩小线宽,以便对于4.5的长宽比,总的Al(0.75 eV)线宽可以合理地接近相同尺寸的Ag棒(0.35 eV)的线宽。这种变窄是由于Al介电函数实部中的频率色散引起的,并且与Al的线宽的辐射贡献降低了65%(1.5至0.5 eV)有关。同时,随着长宽比的增加,等离激元调谐为红色,从而使非辐射宽度增加。这证明了各向异性可以用作控制Al等离激元移相的参数,其中可以根据纵横比调整等离激元线宽(辐射或非辐射)的组成。总体而言,这些数据表明,Al纳米结构中的局部表面等离振子共振移相机理与贵金属固有地不同,这可能允许等离激元材料的新应用,可调节的等离振子寿命和新的物理现象得以观察。

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