2022
DOI: 10.1039/d2tc00877g
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Novel deep-blue hot exciton material for high-efficiency nondoped organic light-emitting diodes

Abstract: The reverse intersystem crossing (RISC) process conducted from high-energy triplet states (Tn, n ≥ 2) to singlet state (Sm, m ≥ 1), termed as hot exciton process, has been confirmed...

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Cited by 15 publications
(7 citation statements)
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“…For the past several years, a series of anthracene‐based blue “hot exciton” materials have been reported. [ 13 ] As shown in Figure , the anthracene core has a delicate alignment of energy levels, which is beneficial to the hRISC process. The introductions of proper donors or acceptors to anthracene could further modulate the excited‐state properties, such as the transition orbital characters of T n and S m states and the S m – T n energy gap, which promote the hRISC process.…”
Section: Introductionmentioning
confidence: 99%
“…For the past several years, a series of anthracene‐based blue “hot exciton” materials have been reported. [ 13 ] As shown in Figure , the anthracene core has a delicate alignment of energy levels, which is beneficial to the hRISC process. The introductions of proper donors or acceptors to anthracene could further modulate the excited‐state properties, such as the transition orbital characters of T n and S m states and the S m – T n energy gap, which promote the hRISC process.…”
Section: Introductionmentioning
confidence: 99%
“…[15] In traditional TADF, the reverse intersystem crossing rate (RISC) occurs from the first excited low-lying triplet state T 1 to the singlet state S 1 , but in the "hot exciton" mechanism the RISC occurs perhaps not from the low-lying triplet, it also occurs from higher excited triplet states. [16,17] Considerably, in conventional TADF emitter, the mechanism involves the transition from the (S 1 -T 1 ) state which is referred to as "cold exciton". [18] In contrast, the "hot exciton" mechanism follows the conversion from the higher-lying triplet, (T n , n > 2) states and singlet (S m , m > 1) states.…”
Section: Introductionmentioning
confidence: 99%
“…However, the IQE in these hot exciton materials is still far from the upper limitation of 100% because the EUE and PLQY cannot reach 100% simultaneously (see Figure S1). , Namely, these empirical rules hardly produce an excellent IQE for hot exciton materials, owing to the rudimentary understanding of the EUE and PLQY. Therefore, it is urgent to unravel the underlying mechanisms and establish theoretical rules to promote the IQE of hot exciton materials.…”
Section: Introductionmentioning
confidence: 99%