2022
DOI: 10.1039/d1sc06867a
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Thermodynamic equilibrium between locally excited and charge-transfer states through thermally activated charge transfer in 1-(pyren-2′-yl)-o-carborane

Abstract: Reversible conversion between excited-states is key to many photophysical phenomena. We studied the equilibrium between LE and CT states by time-resolved and temperature-dependent fluorescence, fs- and ns-transient absorption, and LR-TDDFT calculations.

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Cited by 32 publications
(41 citation statements)
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“…In addition, in our analysis of the S 1 state, a new conformation corresponding to a pure CT character (the rightmost conformation in Figure 1 ) is revealed (vide infra) for the first time in the literature as a result of further elongation of the C 1 –C 2 bond. We also note that Ji et al 62 have shown the existence of a similar CT state (C 1 –C 2 = 2.62 Å) for a 1-(pyren-2-yl)- o -carborane system in a very recent study. In this work, this state is named as the S 1 -M (mixed) state, while the twisted confirmation for the 1-(pyren-2-yl)- o -carborane system is called S 1 -CT.…”
Section: Methodssupporting
confidence: 69%
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“…In addition, in our analysis of the S 1 state, a new conformation corresponding to a pure CT character (the rightmost conformation in Figure 1 ) is revealed (vide infra) for the first time in the literature as a result of further elongation of the C 1 –C 2 bond. We also note that Ji et al 62 have shown the existence of a similar CT state (C 1 –C 2 = 2.62 Å) for a 1-(pyren-2-yl)- o -carborane system in a very recent study. In this work, this state is named as the S 1 -M (mixed) state, while the twisted confirmation for the 1-(pyren-2-yl)- o -carborane system is called S 1 -CT.…”
Section: Methodssupporting
confidence: 69%
“…While this conformation exhibits a highly energetic S 0 point (1.48 eV as shown in Figure ), the calculated energy barriers on the S 1 surfaces are quite reasonable (0.3–0.4 eV), suggesting that the molecule can reach this geometry via electronic-vibronic couplings upon photoexcitation. In a very recent study, the existence of a similar CT state has also been confirmed for the 1-(pyren-2-yl)- o -carborane system, where the C 1 –C 2 bond length becomes 2.62 Å . In both cases, the energy gap between the S 0 and the S 1 surfaces becomes quite small around this point, which can further increase the nonradiative decay rate according to the energy gap law.…”
Section: Resultsmentioning
confidence: 59%
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“…As such, carboranes have been utilized as important building blocks to construct functional molecules and tunable pharmacophores (especially for Boron Neutron Capture Therapy (BNCT) drugs). Among these studies, carboranes are generally treated as an “appended” structural unit. However, it would be more interesting and distinct if carborane-embedded polycyclic systems would be developed with carborane playing a central role. In such a way, the carborane together with the extended part can serve as a new and united structural skeleton. So far, such a “cage extension strategy” to construct boron cluster-cored polycyclics is much less established in contrast to the classical extension of 2D aromatic rings.…”
Section: Introductionmentioning
confidence: 99%
“…Ortho -carborane can act as a multifunctional acceptor in charge transfer (CT) processes when connected to π-systems. 62–65 Additionally, carborane itself has been shown to lower the LUMO energy of boranes, especially when the p z orbital on boron aligns with the C1–C2 σ*-anti-bonding orbital. 48,66–68 A similar effect can be observed when the carborane is attached to boron via a conjugated π-system.…”
Section: Introductionmentioning
confidence: 99%