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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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Wuttig, Matthias
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (39/39 displayed)
- 2024Ostwald Ripening of Ag<sub>2</sub>Te Precipitates in Thermoelectric PbTe: Effects of Crystallography, Dislocations, and Interatomic Bondingcitations
- 2024Metavalent or Hypervalent Bonding:Is There a Chance for Reconciliation?citations
- 2024Ostwald Ripening of Ag2Te precipitates in thermoelectric PbTe: effects of crystallography, dislocations, and interatomic bondingcitations
- 2024Metavalent or Hypervalent Bondingcitations
- 2023A Quantitative Investigation of Functionalized Glazing Stacks by Atom Probe Tomographycitations
- 2023Amorphous and highly nonstoichiometric titania (TiOx) thin films close to metal-like conductivity
- 2023Metavalent or Hypervalent Bonding: Is There a Chance for Reconciliation?citations
- 2022Scaling and Confinement in Ultrathin Chalcogenide Films as Exemplified by GeTecitations
- 2022Nanostructured In3SbTe2 antennas enable switching from sharp dielectric to broad plasmonic resonances
- 2022Halide Perovskites: Advanced Photovoltaic Materials Empowered by a Unique Bonding Mechanismcitations
- 2022Nanostructured In<sub>3</sub>SbTe<sub>2</sub> antennas enable switching from sharp dielectric to broad plasmonic resonancescitations
- 2022The glass transition of water, insight from phase change materialscitations
- 2022Nanostructured In 3 SbTe 2 antennas enable switching from sharp dielectric to broad plasmonic resonancescitations
- 2022Fragile-to-Strong Transition in Phase-Change Material Ge 3 Sb 6 Te 5citations
- 2021Phase Change Memory Materials by Design
- 2021Metavalent Bonding in Phase Change Materials:Provocation or Promise?
- 2021Combining switchable phase‐change materials and phase‐transition materials for thermally regulated smart mid‐infrared modulatorscitations
- 2021The potential of chemical bonding to design crystallization and vitrification kineticscitations
- 2021Halide Perovskites: Advanced Photovoltaic Materials Empowered by a Unique Bonding Mechanism
- 2021Metavalent Bonding in Solids: Provocation or Promise?
- 2021Non-volatile photonic Applications with Phase Change Materials
- 2021Approaching the Glass Transition Temperature of GeTe by Crystallizing Ge 15 Te 85citations
- 2021Metavalent Bonding in Crystalline Solids: How Does It Collapse?citations
- 2021Metavalent Bonding in Crystalline Solids: How Does It Collapse?citations
- 2021Approaching the Glass Transition Temperature of GeTe by Crystallizing Ge<sub>15</sub>Te<sub>85</sub>citations
- 2020Violation of the Stokes–Einstein relation in Ge2Sb2Te5, GeTe, Ag4In3Sb67Te26, and Ge15Sb85, and its connection to fast crystallizationcitations
- 2020Changes of structure and bonding with thickness in chalcogenide thin filmscitations
- 2019Switching between Crystallization from the Glassy and the Undercooled Liquid Phase in Phase Change Material Ge 2 Sb 2 Te 5citations
- 2019Role of grain boundaries in Ge–Sb–Te based chalcogenide superlatticescitations
- 2019Persistence of spin memory in a crystalline, insulating phase-change materialcitations
- 2018Unique Bond Breaking in Crystalline Phase Change Materials and the Quest for Metavalent Bondingcitations
- 2018Atomic disordering processes in crystalline GeTe induced by ion irradiationcitations
- 2017Formation of resonant bonding during growth of ultrathin GeTe filmscitations
- 2016Interband characterization and electronic transport control of nanoscaled GeTe/Sb2Te3 superlatticescitations
- 2016Ordered Peierls distortion prevented at growth onset of GeTe ultra-thin filmscitations
- 2014Amorphous and highly nonstoichiometric titania (TiOx) thin films close to metal-like conductivitycitations
- 2012Role of vacancies in metal-insulator transitions of crystalline phase-change materialscitations
- 2011The influence of a temperature dependent band gap on the energy scale of modulated photocurrent experimentscitations
- 2008Investigation of SnSe, SnSe2, and Sn2Se3 alloys for phase change memory applicationscitations
Places of action
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article
Nanostructured In<sub>3</sub>SbTe<sub>2</sub> antennas enable switching from sharp dielectric to broad plasmonic resonances
Abstract
<jats:title>Abstract</jats:title><jats:p>Phase-change materials (PCMs) allow for non-volatile resonance tuning of nanophotonic components. Upon switching, they offer a large dielectric contrast between their amorphous and crystalline phases. The recently introduced “plasmonic PCM” In<jats:sub>3</jats:sub>SbTe<jats:sub>2</jats:sub> (IST) additionally features in its crystalline phase a sign change of its permittivity over a broad infrared spectral range. While optical resonance switching in unpatterned IST thin films has been investigated before, nanostructured IST antennas have not been studied, yet. Here, we present numerical and experimental investigations of nanostructured IST rod and disk antennas. By crystallizing the IST with microsecond laser pulses, we switched individual antennas from narrow dielectric to broad plasmonic resonances. For the rod antennas, we demonstrated a resonance shift of up to 1.2 µm (twice the resonance width), allowing on/off switching of plasmonic resonances with a contrast ratio of 2.7. With the disk antennas, we realized an increase of the resonance width by more than 800% from 0.24 µm to 1.98 µm while keeping the resonance wavelength constant. Further, we demonstrated intermediate switching states by tuning the crystallization depth within the resonators. Our work empowers future design concepts for nanophotonic applications like active spectral filters, tunable absorbers, and switchable flat optics.</jats:p>