Zhengqing Qi, Jie Yao, Liangliang Zhao, Yiping Cui, Changgui Lu, "Tunable double-resonance dimer structure for surface-enhanced Raman scattering substrate in near-infrared region," Photonics Res. 3, 313 (2015)

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- Photonics Research
- Vol. 3, Issue 6, 313 (2015)

Fig. 1. Schematic of double-resonance gold dimer array substrate.

Fig. 2. (a) Simulated electric field intensity enhancement factors of the dimer grating (green solid line), the single disk grating (black square line), a single dimer (red circle line), and a single disk (blue triangle line) upon gold film separated by a layer of silica spacer. (b) Ez amplitude at position 2 for the gold dimer array case. (c) Schematics of the four structures simulated.

Fig. 3. (a) Intensity (| E | 2 ) distribution on the half-height surface of the gold disk with h SiO 2 = 45 nm at 785 nm (SPR) with maximum intensity 2042. (b) 950 nm (LSPR) with maximum intensity 7066 corresponding to the two resonant modes of the dimer grating case in Fig. 2(a) , respectively.

Fig. 4. (a) Simulated electric field spectrum for the structure with P x = 550 nm , P y = 500 nm , and d = 60 nm at different thicknesses of the silica spacer. (b) Holistic enhancement G SERS via the change of the thickness of the silica spacer.

Fig. 5. Electric field spectrum with P x = 550 nm , P y = 500 nm , and h SiO 2 = 45 nm at different interparticle separations: 15 nm (black line), 30 nm (red dot-dotted dash line), and 45 nm (blue dotted–dashed line).
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Table 1. Normalized Effective Mode Volume and the Quality Factor for Different Interparticle Separation Dimers, a Single Dimer with a Gap of 15 nm, and a Single Disk upon Gold Film Separated by a Layer of Silica Spacer

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