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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Jensen, Flemming
Technical University of Denmark
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (32/32 displayed)
- 2020Fabrication of hollow coaxial Al 2 O 3 /ZnAl 2 O 4 high aspect ratio freestanding nanotubes based on the Kirkendall effectcitations
- 2020Fabrication of hollow coaxial Al2O3/ZnAl2O4 high aspect ratio freestanding nanotubes based on the Kirkendall effectcitations
- 2019High Frequency Pulse Anodising of Aluminium for Decorative Applications
- 2019High frequency pulse anodising of recycled 5006 aluminium alloy for optimised decorative appearancecitations
- 2018Experimental observation of Dyakonov plasmons in the mid-infraredcitations
- 2017Advanced fabrication of hyperbolic metamaterials
- 2017Influence of Ti and Cr Adhesion Layers on Ultrathin Au Filmscitations
- 2017Large-scale high aspect ratio Al-doped ZnO nanopillars arrays as anisotropic metamaterials.citations
- 2017Highly ordered Al-doped ZnO nano-pillar and tube structures as hyperbolic metamaterials for mid-infrared plasmonics
- 2016Fabrication of high aspect ratio TiO2 and Al2O3 nanogratings by atomic layer depositioncitations
- 2016Conductive Oxides Trench Structures as Hyperbolic Metamaterials in Mid-infrared Range
- 2016Fabrication of high aspect ratio TiO 2 and Al 2 O 3 nanogratings by atomic layer depositioncitations
- 2016Fabrication of deep-profile Al-doped ZnO one- and two-dimensional lattices as plasmonic elements
- 2015Friction stir processed Al–TiO2 surface composites: Anodising behaviour and optical appearancecitations
- 2015Effect of High Frequency Pulsing on the Interfacial Structure of Anodised Aluminium-TiO2citations
- 2015Ultra-thin Metal and Dielectric Layers for Nanophotonic Applicationscitations
- 2015Friction stir processed Al-TiO 2 surface composites:Anodising behaviour and optical appearancecitations
- 2015High Frequency Anodising of Aluminium-TiO2 Surface Compositescitations
- 2015Friction stir processed Al-TiO 2 surface composites:DC vs. High frequency pulse and pulse reverse anodising
- 2015High frequency anodising of aluminium–TiO2 surface composites: Anodising behaviour and optical appearancecitations
- 2015Injection molded polymeric hard X-ray lensescitations
- 2015Effect of High Frequency Pulsing on the Interfacial Structure of Anodized Aluminium-TiO2citations
- 2015High frequency anodising of aluminium-TiO 2 surface composites:Anodising behaviour and optical appearancecitations
- 2015Effect of High Frequency Pulsing on the Interfacial Structure of Anodised Aluminium-TiO 2citations
- 2015Friction stir processed Al–TiO 2 surface composites: Anodising behaviour and optical appearancecitations
- 2014Friction stir processed Al - Metal oxide surface composites: Anodization and optical appearance
- 2014Optical appearance of AC anodized Al/TiO 2 composite coatings
- 2014Depositing Materials on the Micro- and Nanoscale
- 2014Microstructure and optical appearance of anodized friction stir processed Al - Metal oxide surface composites
- 2014Optical appearance of AC anodized Al/TiO2 composite coatings
- 2014Etching patterns on the micro‐ and nanoscale
- 2012Dynamic measurement of mercury adsorption and oxidation on activated carbon in simulated cement kiln flue gascitations
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document
Fabrication of deep-profile Al-doped ZnO one- and two-dimensional lattices as plasmonic elements
Abstract
In this work, we report on fabrication of deep-profile one- and two-dimensional lattices made from Al-doped ZnO (AZO). AZO is considered as an alternative plasmonic material having the real part of the permittivity negative in the near infrared range. The exact position of the plasma frequency of AZO is doping concentration dependent, allowing for tuning possibilities. In addition, the thickness of the AZO film also affects its material properties. Physical vapor deposition techniques typically applied for AZO coating do not enable deep profiling of a plasmonic structure. Using the atomic layer deposition technique, a highly conformal deposition method, allows us to fabricate high-aspect ratio structures such as one-dimensional lattices with a period of 400 nm and size of the lamina of 200 nm in width and 3 µm<br/>in depth. Thus, our structures have an aspect ratio of 1:15 and are homogeneous on areas of 2x2 cm2 and more. We also produce two-dimensional arrays of circular nanopillars with similar dimensions. Instead of nanopillars hollow tubes with a wall thickness on demand from 20 nm up to a complete fill can be fabricated.