Abstract

It was predicted a few years ago that a medium with negative index of refraction would allow for perfect imaging. Although no material has been found so far that behaves as a perfect lens, some experiments confirmed the theoretical predictions in the near-field, or quasi-static, regime where the behaviour of a negative index medium can be mimicked by a thin layer of noble metal, such as silver. These results are normally attributed to the excitation of surface plasmons in the metal, which only leads to the restoration of p-polarized evanescent waves. In this work, we show that the restoration of s-polarized evanescent waves and, correspondingly, sub-wavelength imaging by a single dielectric slab are possible. Specifically, we show that at λ = 632 nm a thin layer of GaAs behaves as a superlens for s-polarized waves. Replacing the single-metal slab by a dielectric is not only convenient from a technical point of view, it being much easier to deposit and control the thickness and flatness of dielectric films than metal ones, but also invites us to re-think the connection between surface plasmon excitation and the theory of negative refraction.

Highlights

  • It was predicted a few years ago that a medium with negative index of refraction would allow for perfect imaging

  • It is shown that a thin layer of gallium arsenide (GaAs) efficiently enhances the s-polarized evanescent waves contained in the angular spectrum of a subwavelength object to be imaged

  • Any roughness would be a source of additional surface plasmon excitation that would have detrimental effects on the quality of the image

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Summary

Introduction

It was predicted a few years ago that a medium with negative index of refraction would allow for perfect imaging. No material has been found so far that behaves as a perfect lens, some experiments confirmed the theoretical predictions in the near-field, or quasi-static, regime where the behaviour of a negative index medium can be mimicked by a thin layer of noble metal, such as silver. These results are normally attributed to the excitation of surface plasmons in the metal, which only leads to the restoration of p-polarized evanescent waves. In order to confirm that this effect originates from the presence of the thin layer of GaAs, the same transmission function has been computed for different structures, but with GaAs either removed (figure 2, green curve) or replaced by a layer of the same thickness ts

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