2022
DOI: 10.1002/advs.202201807
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Narrowing the Phase Distribution of Quasi‐2D Perovskites for Stable Deep‐Blue Electroluminescence

Abstract: Solution‐processed quasi‐2D perovskites contain multiple quantum wells with a broad width distribution. Inhomogeneity results in the charge funneling into the smallest bandgap components, which hinders deep‐blue emission and accelerates Auger recombination. Here, a synthetic strategy applied to a range of quasi‐2D perovskite systems is reported, that significantly narrows the quantum well dispersity. It is shown that the phase distribution in the perovskite film is significantly narrowed with controlled, simul… Show more

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Cited by 30 publications
(33 citation statements)
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References 35 publications
(34 reference statements)
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“…Notably the energy funneling process is critical in quasi‐2D perovskite films. [ 29 ] The PL of low‐dimensional phases during energy funneling leads to the asymmetry of the PL shape. [ 30 ] The transient absorption spectra demonstrated the existence of an energy transfer process (Figure S2, Supporting Information).…”
Section: Resultsmentioning
confidence: 99%
“…Notably the energy funneling process is critical in quasi‐2D perovskite films. [ 29 ] The PL of low‐dimensional phases during energy funneling leads to the asymmetry of the PL shape. [ 30 ] The transient absorption spectra demonstrated the existence of an energy transfer process (Figure S2, Supporting Information).…”
Section: Resultsmentioning
confidence: 99%
“…[26][27][28] As a result, the blue PeLEDs with a broad n distribution are often subjected to low color purity and efficiency, therefore, narrow n distribution with minimized n = 1 and high-n phases in perovskites are mostly desired. [29] As the monodispersity of quantum wells is highly dependent on the spatial homogeneous distribution of organic cations in the precursor solution, [21,30] another different ammonium cations have been introduced to compete with PEA + to occupy the allocated positions in the perovskite lattice, which can disturb the PEA + aggregates and thus suppression of low n phases, such as PEAI/3-fluorophenylethylammonium iodide (m-F-PEA) and 1-naphthylmethylammonium iodide (NMAI), [10] PEABr and iso-propylammonium bromide (IPABr), [31][32] etc. In addition, introducing Lewis base additives into perovskites has become one of the most effective strategies to passivate defects and retard the growth of high-n domains via the coordination interaction.…”
Section: Introductionmentioning
confidence: 99%
“…Figure 5b shows the EL spectra under forward bias of 3.4, 3.8, and 4.2 V. The EL peak is located at 442 nm with an fwhm of 13 nm, which is one of the narrowest fwhm report to date among deep-blue perovskite EL devices. 43 This confirms that large-n domains are eliminated, and the phase purity of n = 2 perovskites is significantly increased. The corresponding Commission Internationale de l'Eclairage (CIE) color coordinate is (0.16, 0.02).…”
Section: ■ Results and Discussionmentioning
confidence: 55%
“…On the basis of the pure-phase 2D film, we fabricated EL devices using the following structure (Figure a): ITO/PEDOT:PSS/PVK/perovskite/TPBi/LiF/Al. Figure b shows the EL spectra under forward bias of 3.4, 3.8, and 4.2 V. The EL peak is located at 442 nm with an fwhm of 13 nm, which is one of the narrowest fwhm report to date among deep-blue perovskite EL devices . This confirms that large- n domains are eliminated, and the phase purity of n = 2 perovskites is significantly increased.…”
Section: Resultsmentioning
confidence: 62%