2 research outputs found
Coupled Oscillators for Tuning Fluorescence Properties of Squaraine Dyes
Combining a squaraine (S) and a BODIPY
(B) chromophore in a heterodimer (SB) and two heterotrimers (BSB and
SBS) by alkyne bridges leads to the formation of coupled oscillators
whose fluorescence properties are superior compared to the parent
squaraine chromophore. The lowest energy absorption and emission properties
of these superchromophores are mainly governed by the squaraine part
and are shifted by more than 1000 cm<sup>–1</sup> to the red
by excitonic interaction between the squaraine and the BODIPY dye.
Employing polarization-dependent transient absorption and fluorescence
upconversion measurements, we could prove that the lowest energy absorption
in SB and BSB is caused by a single excitonic state but by two for
SBS. Despite the spectral red-shift of their lowest absorption band,
the fluorescence quantum yields increase for SB and BSB compared to
the parent squaraine chromophore SQA. This is caused by intensity
borrowing from the BODIPY states, which increases the squared transition
moments of the lowest energy band dramatically by 29% for SB and 63%
for BSB compared to SQA. Thereby, exciton coupling leads to a substantial
enhancement of fluorescence quantum yield by 26% for SB and by 46%
for BSB and shifts the emission from the red into the near-infrared.
In this way, the BODIPY-squaraine conjugates combine the best properties
of each class of dye. Thus, exciton coupling in heterodimers and -trimers
is a valuable alternative to tuning fluorescence properties by, e.g.,
attaching substituents to chromophores
Exciton Dynamics from Strong to Weak Coupling Limit Illustrated on a Series of Squaraine Dimers
We present a joint
theoretical and experimental study on the light-induced
exciton relaxation dynamics in a series of three squaraine dimers
spanning the range from weak to intermediate to strong excitonic coupling
strength regime. As revealed by transient-absorption spectroscopy
and mixed quantum-classical dynamics simulations that explicitly take
into account excitation by the laser pulse, three different types
of exciton dynamics could be observed, although the investigated systems
exhibit very similar spectral features. While in the strongly coupled
system (Frenkel limit), the exciton remains delocalized over both
dye monomers, in the system with intermediate coupling, transient
localization–delocalization on a femtosecond time scale can
be observed. Finally, in the weakly coupled heterodimer (Förster
limit), efficient exciton transfer, mediated by transient delocalization
that correlates with a strong nonadiabatic coupling, takes place.
By delivering the first systematic microscopic study on different
regimes of exciton transfer, our findings shed new light on the possible
mechanisms of energy transport in organic molecular excitonic materials