2015
DOI: 10.1021/acs.jpca.5b08640
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Ultrafast Electronic Energy Transfer Beyond the Weak Coupling Limit in a Proximal but Orthogonal Molecular Dyad

Abstract: Electronic energy transfer (EET) from a donor to an acceptor is an important mechanism that controls the light harvesting efficiency in a wide variety of systems, including artificial and natural photosynthesis and contemporary photovoltaic technologies. The detailed mechanism of EET at short distances or large angles between the donor and acceptor is poorly understood. Here the influence of the orientation between the donor and acceptor on EET is explored using a molecule with two nearly perpendicular chromop… Show more

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Cited by 24 publications
(32 citation statements)
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References 39 publications
(70 reference statements)
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“…The absolute absorption of T4 is in good agreement with experiment, the absolute absorption for BOD is slightly too low compared to experiment as the broadening is slightly overestimated. 15 Overall, the absorption for the two peaks of BODT4 is dominated by the absorption of the corresponding building blocks. It remains similar in shape and is slightly red-shifted.…”
Section: 47mentioning
confidence: 97%
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“…The absolute absorption of T4 is in good agreement with experiment, the absolute absorption for BOD is slightly too low compared to experiment as the broadening is slightly overestimated. 15 Overall, the absorption for the two peaks of BODT4 is dominated by the absorption of the corresponding building blocks. It remains similar in shape and is slightly red-shifted.…”
Section: 47mentioning
confidence: 97%
“…15 In this system with orthogonal orientation between acceptor and donor unit and strong electronic coupling, simplified models as discussed above are not applicable to understand the origin or characteristics of the EET following photoexcitation. In our experiments, the ultrafast molecular dynamics following excitation is analyzed based on time-resolved fluorescence depolarization, a powerful tool to understand relaxation processes in molecular systems.…”
Section: -13mentioning
confidence: 99%
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“…Taking the shorter of the two lifetimes as reflecting the bulk molecules, we can estimate that, on average, 50 % of the excitons will undergo at least 400 hops before returning to the ground state whereas 10 % will make at least 1,400 hops. Of course, any such migration will be incoherent and it should be stressed that the Coulombic mechanism usually underestimates the hopping time at very short separations . The mean time needed for an exciton to cross between stacks is 50±8 ps.…”
Section: Resultsmentioning
confidence: 87%