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Efficient Ruddlesden-Popper Perovskite Light-Emitting Diodes with Randomly Oriented Nanocrystals

Authors
Lee, Hyeon-DongKim, HobeomCho, HimchanCha, WonheeHong, YongseokKim, Young-HoonSadhanala, AdityaVenugopalan, VijayKim, Joo SungChoi, Jin WooLee, Chang-LyoulKim, DonghoYang, HoichangFriend, Richard H.Lee, Tae-Woo
Issue Date
Jul-2019
Publisher
WILEY-V C H VERLAG GMBH
Keywords
carrier transport; nanocrystal orientation; nanocrystal pinning; quasi-2D perovskite; structural modulation
Citation
ADVANCED FUNCTIONAL MATERIALS, v.29, no.27, pp.1 - 9
Indexed
SCIE
SCOPUS
Journal Title
ADVANCED FUNCTIONAL MATERIALS
Volume
29
Number
27
Start Page
1
End Page
9
URI
https://scholarworks.bwise.kr/hanyang/handle/2021.sw.hanyang/189748
DOI
10.1002/adfm.201901225
ISSN
1616-301X
Abstract
Ruddlesden-Popper phase (RP-phase) perovskites that consist of 2D perovskite slabs interleaved with bulky organic ammonium (OA) are favorable for light-emitting diodes (LEDs). The critical limitation of LED applications is that the insulating OA arranged in a preferred orientation limits charge transport. Therefore, the ideal solution is to achieve a randomly connected structure that can improve charge transport without hampering the confinement of the electron-hole pair. Here, a structurally modulated RP-phase metal halide perovskite (MHP), (PEA)(2)(CH3NH3)(m-1)PbmBr3m+1 is introduced to make the randomly oriented RP-phase unit and ensure good connection between them by applying modified nanocrystal pinning, which leads to an increase in the efficiency of perovskite LEDs (PeLEDs). The randomly connected RP-phase MHP forces contact between inorganic layers and thereby yields efficient charge transport and radiative recombination. Combined with an optimal dimensionality, (PEA)(2)(CH3NH3)(2)Pb3Br10, the structurally modulated RP-phase MHP exhibits increased photoluminescence quantum efficiency, from 0.35% to 30.3%, and their PeLEDs show a 2,018 times higher current efficiency (20.18 cd A(-1)) than in the 2D PeLED (0.01 cd A(-1)) and 673 times than in the 3D PeLED (0.03 cd A(-1)) using the same film formation process. This approach provides insight on how to solve the limitation of RP-phase MHP for efficient PeLEDs.
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