2023
DOI: 10.1021/acs.jpclett.2c03425
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Uncovering the Mechanism of Thermally Activated Delayed Fluorescence in Coplanar Emitters Using Potential Energy Surface Analysis

Abstract: Planarized emitters exhibiting thermally activated delayed fluorescence (TADF) have attracted attention due to their narrow emission spectra, improved photostability, and high quantum yields, but with large singlet–triplet energy gaps (ΔE ST ) and no heavy atoms, the origin of their TADF remains a subject of debate. Here we prepare two isomeric, coplanar donor–acceptor compounds, with HMAT-2PYM performing dual TADF and room-temperature phosphorescence but with HMAT-4PYM exhibiting only prompt fluorescence. Al… Show more

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Cited by 14 publications
(11 citation statements)
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“…As displayed in Figure , the intramolecular C–H···N distances between the pteridine core and the phenyl linkers range from 2.28 to 2.67 Å, which are shorter than the sum of the van der Waals radii of the hydrogen (H) and nitrogen (N) atoms. Additionally, the C–H–N angles fall between 100 and 124°. These observations suggest the presence of weak intramolecular C–H···N interactions, including H-bonding and van der Waals interactions (vide infra, Theoretical Calculations section), which can rigidify the molecular conformation and restrict the rotational and vibrational motions, thus being conducive to reducing the nonradiative decays of these materials. , Meanwhile, these intramolecular noncovalent interactions, together with the lack of steric hindrance, , result in relatively small torsion angles between the pteridine electron-acceptor and the bridging phenyl rings, which would extend the π-conjugation of the acceptor fragment and be in favor of realizing efficient intramolecular charge transfer. , In contrast to the non-planar diphenylamine donor units of TPA-PT, the rigid dimethylacridine donor units of DMAC-PT ensure large D–A twist angles (θ 3 = 86.24°, θ 4 = 88.19°) via the steric repulsion between the α-position H atoms. The nearly orthogonal D–A configuration is expected to afford an effective separation of the frontier molecular orbital (FMO) distribution and hence a relatively small Δ E ST .…”
Section: Resultsmentioning
confidence: 99%
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“…As displayed in Figure , the intramolecular C–H···N distances between the pteridine core and the phenyl linkers range from 2.28 to 2.67 Å, which are shorter than the sum of the van der Waals radii of the hydrogen (H) and nitrogen (N) atoms. Additionally, the C–H–N angles fall between 100 and 124°. These observations suggest the presence of weak intramolecular C–H···N interactions, including H-bonding and van der Waals interactions (vide infra, Theoretical Calculations section), which can rigidify the molecular conformation and restrict the rotational and vibrational motions, thus being conducive to reducing the nonradiative decays of these materials. , Meanwhile, these intramolecular noncovalent interactions, together with the lack of steric hindrance, , result in relatively small torsion angles between the pteridine electron-acceptor and the bridging phenyl rings, which would extend the π-conjugation of the acceptor fragment and be in favor of realizing efficient intramolecular charge transfer. , In contrast to the non-planar diphenylamine donor units of TPA-PT, the rigid dimethylacridine donor units of DMAC-PT ensure large D–A twist angles (θ 3 = 86.24°, θ 4 = 88.19°) via the steric repulsion between the α-position H atoms. The nearly orthogonal D–A configuration is expected to afford an effective separation of the frontier molecular orbital (FMO) distribution and hence a relatively small Δ E ST .…”
Section: Resultsmentioning
confidence: 99%
“…These observations suggest the presence of weak intramolecular C−H•••N interactions, including H-bonding 38 and van der Waals interactions (vide infra, Theoretical Calculations section), which can rigidify the molecular conformation and restrict the rotational and vibrational motions, thus being conducive to reducing the nonradiative decays of these materials. 39,40 Meanwhile, these intramolecular noncovalent interactions, together with the lack of steric hindrance, 33,34 result in relatively small torsion angles between the pteridine electronacceptor and the bridging phenyl rings, which would extend the π-conjugation of the acceptor fragment and be in favor of realizing efficient intramolecular charge transfer. 41,42 In contrast to the non-planar diphenylamine donor units of TPA-PT, the rigid dimethylacridine donor units of DMAC-PT ensure large D−A twist angles (θ 3 = 86.24°, θ 4 = 88.19°) via the steric repulsion between the α-position H atoms.…”
Section: Synthesis and Characterizationsmentioning
confidence: 99%
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“… Suppression of unwanted nonradiative pathways would lead to efficient room-temperature phosphorescence (RTP) or TADF, depending on these specific molecular features mentioned above. Both these phenomena have vital significance in optical devices. To achieve a high RISC rate ( k RISC ) in conventional TADF emitters, a well-known strategy for lowering the HOMO–LUMO overlap integral and, therefore, a low Δ E S–T has been commonly followed. Fine-tuning the k RISC by utilizing the hybrid electronic states of suitable energy has also been successful in achieving efficient TADF emitters. The singlet–triplet energy offset (Δ E S–T ) and the SOC matrix element of these states drive the forward and backward spin-flip processes (ISC and RISC). Rates of various nonradiative deactivation pathways of triplet excitons are also crucial for deciding the overall quantum yields (QYs) of the TADF or phosphorescence. , The functional features of RTP and TADF span from efficient lighting devices to metal-free photocatalysis for organic transformations that warrant precise engineering of the energy levels. , The spin-forbidden nature of the T 1 → S 0 transitions results in longer emission lifetimes of the order of ms that can be further extended to the order of seconds to exhibit ultralong RTP. , Likewise, the rate of delayed fluorescence ( k d ) is controlled by the energy offset of triplet states and singlet manifold and consequently is a competing process to the RTP ( k r T ) . A systematic experimental approach and design strategy are necessary to attain molecules of selective emission pathways from the triplet states. , …”
Section: Introductionmentioning
confidence: 99%