Relation between 2D/3D chirality and the appearence of chiroptical effects in real nanostructures.

The optical activity of fabricated metallic nanostructures is investigated by complete polarimetry. While lattices decorated with nanoscale gammadia etched in thin metallic films have been described as two dimensional, planar nanostructures, they are better described as quasi-planar structures with...

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Detalles Bibliográficos
Autores: Arteaga Barriel, Oriol, Sancho i Parramon, Jordi, Nichols, Shane, Maoz, Ben M., Canillas i Biosca, Adolf, Bosch i Puig, Salvador, Markovich, Gil, Kahr, Bart
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2016
País:España
Institución:Varias* (Consorci de Biblioteques Universitáries de Catalunya, Centre de Serveis Científics i Acadèmics de Catalunya)
Repositorio:Recercat. Dipósit de la Recerca de Catalunya
OAI Identifier:oai:recercat.cat:2445/69182
Acceso en línea:https://hdl.handle.net/2445/69182
Access Level:acceso abierto
Palabra clave:Materials nanoestructurats
Plasmons
Nanoestructures
Quiralitat
Nanostructured materials
Plasmons (Physics)
Nanostructures
Chirality
Descripción
Sumario:The optical activity of fabricated metallic nanostructures is investigated by complete polarimetry. While lattices decorated with nanoscale gammadia etched in thin metallic films have been described as two dimensional, planar nanostructures, they are better described as quasi-planar structures with some three dimensional character. We find that the optical activity of these structures arises not only from the dissymmetric backing by a substrate but, more importantly, from the selective rounding of the nanostructure edges. A true chiroptical response in the far-field is only allowed when the gammadia contain these non-planar features. This is demonstrated by polarimetric measurements in conjunction with electrodynamical simulations based on the discrete dipole approximation that consider non-ideal gammadia. It is also shown that subtle planar dissymmetries in gammadia are sufficient to generate asymmetric transmission of circular polarized light.