1981
DOI: 10.1016/0009-2614(81)85280-3
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Radiationless transitions in electron donor-acceptor complexes: selection rules for S1 → T intersystem crossing and efficiency of S1 → S0 internal conversion

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Cited by 93 publications
(107 citation statements)
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“…[4][5][6][7][8][9] One way to improve the TADF emission contribution is to minimize the energy splitting (∆E ST ) between singlet and triplet states. Recent experimental studies [10][11][12] along with initial theoretical work [13][14][15] identify that the SOC mechanism in these TADF systems is a complex second order process requiring vibronic coupling between 3 CT and 3 LE to mediate the spin flip back to the 1 CT state, the 3 LE state mediates the SOC between the singlet and triplet CT states 15 . Hence whereas the CT states are very sensitive to the local enviroment 10 the local triplet states are not, therefore the host differential effects the energy gaps which directly changes the rate of reverse intersystem crossing (rISC).…”
Section: Toc Graphics Abstract Blue Oled Tadf Mechanism Charge Tranmentioning
confidence: 99%
“…[4][5][6][7][8][9] One way to improve the TADF emission contribution is to minimize the energy splitting (∆E ST ) between singlet and triplet states. Recent experimental studies [10][11][12] along with initial theoretical work [13][14][15] identify that the SOC mechanism in these TADF systems is a complex second order process requiring vibronic coupling between 3 CT and 3 LE to mediate the spin flip back to the 1 CT state, the 3 LE state mediates the SOC between the singlet and triplet CT states 15 . Hence whereas the CT states are very sensitive to the local enviroment 10 the local triplet states are not, therefore the host differential effects the energy gaps which directly changes the rate of reverse intersystem crossing (rISC).…”
Section: Toc Graphics Abstract Blue Oled Tadf Mechanism Charge Tranmentioning
confidence: 99%
“…Previous work has shown that in the one-electron approximation, intersystem crossing due to spin orbit coupling between the singlet charge transfer state ( 1 CT) and a locally triplet excited state ( 3 LE) is of fundamental importance to harvest triplet states, since the interconversion between the 1 CT and 3 CT states is often not efficient. 10,11 However, the presence of a local triplet energetically close to the CT manifold will strongly influence the efficiency of the TADF mechanism through charge transfer spin orbit coupling. Here, we explore the energy alignment between the CT manifold and a local triplet excited state in order to maximize the reverse intersystem crossing in a phenothiazine-dibenzothiophene-S,S-dioxide molecule, so this emitter can be used to design polymer materials showing efficient TADF emission in their pristine films.…”
Section: Introductionmentioning
confidence: 99%
“…1 However, this process is formerly forbidden for perpendicular HOMO and LUMO orbitals, which is the case in PTZ-DBTO2, due to unfavourable spin-orbit coupling (SOC) and Franck-Condon factors. 10,11,23 However, crossing between the 1 CT state and an energetically close local triplet state is efficient, as was shown by Dance et al 24 Hyperfine coupling (HFC) can in principle interconvert 1 CT to 3 CT and back. 25,26 However the exchange energy, i.e.…”
mentioning
confidence: 96%
“…Spin orbit coupling (SOC) for example is formally forbidden between singlet and triplet CT states for the case of near orthogonal D and A units, and thus the 1 CT state can only couple strongly to a close lying local triplet state. 13,14 The gap between these two states is thus the real ∆EST that requires thermal energy for triplets to cross over to the singlet state. These means that 1 CT can be either above or below the coupling triplet state for TADF to occur, but needs to be close to a local triplet state, so efficient SOC can occur.…”
Section: Introductionmentioning
confidence: 99%