2023
DOI: 10.1016/j.jlumin.2023.120029
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Accessing blue-room-temperature phosphorescence from pyridine-fused extended coumarins

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Cited by 8 publications
(5 citation statements)
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“…In contrast, harvesting triplet excitons via room-temperature phosphorescence (RTP) from the lowest triplet (T1) state to the ground (S0) state has become an attractive alternative approach. Recently, many design principles that rely on intra- and/or intermolecular interactions, aggregates, , host–guest chemistry, excited-state engineering, halogen effect, ,, heavy chalcogen atom effect, and orthogonal donor–acceptor (D–A), ,,, biaryl, and donor–spacer–acceptor ,, geometries have been developed. Nevertheless, a handful of reports comprising chemical modification, mechanical force, , conformational switching, intramolecular CT, regioisomeric effect on the excited state, and change of host matrices have recently observed simultaneous TADF and RTP. , Despite these achievements, structure–property correlation in simultaneous thermally enhanced phosphorescence (TEP) and its impact on TADF remain unclear due to fast internal conversion and the supersensitive nature of the triplet excitons.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast, harvesting triplet excitons via room-temperature phosphorescence (RTP) from the lowest triplet (T1) state to the ground (S0) state has become an attractive alternative approach. Recently, many design principles that rely on intra- and/or intermolecular interactions, aggregates, , host–guest chemistry, excited-state engineering, halogen effect, ,, heavy chalcogen atom effect, and orthogonal donor–acceptor (D–A), ,,, biaryl, and donor–spacer–acceptor ,, geometries have been developed. Nevertheless, a handful of reports comprising chemical modification, mechanical force, , conformational switching, intramolecular CT, regioisomeric effect on the excited state, and change of host matrices have recently observed simultaneous TADF and RTP. , Despite these achievements, structure–property correlation in simultaneous thermally enhanced phosphorescence (TEP) and its impact on TADF remain unclear due to fast internal conversion and the supersensitive nature of the triplet excitons.…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, highest occupied and lowest unoccupied natural transition orbital (HONTO/LUNTO) analysis of the F1 revealed that both S1′ and T1′ show CT character, as the hole and electron wave functions are distributed over the long (fused rings) and short (TPN) axes of the molecular backbone (Figure b). Upon careful investigation of the hole and electron wave functions of T1′, we found a shift in electron density from the O atoms (long axis) toward the carbon and nitrogen atoms of the CN group (short axis), leading to nπ* character of the triplet state, which is effective in realizing efficient RTP . However, the ππ* character of the triplet state can also be realized from transition orbitals along the long axis of the molecular backbone.…”
Section: Resultsmentioning
confidence: 99%
“…Upon careful investigation of the hole and electron wave functions of T1′, we found a shift in electron density from the O atoms (long axis) toward the carbon and nitrogen atoms of the CN group (short axis), leading to nπ* character of the triplet state, which is effective in realizing efficient RTP. 25 However, the ππ* character of the triplet state can also be realized from transition orbitals along the long axis of the molecular backbone. Also, NTOs of both S1′ and T1′ states are almost similar, which implies a low SOC value between the two states, which hinders direct RISC from T1 to S1.…”
Section: Quantum Chemistry Analysismentioning
confidence: 99%
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“…However, achieving RTP (T1 → S0) is an exasperating task because phosphorescence is a quantum mechanically forbidden process that occurs at a meager rate. Numerous design principles that rely on aggregates, , host guest chemistry, , heavy atom effects, , orthogonal donor–acceptor (D–A), biaryl, D–spacer–A geometries, mechanical forces, conformational effects, , and inter/intramolecular charge transfer ,, have been overwhelmingly developed to observe RTP, where a low S1–T1 gap (Δ E ST ) is considered an essential prerequisite. However, achieving blue–violet RTP remains challenging.…”
mentioning
confidence: 99%