posted on 2014-12-11, 00:00authored byYonghong Deng, Wen Yuan, Zhe Jia, Gao Liu
Understanding
of H- and J-aggregation behaviors in fluorene-based polymers is significant
both for determining the origin of various red-shifted emissions occurring
in blue-emitting polyfluorenes and for developing polyfluorene-based
device performance. In this contribution, we demonstrate a new theory
of the H- and J-aggregation of polyfluorenes and oligofluorenes, and
understand the influence of chromosphere aggregation on their photoluminescent
properties. H- and J-aggregates are induced by a continuous increasing
concentration of the oligofluorene or polyfluorene solution. A relaxed
molecular configuration is simulated to illustrate the spatial arrangement
of the bonding of fluorenes. It is indicated that the relaxed state
adopts a 21 helical backbone conformation with a torsion
angle of 18° between two connected repeat units. This configuration
makes the formation of H- and J-aggregates through the strong π–π
interaction between the backbone rings. A critical aggregation concentration
is observed to form H- and J-aggregates for both polyfluorenes and
oligofluorenes. These aggregates show large spectral shifts and distinct
shape changes in photoluminescent excitation (PLE) and emission (PL)
spectroscopy. Compared with “isolated” chromophores,
H-aggregates induce absorption spectral blue-shift and fluorescence
spectral red-shift but largely reduce fluorescence efficiency. “Isolated”
chromophores not only refer to “isolated molecules”
but also include those associated molecules if their conjugated backbones
are not compact enough to exhibit perturbed absorption and emission.
J-aggregates induce absorption spectral red-shift and fluorescence
spectral red-shift but largely enhance fluorescence efficiency. The
PLE and PL spectra also show that J-aggregates dominate in concentrated
solutions. Different from the excimers, the H- and J-aggregate formation
changes the ground-state absorption of fluorene-based chromophores.
H- and J-aggregates show changeable absorption and emission derived
from various interchain interactions, unlike the β phase, which
has relatively fixed absorption and emission derived from an intrachain
interaction.