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Structural Disorder as the Origin of Optical Properties and Spectral Dynamics in Squaraine Nano-Aggregates

In contrast to regular J- and H-aggregates, thin film squaraine aggregates usually have broad absorption spectra containing both J-and H-like features, which are favorable for organic photovoltaics. Despite being successfully applied in organic photovoltaics for years, a clear interpretation of thes...

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Published in:Journal of the American Chemical Society 2022-10, Vol.144 (42), p.19372-19381
Main Authors: Bernhardt, Robin, Manrho, Marìck, Zablocki, Jennifer, Rieland, Lukas, Lützen, Arne, Schiek, Manuela, Meerholz, Klaus, Zhu, Jingyi, Jansen, Thomas L. C., Knoester, Jasper, van Loosdrecht, Paul H. M.
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cited_by cdi_FETCH-LOGICAL-a339t-aab53a2e97176274c19dd645d14cf1ba9bdd7dece6026526e6ca9a36fb75c49e3
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creator Bernhardt, Robin
Manrho, Marìck
Zablocki, Jennifer
Rieland, Lukas
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Meerholz, Klaus
Zhu, Jingyi
Jansen, Thomas L. C.
Knoester, Jasper
van Loosdrecht, Paul H. M.
description In contrast to regular J- and H-aggregates, thin film squaraine aggregates usually have broad absorption spectra containing both J-and H-like features, which are favorable for organic photovoltaics. Despite being successfully applied in organic photovoltaics for years, a clear interpretation of these optical properties by relating them to specific excited states and an underlying aggregate structure has not been made. In this work, by static and transient absorption spectroscopy on aggregated n-butyl anilino squaraines, we provide evidence that both the red- and blue-shifted peaks can be explained by assuming an ensemble of aggregates with intermolecular dipole–dipole resonance interactions and structural disorder deriving from the four different nearest neighbor alignmentsin sharp contrast to previous association of the peaks with intermolecular charge-transfer interactions. In our model, the next-nearest neighbor dipole–dipole interactions may be negative or positive, which leads to the occurrence of J- and H-like features in the absorption spectrum. Upon femtosecond pulse excitation of the aggregated sample, a transient absorption spectrum deviating from the absorbance spectrum emerges. The deviation finds its origin in the excitation of two-exciton states by the probe pulse. The lifetime of the exciton is confirmed by the band integral dynamics, featuring a single-exponential decay with a lifetime of 205 ps. Our results disclose the aggregated structure and the origin of red- and blue-shifted peaks and explain the absence of photoluminescence in squaraine thin films. Our findings underline the important role of structural disorder of molecular aggregates for photovoltaic applications.
doi_str_mv 10.1021/jacs.2c07064
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In this work, by static and transient absorption spectroscopy on aggregated n-butyl anilino squaraines, we provide evidence that both the red- and blue-shifted peaks can be explained by assuming an ensemble of aggregates with intermolecular dipole–dipole resonance interactions and structural disorder deriving from the four different nearest neighbor alignmentsin sharp contrast to previous association of the peaks with intermolecular charge-transfer interactions. In our model, the next-nearest neighbor dipole–dipole interactions may be negative or positive, which leads to the occurrence of J- and H-like features in the absorption spectrum. Upon femtosecond pulse excitation of the aggregated sample, a transient absorption spectrum deviating from the absorbance spectrum emerges. The deviation finds its origin in the excitation of two-exciton states by the probe pulse. 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title Structural Disorder as the Origin of Optical Properties and Spectral Dynamics in Squaraine Nano-Aggregates
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