Amplified Photoluminescence of CsPbX3 Perovskites Confined in Silica Film with a Chiral Nematic Structure
Metal halide perovskites (MHPs, CsPbX3: X = Cl, Br, I) have advanced the field of optoelectronic devices due to their remarkable light‐emitting capabilities, stemming from the large overlap between their emission and absorption spectra, offering the possibility to reabsorb their own emitted photons....
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Veröffentlicht in: | Advanced materials interfaces 2024-01, Vol.11 (3), p.n/a |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Metal halide perovskites (MHPs, CsPbX3: X = Cl, Br, I) have advanced the field of optoelectronic devices due to their remarkable light‐emitting capabilities, stemming from the large overlap between their emission and absorption spectra, offering the possibility to reabsorb their own emitted photons. Herein, a straightforward method is reported to confine CsPbBr3 into mesoporous silica films with a chiral nematic structure, allowing the amplification of the photoluminescence (PL). The simple room temperature ligand‐free synthesis allows facile growth of CsPbBr3 in silica photonic films, in which the Bragg peak position can be tuned from the UV to the visible range. The perovskite/silica films demonstrate a remarkable improvement in PL intensity and lifetime compared to the as‐synthesized non‐confined perovskite nanocrystals (NCs) due to the overlap of the Bragg peak position of the chiral nematic photonic films and CsPbBr3 absorption band. Such a PL enhancement stems from the slow photon effect induced at blue and red Bragg peak edges that facilitates the photon recycling of the emitted photons. This innovative approach offers a new way to fabricate highly emissive and long‐lived photoluminescent films at ambient conditions, potentially advancing perovskite utilization in light‐emitting devices.
A simple ambient ligand‐free synthesis of the highly luminescent spherical CsPbBr3 perovskite nanoparticles is achieved in mesoporous silica photonic films. Such photoluminescence enhancement stems from the overlap of the Bragg peak position of the photonic films and CsPbBr3 absorption band, inducing the slow photon effect at Bragg peak edges facilitating the photon recycling of the emitted photons. |
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ISSN: | 2196-7350 2196-7350 |
DOI: | 10.1002/admi.202300636 |