纳米柱
波长
材料科学
时域有限差分法
光学
等离子体子
拉曼散射
光电子学
电磁场
电磁辐射
散射
近场和远场
极化(电化学)
拉曼光谱
物理
纳米技术
纳米结构
化学
物理化学
量子力学
作者
N.K. Gupta,Rajib Ghosh,Anuj Dhawan
摘要
Bridged-bowtie nanohole arrays and cross bridged-bowtie nanohole arrays in a gold film are presented as surfaceenhanced Raman scattering (SERS) substrates. We employed the numerical FDTD method to calculate the maximum electromagnetic SERS enhancement factor (EF) as a function of wavelength. It is found that the proposed nanohole arrays do not only display an extremely large enhancement factor but also have the hotspot spread over a larger area compared to the various other nanopillar structures. The calculation of electromagnetic SERS enhancement factor reveals that the cross bridged-bowtie nanohole arrays exhibit the maximum electromagnetic SERS EF of ~ 109 spreading over an area of 100 nm2. In addition, the electromagnetic SERS EF of ~ 108 is spread over 500 nm2 area which is higher than hotspot area in case of nanopillar structures. The resonance wavelength of the nanohole array can be tuned by varying the size of the nanoholes. These nanohole arrays can be employed both in transmission as well as in reflection mode as effective SERS substrates. In addition, bridged-bowtie and cross bridged-bowtie nanohole arrays show the significantly high electromagnetic SERS EF at more than one wavelength and therefore are useful for application involving multiple wavelength SERS response. Furthermore, the cross bridged-bowtie nanohole array exhibit the spatial tunability of hotspot by rotating the direction of polarization of incident field.
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