2022
DOI: 10.1038/s41566-022-01103-x
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Extreme γ-ray radiation hardness and high scintillation yield in perovskite nanocrystals

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Cited by 55 publications
(99 citation statements)
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“…We highlight that the spectral position of the first excitonic absorption and luminescence peaks are essentially identical in the reference and CsPbBr 3 :NiO X PNCs samples, indicating that the electronic structure of the nanocrystal’s core is unaltered by the treatment, and that the bands alignment at the heterointerface does not cause exciton splitting, which is consistent with ∼1 monolayer thin NiO X coating. We finally notice that the PL spectrum of NiO X -treated PNCs is slightly blue-shifted with respect to the pristine PNCs, which is likely the consequence of the effective passivation of surface defect sites (likely halide vacancies) in agreement with recent literature. , …”
supporting
confidence: 90%
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“…We highlight that the spectral position of the first excitonic absorption and luminescence peaks are essentially identical in the reference and CsPbBr 3 :NiO X PNCs samples, indicating that the electronic structure of the nanocrystal’s core is unaltered by the treatment, and that the bands alignment at the heterointerface does not cause exciton splitting, which is consistent with ∼1 monolayer thin NiO X coating. We finally notice that the PL spectrum of NiO X -treated PNCs is slightly blue-shifted with respect to the pristine PNCs, which is likely the consequence of the effective passivation of surface defect sites (likely halide vacancies) in agreement with recent literature. , …”
supporting
confidence: 90%
“…We finally notice that the PL spectrum of NiO X -treated PNCs is slightly blue-shifted with respect to the pristine PNCs, which is likely the consequence of the effective passivation of surface defect sites (likely halide vacancies) in agreement with recent literature. 11,90 We then proceeded with experimentally validating the potential of the ultrathin emissive layer approach by fabricating and testing planar devices with the architecture shown in Figure 1a embedding an ultrathin PNC emissive layer (d = 10 nm). The cross-sectional TEM image is reported in Figure 3a, showing a continuous film of CsPbBr 3 :NiO X PNCs with clear interfaces.…”
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confidence: 99%
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“…Single crystals of this material were reported to tolerate different doses of γ rays of up to 8 kGy, but their optical and electrical properties change after a cumulative dose of >25 kGy . However, very recently it has been reported that CsPbI 3 nanocrystals could tolerate an “extreme dose” of γ rays approaching 1 MGy …”
mentioning
confidence: 99%
“…25 Zaffalon et al demonstrated an exceptionally stable scintillation efficiency of both CsPbBr 3 and CsPbBr 3 :F nanocrystals under an accumulated dose of 1 MGy. 26 The radioluminescence efficiency of CsPbBr 3 :F nanocrystals could retain their initial value while the photoluminescence quantum yield (PLQY) decreased by ∼30%. They contributed the excellent stability to the self-healing ability of the structural defects created by irradiation which has been observed in different perovskite material systems.…”
mentioning
confidence: 98%