Abstract

We systematically study the contribution of local-field distribution to second-harmonic generation (SHG) in cross-shaped Ag nanohole arrays, which is usually covered by resonance enhancement effect. By increasing one arm-length of the centrosymmetric cross-shaped Ag nanohole, the local-field distribution varies from centrosymmetric to non-centrosymmetric, while the localized surface plasmon resonance peak is red-shifted to the wavelength of the pumping laser accordingly. Both experimental and stimulated results indicate that the contribution of the asymmetric local-field distribution to SHG is quantitatively separated from a strong resonance enhancement effect. It shows that the pure effective second-order nonlinear susceptibility increases as the asymmetric degree of local-field distribution increases, and the largest effective second-order nonlinear susceptibility is ~2.5 times to that in a centrosymmetric local-field distribution. Our results provide evidence for optimizing the design of nonlinear plasmonic nanoantennas and metasurfaces.

Highlights

  • Localized surface plasmon resonances (LSPRs), arising from the interaction of light with noble metal nanostructures, can be described as the collective oscillations of free conduction electrons [1]

  • Since the resonance enhancement effect is usually prominent, this relatively small contribution from the asymmetric local-field distribution is neglected or covered by the strong resonance enhancement factors [31,32]. It is a complicated and crucial question to distinguish the influence of the asymmetric local-field distributions from the resonance enhancement effect and make a compromise between these two effects, which is essential in optimizing the designs of nonlinear plasmonic nanoantennas and metasurfaces

  • By increasing one arm-length of the centrosymmetric cross-shaped Ag nanohole, the local-field distribution varies from centrosymmetric to non-centrosymmetric

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Summary

Introduction

Localized surface plasmon resonances (LSPRs), arising from the interaction of light with noble metal nanostructures, can be described as the collective oscillations of free conduction electrons [1] It sensitively depends on the size and shape of nanostructures [2,3,4] and leads to a strong enhancement of local electromagnetic fields, which shows potential applications in super-resolution imaging [5], single molecule detection [6] and light harvesting [7]. The experimental results show that the contribution of asymmetric local-field can be quantitatively extracted from the strong resonance enhancement effect by a white-light supercontinuum signal, which is supported by a theoretical calculation based on nonlinear scattering theory.

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