Abstract

Plasmonic coupling provides a highly localized electromagnetic field in the gap of noble metals when illuminated by a light. The plasmonic field enhancement is generally known to be inversely proportional to the gap distance. Given such a relation, reducing the gap distance appears to be necessary to achieve the highest possible field enhancement. At the sub-nanometer scale, however, quantum mechanical effects have to be considered in relation to plasmonic coupling. Here, we use graphene as a spacer to observe plasmonic field enhancement in sub-nanometer gap. The gap distance is precisely controlled by the number of stacked graphene layers. We propose that the sudden drop of field enhancement for the single layer spacer is originated from the plasmon tunneling through the thin spacer. Numerical simulation which incorporates quantum tunneling is also performed to support the experimental results. From the fact that field enhancement with respect to the number of graphene layers exhibits different behavior in two wavelengths corresponding to on- and off-resonance conditions, tunneling phenomenon is thought to destroy the resonance conditions of plasmonic coupling.

Highlights

  • Khang June Lee, Shinho Kim, Woonggi Hong, Hamin Park, Min Seok Jang, Kyoungsik Yu & Sung-Yool Choi

  • We have investigated plasmonic coupling and the quantum tunneling in a vertically stacked structure of Au-NPs/ spacer/Au-film where the thickness of the spacer could be adjusted by the number of graphene layers

  • One noticeable feature among our observations is that a single-layer graphene spacer is so thin that the near-field enhancement associated with the plasmonic coupling is somewhat suppressed by the presence of quantum tunneling through the spacer

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Summary

Thickness of Graphene Spacer

Khang June Lee, Shinho Kim, Woonggi Hong, Hamin Park, Min Seok Jang, Kyoungsik Yu & Sung-Yool Choi. In the case of an SLG spacer, the resonance condition of plasmonic coupling is totally destroyed by the plasmon tunneling, and the field enhancement is considerably reduced in most spectral ranges. Such a tunneling phenomenon gradually disappears as the wavelength becomes large. This suggests that when designing plasmonic nanostructures a proper combination of spacer thickness and light wavelength needs to be carefully considered to achieve the highest possible plasmonic performance

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