Huang Yu, Zhou Qin, Hou Mengjing, Ma Lingwei, Zhang Zhengjun
State Key Laboratory of New Ceramics and Fine Processing, School of Materials Science and Engineering, Tsinghua University, Beijing 100084, P. R. China.
Institute of Nuclear and New Energy Technology, Tsinghua University, Beijing 100084, P. R. China.
Phys Chem Chem Phys. 2015 Nov 21;17(43):29293-8. doi: 10.1039/c5cp04460j.
In the field of plasmonics, the nanogap effect is often related to one aspect like the near-field enhancement at a single excitation wavelength or the far-field resonance shift. In this study, taking full advantage of finite element method (FEM) calculations, we present a comprehensive and quantitative analysis of the nanogap effect on the plasmonic behaviors of metallic nanoparticle dimers. Firstly, near-field spectroscopy is proposed in order to extract the near-field resonance wavelengths. Focusing on the bonding dipole mode, it is found that the near-field enhancement factors exhibit a weak power-law dependence on the gap size, while the near-field resonance shift decays nearly exponentially as the gap size increases, with a lower decay length than that for the far-field resonance shift. The spectral deviation between these two shifts is suggested to be taken into account for spectroscopy applications of plasmonic devices, although it may be negligible for dimer structures with rather small gaps.
在等离激元学领域,纳米间隙效应通常与单个激发波长下的近场增强或远场共振位移等某一方面相关。在本研究中,我们充分利用有限元方法(FEM)计算,对纳米间隙对金属纳米颗粒二聚体等离激元行为的影响进行了全面且定量的分析。首先,提出了近场光谱法以提取近场共振波长。聚焦于键合偶极子模式,发现近场增强因子对间隙尺寸呈现出较弱的幂律依赖性,而近场共振位移随着间隙尺寸的增加几乎呈指数衰减,其衰减长度比远场共振位移的衰减长度更低。建议在等离激元器件的光谱应用中考虑这两种位移之间的光谱偏差,尽管对于间隙相当小的二聚体结构来说,这种偏差可能可以忽略不计。