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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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Abbrent, Sabina
Institute of Macromolecular Chemistry
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (4/4 displayed)
- 2024Accelerating effect of metal ionic liquids for epoxy-anhydride copolymerizationcitations
- 2022Structure modulation for bandgap engineered vacancy-ordered Cs 3 Bi 2 Br 9 perovskite structures through copper alloyingcitations
- 2022Structure modulation for bandgap engineered vacancy-ordered Cs3Bi2Br9 perovskite structures through copper alloyingcitations
- 2020Magnetizing lead-free halide double perovskitescitations
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article
Structure modulation for bandgap engineered vacancy-ordered Cs3Bi2Br9 perovskite structures through copper alloying
Abstract
<p>Lead-free, vacancy-ordered, Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub> perovskite is considered promising inorganic, stable, and non-toxic halide perovskite for optoelectronic and photovoltaic applications. However, its wide bandgap limits its state-of-art applications. We notice an observable enhancement of light absorption of Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub> perovskite crystals upon CuBr<sub>2</sub> addition to the perovskite precursor. X-ray diffraction, <sup>133</sup>Cs solid state NMR, Raman spectroscopy, X-ray photoelectron spectroscopy, and density functional theory calculations were studied to find out the nature of the perovskite crystal formation mechanism. With the addition of up to 50% CuBr<sub>2</sub>, the Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub> perovskite retains its matrix structure with homogeneously distributed Cs<sub>2</sub>CuBr<sub>4</sub> large domains. Drop-casting of perovskite/DMSO solutions over TiO<sub>2</sub> thin films reveals a reduction of the direct bandgap from 2.56 eV for pristine Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub> to 1.77 eV for a 50% Cu<sup>2+</sup> alloyed one. First-principles calculations reveal the possibility of Cs<sub>2</sub>CuBr<sub>4</sub> phase formation with higher Cu alloying, which can be the main reason behind bandgap narrowing. For homogeneously Cu alloyed Cs<sub>3</sub>Bi<sub>2</sub>Br<sub>9</sub>, reduction of the effective bandgap can occur due to the formation of compensating defect levels (V<sub>Br</sub>, Cu<sub>Br</sub>) above the pristine valence band maxima (VBM). These results highlight the importance of alloying for structure modulation for bandgap engineered vacancy-ordered perovskite structures.</p>