2018
DOI: 10.1039/c8ra07891b
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Hot exciton transition for organic light-emitting diodes: tailoring excited-state properties and electroluminescence performances of donor–spacer–acceptor molecules

Abstract: SPNCN-Cz device exhibits ηex (3.15%), ηc (2.56 cd A−1), ηp (2.45 lm W−1) with CIE (0.15, 0.07).

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Cited by 20 publications
(12 citation statements)
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References 95 publications
(68 reference statements)
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“…52 As seen, o-2CzBT, m-2CzBT, and p-2CzBT present two independent slopes, and the lower slope in low-polarity solvents is ascribed to the LE state while the larger slope in high-polarity solvents is attributed to the CT state, which is a typical behavior of HLCT materials. 32,[53][54][55] Therefore, based on the aforementioned theoretical calculations (electronic structures and properties of excited states) and photophysical studies (nanosecond-scaled lifetimes and solvatochromic effects), the HLCT feature is verified for o-2CzBT, m-2CzBT, and p-2CzBT through the coupling and intercrossing between the LE and CT states. 56…”
Section: Photophysical Propertiesmentioning
confidence: 98%
“…52 As seen, o-2CzBT, m-2CzBT, and p-2CzBT present two independent slopes, and the lower slope in low-polarity solvents is ascribed to the LE state while the larger slope in high-polarity solvents is attributed to the CT state, which is a typical behavior of HLCT materials. 32,[53][54][55] Therefore, based on the aforementioned theoretical calculations (electronic structures and properties of excited states) and photophysical studies (nanosecond-scaled lifetimes and solvatochromic effects), the HLCT feature is verified for o-2CzBT, m-2CzBT, and p-2CzBT through the coupling and intercrossing between the LE and CT states. 56…”
Section: Photophysical Propertiesmentioning
confidence: 98%
“…While 2EHO-CNPE retains the LE-dominated HLCT behavior in this high polarity region, 2EHO-TPA-CNPE and 2EHO-TPA-PE OPE π-systems showed much larger slopes (∼27 170−29 700) in the Lippert−Mattaga model yielding very large μ e 's of 33.1−35.3 D. Note that these significantly large μ e values are on the order of some of the highest excited state dipole moments predicted for CT compounds in the literature. 59,60 Considering that 2EHO-TPA-PE and 2EHO-TPA-CNPE molecular lengths are ∼3.55 nm, these μ e 's correspond to a large degree of charge separation (∼0.70−0.75 charge•nm) along the molecular π-backbone. These findings reveal that in low-to-medium polarity region there is a common LE-dominant HLCT excited state character for all three OPE molecules.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…Researchers have used the styryl moiety as a spacer in the design strategy of the molecular structure, and it will increase the twisting nature of the molecules, and more twisting nature of the molecules push emission toward lower wavelength, due to restricting p-conjugation in the molecules. [126][127][128][129] In 2017, V. Thanikachalam et al designed and synthesized three blueemitting fluorophores, TPA-BDIS 74, TPA-BPIS 75, and Cz-BPIS 76, by connecting donor TPA/Cz and acceptor BI/PI through the styryl as a spacer (Fig. 21).…”
Section: Phenanthroimidazole-styryl Spacer Based Hlct Fluorophoresmentioning
confidence: 99%