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| Naji, M. |
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| Motta, Antonella |
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| Mohamed, Tarek |
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| Ertürk, Emre |
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| Taccardi, Nicola |
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| Petrov, R. H. | Madrid |
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| Bih, L. |
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| Casati, R. |
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| Kočí, Jan | Prague |
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| Šuljagić, Marija |
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| Azam, Siraj |
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| Ospanova, Alyiya |
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| Ali, M. A. |
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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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Noual, Adnane
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Publications (5/5 displayed)
- 2022Optomechanical Hot-Spots in Metallic Nanorod–Polymer Nanocompositescitations
- 2022Optomechanical Hot-Spots in Metallic Nanorod–Polymer Nanocompositescitations
- 2021Optomechanic Coupling in Ag Polymer Nanocomposite Filmscitations
- 2020Optically reconfigurable graphene/metal metasurface on Fe:LiNbO3 for adaptive THz opticscitations
- 2016Nanopores within 3D-structured gold film for sensing applications
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article
Optically reconfigurable graphene/metal metasurface on Fe:LiNbO3 for adaptive THz optics
Abstract
We demonstrate, experimentally, nonvolatile optical control of terahertz metasurfaces composed of a metallic split-ring resonator array sandwiched between monolayer graphene and a photoconductive Fe:LiNbO<sub>3</sub> substrate. We demonstrate frequency-selective tuning of THz transmission amplitude, and our results pave the way toward spatially resolved control of THZ metasurfaces for beam steering, imaging, and sensing applications. The substrate (Fe:LiNbO<sub>3</sub>) supports nonvolatile yet reversible photoinduced charge distributions, which locally modify the electrostatic environment of the nano-thickness graphene monolayer, altering the graphene electrical conductivity and therefore changing the resonance spectra of the metamaterial array. We present light-induced normalized transmittance changes up to 35% that are nonvolatile and persist after the illumination source is removed yet can be reversed by thermal annealing.