In understanding the mechanism of aggregation-induced
emission
(AIE), the multilevel ONIOM framework has been demonstrated as one
of the efficient tools that can capture the essential mechanistic
information by choosing a single fluorophore as the quantum mechanics
(QM) model and putting all surrounding molecules in the low-level
region. Recently, the ionic styryl-pyridine salt (namely, SPH) has
been reported as a new class of AIEgen with a high fluorescence yield.
In the SPH crystal, a pair of ionic SPH molecules are closely stacked
with each other in an antiparallel, head-to-tail pattern, thus the
choice of QM models (an individual or dimeric structure) becomes critical
in the ONIOM study. Herein we report the AIE mechanism of the ionic
SPH at the QM ((TD)-CAM-B3LYP) and ONIOM(QM:MM) levels. As usual,
the fluorescence quenching of SPH in tetrahydrofuran (THF) solution
is attributed to a nonradiative relaxation via the central CC
bond rotation, with a rather low barrier of 2.7 kcal/mol. In crystals,
either with a monomer or dimer model, the fluorescence quenching channel
is found to be restricted due to the obvious CC rotation barriers.
Compared with the monomer model, the dimer model, by treating the
orbital interaction of the two SPH molecules at the QM level, provides
significantly increased barriers and a red-shifted emission wavelength
that better matches the experimental value. In addition, the calculated
exciton coupling in the fluorescence emission state can be discovered
only by a dimer model. The findings here emphasize not only the importance
of choosing a proper model in the ONIOM study of AIE but also expanding
our understanding of novel AIE systems.