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Optical properties of gold particles with near micron size: localized and propagating surface plasmons

机译:接近微米尺寸的金粒子的光学特性:局部等离激元等离激元

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This proceeding summarizes the optical properties of plasmonic structures from nanoscale to macroscale. Of particular interest, Au triangles and hole arrays of near micron size exhibit concomitantly surface plasmon resonance (SPR) and localized surface plasmon resonance (LSPR) optical properties in the Vis-NIR region, resulting in excellent optical properties for biosensing. In transmission spectroscopy, 15 nm nanoparticles absorbs at λ = 525 nm, nanotriangles of > 200 nm edge length absorbs at λ > 600 nm while nanohole arrays exhibit a more complex spectrum including absorption and enhanced optical transmission (EOT) features. Nanohole arrays are also sensitive to refractive index (RI) change and it can be optimized by tailoring the hole diameter and the periodicity. Au triangles ranging from nano (200 nm) to micron size (1.5 μm) are active in LSPR with an absorption peak that redshifts with the increasing aspect ratio of the structure. In total internal reflection (TIR) experiment, Au triangles with an edge length of 500 nm or greater present an absorption peak at λ = 800 nm. Also, triangles of 700, 950 and 1800 nm have a maximum transmission around λ = 650 nm that is highly sensitive to refraction index (RI) variations. This absorption peak is attributed to propagating SPR, similarly to the optical phenomenon occurring on a smooth Au film as used in the Kretschmann configuration of SPR. Lastly, nanohole and microhole arrays spectra, measured in TIR, are a composite of both triangles (LSPR) and thin film spectra (SPR).
机译:此过程总结了从纳米尺度到宏观尺度的等离激元结构的光学性质。特别令人感兴趣的是,Au三角形和接近微米尺寸的孔阵列在Vis-NIR区域中同时显示表面等离振子共振(SPR)和局部表面等离振子共振(LSPR)光学特性,从而为生物传感提供了出色的光学特性。在透射光谱学中,15 nm纳米颗粒在λ= 525 nm处吸收,边缘长度> 200 nm的纳米三角形在λ> 600 nm处吸收,而纳米孔阵列则表现出更复杂的光谱,包括吸收和增强的光学透射(EOT)功能。纳米孔阵列对折射率(RI)的变化也很敏感,可以通过调整孔径和周期性来对其进行优化。在LSPR中,从纳米(200 nm)到微米大小(1.5μm)的金三角形具有活跃的吸收峰,吸收峰随着结构的长宽比的增加而发生红移。在全内反射(TIR)实验中,边长为500 nm或更大的Au三角形在λ= 800 nm处出现吸收峰。同样,700、950和1800 nm的三角形在λ= 650 nm附近具有最大透射率,它对折射率(RI)的变化高度敏感。该吸收峰归因于传播的SPR,类似于在SPR的Kretschmann配置中使用的光滑Au膜上发生的光学现象。最后,在TIR中测量的纳米孔和微孔阵列光谱是三角形(LSPR)和薄膜光谱(SPR)的合成。

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