Herein, we report the cocrystals
of an AIEgenic tetraphenol, namely
tetrakis(4-hydroxybiphenyl)ethylene (THBPE), with a few bispyridyl
aza donors, built with phenol···pyridine hydrogen bonding.
We employed two different crystallization conditions: diffusion of
hexane into THF and slow evaporation from ethyl acetate. The former
condition readily afforded cocrystals in all instances except one,
whereas the latter afforded only one. Attempted cocrystallization
with 4,4′-bipyridine (BP) did not result in any cocrystals
but instead afforded THF solvates of the tetraphenol. The rigid coformers
4,4′-azopyridine (AP) and 1,2-bis(4-pyridyl)ethylene (BPE)
resulted in nonemissive close-packed cocrystal solvates. In both cases,
the THF solvent competes with the pyridyl moiety for hydrogen bonding
at two of the four possible sites in the tetraphenol, which is uncommon
for a phenol···pyridine supramolecular synthon. However,
the synthon wins out in the crystals from ethyl acetate solution with
one coformer (AP) to form a fully hydrogen bonded square lattice (
sql
) network. The moderately flexible 1,2-bis(4-pyridyl)ethane
(BPA) led to a close-packed hydrated cocrystal solvate. The highly
flexible 1,2-bis(4-pyridyl)propane (BPP) afforded emissive cocrystals,
with nanotubular pores of 10 Å diameter. The latter cocrystal
adopts a
qtz
topology with 8-fold interpenetration.
The last two cocrystals are emissive in the solid state, which is
unusual for phenol···pyridine hydrogen-bonded complexes.
The quantum yields of the solid-state emission exhibited by the lastlatter
two cocrystals are 16% and 25%, which are higher than that of the
tetraphenol at 9%. The observed emission property can be correlated
with how uniquely and efficiently the AIEgens are packed in the solid
with the assistance of coformers. The cocrystallization experiments
with rigid tetraphenol and diverse bispyridyl coformers also provide
insight into the formation of cocrystals along with solvates and hydrated
solvates. Notably, four among the five cocrystals reported herein
have Z′ = 2.