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Electronic Structure and Excited-State Dynamics of DNA-Templated Monomers and Aggregates of Asymmetric Polymethine Dyes.

Katelyn M DuncanHannah M ByersMadaline E HoudekSimon K RoyAustin BiaggneMatthew S BarclayLance K PattenJonathan S HuffDonald L KellisChristopher K WilsonJeunghoon LeePaul H DavisOlga A MassLan LiDaniel B TurnerJohn A HallWilliam B KnowltonBernard YurkeRyan D Pensack
Published in: The journal of physical chemistry. A (2023)
Aggregates of conjugated organic molecules (i.e., dyes) may exhibit relatively large one- and two-exciton interaction energies, which has motivated theoretical studies on their potential use in quantum information science (QIS). In practice, one way of realizing large one- and two-exciton interaction energies is by maximizing the transition dipole moment (μ) and difference static dipole moment (Δ d ) of the constituent dyes. In this work, we characterized the electronic structure and excited-state dynamics of monomers and aggregates of four asymmetric polymethine dyes templated via DNA. Using steady-state and time-resolved absorption and fluorescence spectroscopy along with quantum-chemical calculations, we found the asymmetric polymethine dye monomers exhibited a large μ, an appreciable Δ d , and a long excited-state lifetime (τ p ). We formed dimers of all four dyes and observed that one dye, Dy 754, displayed the strongest propensity for aggregation and exciton delocalization. Motivated by these results, we undertook a more comprehensive survey of Dy 754 dimer and tetramer aggregates using steady-state absorption and circular dichroism spectroscopy. Modeling these spectra revealed an appreciable excitonic hopping parameter ( J ). Lastly, we used femtosecond transient absorption spectroscopy to characterize τ p of the dimer and tetramer, which we observed to be exceedingly short. This work revealed that asymmetric polymethine dyes exhibited μ, Δ d , monomer τ p , and J values promising for QIS; however, further work is needed to overcome excited-state quenching and achieve long aggregate τ p .
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