2020
DOI: 10.1016/j.mattod.2019.10.021
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Perovskite nanostructures: Leveraging quantum effects to challenge optoelectronic limits

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Cited by 30 publications
(27 citation statements)
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References 233 publications
(303 reference statements)
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“…The optical studies of perovskite NC ensembles are valuable in guiding their efficient applications in classical optoelectronic devices, the current status of which has been detailed in several recent reviews. 73,74 At the single-particle level, the perovskite NCs are associated with unique single-photon emission characteristics and exciton fine structures, which have outlined a prospective route toward their potential usage in quantum information technologies.…”
mentioning
confidence: 99%
“…The optical studies of perovskite NC ensembles are valuable in guiding their efficient applications in classical optoelectronic devices, the current status of which has been detailed in several recent reviews. 73,74 At the single-particle level, the perovskite NCs are associated with unique single-photon emission characteristics and exciton fine structures, which have outlined a prospective route toward their potential usage in quantum information technologies.…”
mentioning
confidence: 99%
“…Solution-processed quasi-2D or mixed 3D-2D perovskite structures are already proved to be a potential material for light-emitting applications due to their quantum well structures enable efficient recombination of charge carriers into the 3D perovskites, enhancing the PL intensity, and crystal stability. [41][42][43] In a similar way, thermally evaporated quasi-2D perovskite films were utilized as an active layer in PeLEDs to further improve the device performance. [56] The PbBr 2 films were vacuum deposited on top of ITO-coated glass substrates (covered with spin-coated PEDOT : PSS layer) at a chamber pressure of 2 × 10 À 6 Torr.…”
Section: Green-emitting Peledsmentioning
confidence: 99%
“…But the optical properties of the APbI 3 perovskites slightly modify with the exchange in A ‐site cations, as the bandgap varies in this order of MA + (1.55 eV)> Cs + (1.5 eV)>FA + (1.45 eV), though the ionic radii of A ‐site cation ( Cs + , MA + , or FA + ) varies rapidly in the range of 1.8–2.5 Å [39,40] . The density functional theory (DFT) calculations revealed that the A ‐site cations do not contribute much to the electronic states close to the band edges [41] . This small variation in the bandgap energy has resulted from the change in the crystal lattice parameter after cation exchange.…”
Section: Characteristics Of Mhpsmentioning
confidence: 99%
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