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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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Lorenz, Michael
KU Leuven
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (13/13 displayed)
- 2024Ni‐Alloyed Copper Iodide Thin Films: Microstructural Features and Functional Performancecitations
- 2023Ultrawide bandgap willemite-type Zn<sub>2</sub>GeO<sub>4</sub> epitaxial thin filmscitations
- 2022Competing exciton localization effects due to disorder and shallow defects in semiconductor alloys
- 2020Control of phase formation of (AlxGa1 - X)2O3thin films on c-plane Al2O3
- 2017Structure and cation distribution of (Mn0.5Zn0.5)Fe2O4 thin films on SrTiO3(001)
- 2016The 2016 oxide electronic materials and oxide interfaces roadmap
- 2016Temperature dependent self-compensation in Al- and Ga-doped Mg0.05 Zn0.95O thin films grown by pulsed laser deposition
- 2016Room-temperature domain-epitaxy of copper iodide thin films for transparent CuI/ZnO heterojunctions with high rectification ratios larger than 109citations
- 2015Dielectric function in the spectral range (0.5–8.5)eV of an (Alx Ga1−x )2O3 thin film with continuous composition spread
- 2015Lattice parameters and Raman-active phonon modes of β-(AlxGa1−x)2O3
- 2015Correlation of magnetoelectric coupling in multiferroic BaTiO3-BiFeO3 superlattices with oxygen vacancies and antiphase octahedral rotations
- 2014Lattice parameters and Raman-active phonon modes of (InxGa1–x)2O3 for x < 0.4
- 2012Visible emission from ZnCdO/ZnO multiple quantum wellscitations
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article
Ni‐Alloyed Copper Iodide Thin Films: Microstructural Features and Functional Performance
Abstract
To tailor electrical properties of often degenerate pristine CuI, Ni is introduced as alloy constituent. Cosputtering in a reactive, but also in an inert atmosphere as well as pulsed laser deposition (PLD), is used to grow Ni x Cu 1 − x I $({Ni})_{x} ({Cu})_{1 - x} {I}$ thin films. The Ni content within the alloy thin films is systematically varied for different growth techniques and growth conditions. A solubility limit is evidenced by an additional NiI 2 (H 2 O) 6 $({NiI})_{2} (({(H})_{2} {O)})_{6}$ phase for Ni contents x ≥ 0.31 $x0.31$ , observed in X‐Ray diffraction and atomic force microscopy by a change in surface morphology. Furthermore, metallic, nanoscaled nickel clusters, revealed by X‐Ray photoelectron spectroscopy and high‐resolution transmission electron microscopy (HRTEM), underpin a solubility limit of Ni in CuI. Although no reduction of charge carrier density is observed with increasing Ni content, a dilute magnetic behavior of the thin films is observed in vibrating sample magnetometry. Further, independent of the deposition technique, unique multilayer features are observed in HRTEM measurements for thin films of a cation composition of x ≈ 0.06 $x$ . Opposite to previous claims, no transition to n‐type behavior was observed, which was also confirmed by density functional theory calculations of the alloy system.