Volume 5, Issue 18 pp. 2105-2110
Full Paper

Parallel Preparation of Densely Packed Arrays of 150-nm Gold-Nanocrescent Resonators in Three Dimensions

Markus Retsch

Markus Retsch

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany)

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Matthias Tamm

Matthias Tamm

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany)

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Noelia Bocchio

Noelia Bocchio

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany)

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Natalie Horn

Natalie Horn

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany)

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Renate Förch

Renate Förch

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany)

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Ulrich Jonas

Ulrich Jonas

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany)

FORTH/IESL Voutes Street, P.O. Box 1527, 1110 Heraklion, Crete (Greece)

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Maximilian Kreiter

Corresponding Author

Maximilian Kreiter

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany)

Max Planck Institut für Polymerforschung Ackermannweg 10, 55128 Mainz (Germany).Search for more papers by this author
First published: 14 September 2009
Citations: 57

Abstract

Metallic nanostructures show interesting optical properties due to their plasmonic resonances, and when arranged in three-dimensional (3D) arrays hold promise for optical metamaterials with negative refractive index. Towards this goal a simple, cheap, and parallel method to fabricate large-area, ordered arrays of 150-nm gold nanocrescents supporting plasmonic resonances in the near-infrared spectral range is demonstrated. In this process hexagonally ordered monolayers of monodisperse colloids are prepared by a simple floating technique, and subsequently the individual particles are size-reduced in a plasma process and used as a shadow mask with the initial lattice spacing. The resulting two-dimensional array of plasmonic resonators is coated with a transparent silica layer, which serves as a support for a second layer prepared by the identical process. The mutual orientation of the nanostructures between the individual layers can be freely adjusted, which determines the polarization-dependent absorption of the array and opens the possibility to introduce chirality in this type of 3D metamaterial. The iteration of this simple and efficient methodology yields 3D arrays with optical features as sharp as those of the individual nanocrescents, and shows strong potential for large-scale production of high-quality optical metamaterials.

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