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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
Places of action
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document
3D geometrically isotropic metamaterial for telecom wavelengths
Abstract
We present a new design for a unit cell with the cubic symmetry and sizes less than one sixth of the vacuum wavelength possessing a negative refractive index in the IR region. The main challenges in designing and fabricating metamaterials nowadays are in obtaining isotropic electric and magnetic responses keeping in the same time the cell dimensions within the effective medium approximation. Several approaches have been made to develop such a structure in the microwave region [1, 2], nevertheless, there is still a lack of structures to be used in the IR and visible diapasons. Since the dimension of the unit cell is not infinitely small, certain geometrical constraints have to be fulfilled to obtain an isotropic response of the material [3]. These conditions and the metal behaviour close to the plasma frequency increase the design complexity. Our unit cell is composed of two main parts. The first part generates the electric response, thus providing the negative real part of permittivity in the desired spectral range. The usual way is to utilize a set of metallic wires, so called diluted metal that exhibits a Drude-like behaviour. Our study shows that this behaviour is obtainable if the wires are arranged in a cage-like structure. For the magnetic response we use metallic plates forming an open cube located inside the “cage”. For this topology the plates can be thought of as capacitors in a resonant LC circuit [4]. By adjusting the resonant circuit frequency in the IR range a double negative response is obtained in a certain bandwidth. The proposed unit cell has the cubic point group of symmetry and being repeatedly placed in space can effectively reveal isotropic optical properties. We use the CST commercial software to characterise the “cube-in-cage” structure. Reflection and transmission spectra are shown in Fig.1a. The effective refractive index is retrieved accordingly to the standard algorithm [5] (see Fig.1b). After several cycles of naïve optimizations, the refractive index reaches -2.4 at 1.55μm (ca. 192.5THz). The maximum FOM in the band, where Re(n) <0 is 2.4 at 1.54μm (ca. 195.2THz). At this wavelength the refraction index is equal to -1.44. These values together with the effective cubic symmetry of the unit cell entitle us to assume the high potential of the suggested design as a constitutive block for an isotropic, relatively low-loss, metamaterial in the near IR region.