2023
DOI: 10.1016/j.xcrp.2022.101245
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The El-Sayed’s rule analogy enables long-lived room temperature phosphorescence in twisted biphenyls

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Cited by 14 publications
(14 citation statements)
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“…The latter rule suggests that the change in spin multiplicity is intriguingly coupled to a change in orbital symmetry in order to conserve the total angular momentum in the exciton transfer process. In fact, excited states with different wave function spatial symmetry leading to large SOC was well illustrated in several earlier studies. , This essentially leads to a large SOC for S 1 → T 2 ISC in Az-CHS and, thereby, resulting in a very high S 1 ( n π*) → T 2 (ππ*) ISC of k ISC ∼10 9 s –1 (see SOC and ISC rates from Figure ). Importantly, an in-plane vibration with mode-frequency similar to ω eff of 1407 cm –1 associated with a large Huang–Rhys factor is identified to drive the exciton transfer.…”
Section: Resultssupporting
confidence: 67%
“…The latter rule suggests that the change in spin multiplicity is intriguingly coupled to a change in orbital symmetry in order to conserve the total angular momentum in the exciton transfer process. In fact, excited states with different wave function spatial symmetry leading to large SOC was well illustrated in several earlier studies. , This essentially leads to a large SOC for S 1 → T 2 ISC in Az-CHS and, thereby, resulting in a very high S 1 ( n π*) → T 2 (ππ*) ISC of k ISC ∼10 9 s –1 (see SOC and ISC rates from Figure ). Importantly, an in-plane vibration with mode-frequency similar to ω eff of 1407 cm –1 associated with a large Huang–Rhys factor is identified to drive the exciton transfer.…”
Section: Resultssupporting
confidence: 67%
“…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 Figure S25, it is shown that the HOMO and HOMO–1 have degenerated consisting of lone pair (n) electrons of C atoms of carbene and N atoms of pyridine, together with d electrons of Cu 3 and π electrons in the N–C–N moieties in the five-member rings; while the electron density of LUMO delocalizes on Cu 3 (s, p orbital) and N–C–N (π* orbital) moieties. Thus, the different electronic configurations would possess effective SOC channels between the low-lying excited states. , …”
Section: Resultsmentioning
confidence: 99%
“…Thus, the different electronic configurations would possess effective SOC channels between the low-lying excited states. 74,75 Furthermore, the phosphorescence wavelength was calculated by the energy difference between T 1 and the relaxation energy at the singlet energy surface (S 0 ). Indeed, at the PBE0/ def2-SVP theoretical level, the calculated phosphorescence wavelength is 459 nm, fitting well with the experimental value (456 nm).…”
Section: ■ Introductionmentioning
confidence: 99%