Opto-Electronic Advances, 2018, 1 (6): 180010, Published Online: Mar. 19, 2019  

Mode evolution and nanofocusing of grating-coupled surface plasmon polaritons on metallic tip

Author Affiliations
1 MOE Key Laboratory of Material Physics and Chemistry under Extraordinary Conditions and Shaanxi Key Laboratory of Optical Information Technology, School of Science, Northwestern Polytechnical University, Xi'an 710072, China
2 Key Laboratory of Optoelectronic Technology and Systems (Ministry of Education), Chongqing University, Chongqing 400044, China
3 MOE Key Laboratory of Weak-Light Nonlinear Photonics, TEDA Applied Physics Institute and School of Physics, Nankai University, Tianjin 300457, China
Figures & Tables

Fig. 1. Geometry of a conical silver tip with grating-assisted light coupling.The excitation light is focused onto the diffractive grating. R is the cross-sectional radius of the tip body gradually decreasing from 1 μm to 20 nm. The tip apex is modeled as a hemisphere with a radius of r.

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Fig. 2. (a) Sketch map of SPPs excitation using a planar grating; (b) Dispersion relationship of SPPs and the grating coupling; (c) Reflection obtained from the field monitor located above the surface without grating; (d) Re(Hy) distribution of the grating-coupled SPPs generation and propagation along the silver-air interface with excitation wavelength at λ=632.8 nm and θ=28.5°.

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Fig. 3. Effective indices neff in real part (a) and imaginary part (b) of guided SPP modes versus the radius of cylindrical silver guide R. (c) Sketch map of a silver tip removing the diffracting grating. (d–j) Transverse modes intensity distributions of guided modes for R=1 μm.

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Fig. 4. (a) Transverse mode intensity distributions of the grating-coupled SPPs at R=1 μm; (b–g) Transverse mode intensity distributions of the hybrid mode at R=800, 750, 600, 350, 230, and 20 nm, respectively. (h) Electric field intensity distribution at the tip apex. (i) Transverse electric field intensity distribution at 1 nm below the tip apex.

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Fig. 5. Adiabatic parameter δ of TM01 mode versus R.

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Fig. 6. (a) Gap-mode configuration with the gap distance d=2 nm. (b) Electric field intensity and polarization distributions in the x-z plane. (c) Electric field intensity distribution in the x-y plane at 1 nm below the tip apex. (d) Comparison of electric field enhancement factor between the non-gap mode (Fig. 4(i)) and gap mode located at 1 nm below the apex of the silver tip.

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Fanfan Lu, Wending Zhang, Ligang Huang, Shuhai Liang, Dong Mao, Feng Gao, Ting Mei, Jianlin Zhao. Mode evolution and nanofocusing of grating-coupled surface plasmon polaritons on metallic tip[J]. Opto-Electronic Advances, 2018, 1(6): 180010.

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