Manipulating the excited states from charge-transfer to hybridized local and charge-transfer towards high-performance blue electroluminescence

[Display omitted] •The excited states of three blue emitters are manipulated from CT to HLCT.•Blue vacuum-evaporated HLCT OLEDs exhibit maximum EQE of 7.52%.•The solution-processed HLCT OLED shows a high maximum EQE of 6.49%.•Very low efficiency roll-offs of 0.8% and 3.7% at 100 and 1000 cd m−2 are...

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Veröffentlicht in:Chemical engineering journal (Lausanne, Switzerland : 1996) Switzerland : 1996), 2023-10, Vol.473, p.145295, Article 145295
Hauptverfasser: Jiang, He, Li, Hanlin, Qiu, Jiahao, Jin, Jibiao, Xi, Chunying, Tao, Peng, Zhang, Baohua, Ma, Dongge, Wong, Wai-Yeung
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Sprache:eng
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Zusammenfassung:[Display omitted] •The excited states of three blue emitters are manipulated from CT to HLCT.•Blue vacuum-evaporated HLCT OLEDs exhibit maximum EQE of 7.52%.•The solution-processed HLCT OLED shows a high maximum EQE of 6.49%.•Very low efficiency roll-offs of 0.8% and 3.7% at 100 and 1000 cd m−2 are achieved. Manipulating the excited states of organic luminescent materials can efficiently improve the utilization of both singlet and triplet excitons for developing high-performance organic light-emitting diodes (OLEDs), but the issue remains difficult due to the lack of well-controlled ways. Here, we proposed a molecular design strategy of excited state manipulation from charge-transfer (CT) to hybridized local and charge-transfer (HLCT) via adjusting the cyano position on pyridine acceptor. The meta-substituted PyAn4CN is mainly composed of a CT component, while the para-substituted PyAn5CN is endowed with a HLCT component. On further extending the conjugation of PyAn5CN by inserting a benzene unit between the pyrene and anthracene core, the HLCT character is preserved in PyPhAn5CN, accompanied by a faster radiative decay. Consequently, the vacuum-evaporated OLEDs exhibit blue electroluminescence (EL) with the emission peaks in the range of 455–460 nm and high external quantum efficiency (EQE) up to 7.52%, together with well-suppressed efficiency roll-offs of 0.8% and 3.7% at the luminance of 100 and 1000 cd m-2, respectively. More importantly, the solution-processed device shows an excellent performance with EQE of 6.49%, which is one of the best results in the solution-processed HLCT OLEDs. Our results clearly indicate that the formation of HLCT state is an efficient way to realize high-efficiency blue electrofluorescence.
ISSN:1385-8947
1873-3212
DOI:10.1016/j.cej.2023.145295