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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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Soavi, Giancarlo
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Topics
Publications (6/6 displayed)
- 2022Strongly Coupled Coherent Phonons in Single-Layer MoS2.
- 2022Wide‐Bandgap Double Perovskites with Multiple Longitudinal‐Optical Phonon Scatteringcitations
- 2020Strongly Coupled Coherent Phonons in Single-Layer MoS2citations
- 2020Control of crystal symmetry breaking with halogen substituted benzylammonium in layered hybrid metal-halide perovskitescitations
- 2019Hot electrons modulation of third harmonic generation in graphene
- 2015Ultrafast pseudospin dynamics in graphenecitations
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article
Wide‐Bandgap Double Perovskites with Multiple Longitudinal‐Optical Phonon Scattering
Abstract
<jats:title>Abstract</jats:title><jats:p>Alloyed lead‐free double perovskites display intense photoluminescence, are environmentally friendly, and their devices show long‐term operation. Thanks to these properties, which make them excellent warm white‐emitting materials, they have recently received great attention in lighting applications. An important factor to tune the optical properties of alloyed lead‐free double perovskites is the presence of self‐trapped excitons. Here, it is demonstrated that in lead‐free double perovskites, the strong electron–phonon coupling plays a crucial role in the generation of self‐trapped excitons. The strong electron–phonon coupling is confirmed by a large Huang–Rhys factor and by the presence of multiphonon transitions. In particular, sharp emission lines superimposed on the broad photoluminescence emission band of one of these samples (Cs<jats:sub>2</jats:sub>Ag<jats:sub>0.6</jats:sub>Na<jats:sub>0.4</jats:sub>InCl<jats:sub>6</jats:sub> 0.5%Bi) are observed; these are due to the strong coupling of longitudinal‐optical phonons with excited electronic states caused by the tetragonally distorted AgCl<jats:sub>6</jats:sub> octahedrons. Such a strong coupling of longitudinal‐optical phonons to electrons can effectively modulate the photophysical properties of alloyed double perovskites, and its understanding is, thus, of paramount importance for the design of future optoelectronic devices.</jats:p>