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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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Mkhoyan, K. Andre
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (17/17 displayed)
- 2023Optical Properties of Electrochemically Gated La 1− xSr xCoO 3−δ as a Topotactic Phase-Change Materialcitations
- 2023Anomalous strain relaxation and its impact on the valence-driven spin-state/metal-insulator transition in epitaxial (Pr1−yYy)1−xCaxCoO3−δcitations
- 2023Spin Hall conductivity in Bi$_{1-x}$Sb$_x$ as an experimental test of bulk-boundary correspondence
- 2021Spin and Charge Interconversion in Dirac-Semimetal Thin Filmscitations
- 2020Layer Dependence of Dielectric Response and Water-Enhanced Ambient Degradation of Highly Anisotropic Black Ascitations
- 2020Ambipolar transport in van der Waals black arsenic field effect transistorscitations
- 2020Plasmonic nanocomposites of zinc oxide and titanium nitridecitations
- 2020Self-Assembled Periodic Nanostructures Using Martensitic Phase Transformationscitations
- 2020Thermal transport in ZnO nanocrystal networks synthesized by nonthermal plasmacitations
- 2018Room-temperature high spin–orbit torque due to quantum confinement in sputtered BixSe(1–x) filmscitations
- 2015Giant Spin Pumping and Inverse Spin Hall Effect in the Presence of Surface and Bulk Spin-Orbit Coupling of Topological Insulator Bi2Se3citations
- 2015Nonequilibrium-Plasma-Synthesized ZnO Nanocrystals with Plasmon Resonance Tunable via Al Doping and Quantum Confinementcitations
- 2015Hybrid molecular beam epitaxy for the growth of stoichiometric BaSnO3citations
- 2012Sputter deposition of semicrystalline tin dioxide filmscitations
- 2012Improving the damp-heat stability of copper indium gallium diselenide solar cells with a semicrystalline tin dioxide overlayercitations
- 2010Orientation and morphological evolution of catalyst nanoparticles during carbon nanotube growthcitations
- 2010Effect of hydrogen on catalyst nanoparticles in carbon nanotube growthcitations
Places of action
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article
Nonequilibrium-Plasma-Synthesized ZnO Nanocrystals with Plasmon Resonance Tunable via Al Doping and Quantum Confinement
Abstract
<p>Metal oxide semiconductor nanocrystals (NCs) exhibit localized surface plasmon resonances (LSPRs) tunable within the infrared (IR) region of the electromagnetic spectrum by vacancy or impurity doping. Although a variety of these NCs have been produced using colloidal synthesis methods, incorporation and activation of dopants in the liquid phase has often been challenging. Herein, using Al-doped ZnO (AZO) NCs as an example, we demonstrate the potential of nonthermal plasma synthesis as an alternative strategy for the production of doped metal oxide NCs. Exploiting unique, thoroughly nonequilibrium synthesis conditions, we obtain NCs in which dopants are not segregated to the NC surfaces and local doping levels are high near the NC centers. Thus, we achieve overall doping levels as high as 2 × 10<sup>20</sup> cm<sup>-3</sup> in NCs with diameters ranging from 12.6 to 3.6 nm, and for the first time experimentally demonstrate a clear quantum confinement blue shift of the LSPR energy in vacancy- and impurity-doped semiconductor NCs. We propose that doping of central cores and heavy doping of small NCs are achievable via nonthermal plasma synthesis, because chemical potential differences between dopant and host atoms - which hinder dopant incorporation in colloidal synthesis - are irrelevant when NC nucleation and growth proceed via irreversible interactions among highly reactive gas-phase ions and radicals and ligand-free NC surfaces. We explore how the distinctive nucleation and growth kinetics occurring in the plasma influences dopant distribution and activation, defect structure, and impurity phase formation.</p>