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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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Malureanu, Radu
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (51/51 displayed)
- 2022Chemical Vapor-Deposited Graphene on Ultraflat Copper Foils for van der Waals Hetero-Assemblycitations
- 2022Chemical Vapor-Deposited Graphene on Ultraflat Copper Foils for van der Waals Hetero-Assemblycitations
- 2021Acceleration of radiative recombination in quasi-2D perovskite films on hyperbolic metamaterialscitations
- 2020Plasmonic nanojet:an experimental demonstrationcitations
- 2020Microspherical nanoscopy: is it a reliable technique?citations
- 2020Microspherical nanoscopy: is it a reliable technique?citations
- 2020Plasmonic nanojetcitations
- 2019Lamellas metamaterials: Properties and potential applications
- 2019Lamellas metamaterials: Properties and potential applications
- 2018Initial Investigation for the Fabrication of Hyperbolic Metamaterials Based on Ultra-Thin Au Layers
- 2018Which Computational Methods Are Good for Analyzing Large Photonic Crystal Membrane Cavities?
- 2018Which Computational Methods Are Good for Analyzing Large Photonic Crystal Membrane Cavities?
- 2017Advanced fabrication of hyperbolic metamaterials
- 2017Two-Photon Polymerization lithography for three-dimensional micro polymer parts manufacturing evaluation
- 2017Broadband infrared absorption enhancement by electroless-deposited silver nanoparticlescitations
- 2016Conductive Oxides Trench Structures as Hyperbolic Metamaterials in Mid-infrared Range
- 2016Fabrication of deep-profile Al-doped ZnO one- and two-dimensional lattices as plasmonic elements
- 2015Ultra-thin Metal and Dielectric Layers for Nanophotonic Applicationscitations
- 2014Super-resolution near field imaging device
- 2014Super-resolution near field imaging device
- 2014Linear and nonlinear properties of chalcogenide glasses in the terahertz frequency
- 2014Nanoplasmonic solution for nonlinear optics
- 2013Terahertz-induced Kerr effect in amorphous chalcogenide glassescitations
- 2013Fabrication and characterization of transparent metallic electrodes in the terahertz domain
- 2013Fabrication and characterization of transparent metallic electrodes in the terahertz domain
- 2012Metamaterials modelling, fabrication, and characterisation techniques
- 2012Metamaterials modelling, fabrication, and characterisation techniques
- 2012Ultrabroadband terahertz spectroscopy of chalcogenide glassescitations
- 2012Metamaterials modelling, fabrication and characterisation techniques
- 2012Metamaterials modelling, fabrication and characterisation techniques
- 2011Enhanced broadband optical transmission in metallized woodpilescitations
- 2011Enhanced broadband optical transmission in metallized woodpilescitations
- 2011Wave impedance retrieving via Bloch modes analysis
- 2011Wave impedance retrieving via Bloch modes analysis
- 2011Wave propagation in structured materials as a platform for effective parameters retrieving
- 2011Ultrabroadband THz spectroscopy of disordered materials
- 2010Enhanced broadband optical transmission in metallized woodpiles
- 2010Enhanced broadband optical transmission in metallized woodpiles
- 2010Optimisation of the electroless metal deposition technique for use in photonics
- 2010Optimisation of the electroless metal deposition technique for use in photonics
- 2010Controlled Ag electroless deposition in bulk structures with complex three-dimensional profilescitations
- 2010Controlled Ag electroless deposition in bulk structures with complex three-dimensional profilescitations
- 2009Isotropic metal deposition technique for metamaterials fabrication
- 2009Nested structures approach for bulk 3D negative index materials:[invited]
- 20093D geometrically isotropic metamaterial for telecom wavelengths
- 20093D geometrically isotropic metamaterial for telecom wavelengths
- 2009Bulk metamaterials: Design, fabrication and characterization
- 2009Isotropic metal deposition technique for metamaterials fabrication
- 2009Bulk metamaterials: Design, fabrication and characterization:[invited]
- 2009Nested structures approach for bulk 3D negative index materials
- 2008Accurate analysis of planar metamaterials using the RLC theory
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document
Fabrication and characterization of transparent metallic electrodes in the terahertz domain
Abstract
The demand for transparent electrodes keeps increasing as new generations of electronic devices appear, including solar cells and touch screens. Indium tin oxide (ITO) is the most promising transparent electrode material to date [1] although there are several limitations when using ITO. Firstly, it is a brittle material and therefore flexible devices such as electronic paper would be hard to achieve. Secondly, the continuous increase in the price of indium due to limited availability worldwide makes its use unsustainable in the future.<br/>Our work is motivated by early work [2] showing that an optically opaque layer with a negative permittivity can be perfectly transparent when sandwiched between two carefully designed metamaterial layers. Here we present a method to achieve a transparent metallic electrode deposited on a substrate. By placing a composite layer consisting of dielectric and metallic stripes (AB layer) on top of the metallic electrode (C layer) (see Fig. 1(a)) we found that the backscattering from the metallic film (C layer) can be almost perfectly canceled, leading to transparency of the whole structure. We fabricated the transparent metallic electrodes and characterized them by the use of the T-Ray 4000 terahertz time-domain spectroscopy system. The physics behind the cancellation of the scattering from the target opaque layer requires carefully chosen geometrical parameters of the metamaterial layers, AB and C, (see Fig. 1(b)). Figure 1(c) displays the transmittance through the whole sample normalized to that through the silicon substrate. The transmittance through the C layer mesh is quite low for the frequency range 0.2 - 0.8 THz, reaching its maximum of approximately 0.45 at 0.8 THz. By placing the AB mesh on top of the C layer separated by 12.5 μm silica, the ABC device achieves almost a perfect transmittance at 0.57 THz. Moreover, in the frequency range 0.3 - 0.6 THz the ABC device has still higher transmittance than the C layer alone. Our experimental results match nicely with the full-wave simulations (solid lines, Fig. 1(c)) [3].