Null
aggregates are an elusive, emergent class of molecular assembly
categorized as spectroscopically uncoupled molecules. Orthogonally
stacked chromophoric arrays are considered as a highlighted architecture
for null aggregates. Herein, we unveil the null exciton character in a series of crystalline Greek
cross (+)-assembly of 6,13-bisaryl-substituted pentacene derivatives.
Quantum chemical computations suggest that the synergistic perpendicular
orientation and significant interchromophoric separations realize
negligible long-range Coulombic and short-range charge-transfer-mediated
couplings in the null aggregate. The Greek cross (+)-orientation of
pentacene dimers exhibits a selectively higher electron-transfer coupling
with near-zero hole-transfer coupling and thereby contributes to the
lowering of charge-transfer-mediated coupling even at shorter interchromophoric
distances. Additional investigations on the nature of excitonic states
of pentacene dimers proved that any deviation from a 90° cross-stacked
orientation results in the emergence of delocalized Frenkel/mixed-Frenkel–CT
character and the consequent loss of null exciton/monomer-like properties.
The retention of exciton isolation even at a short-range coupling
regime reassures the universality of null excitonic character in perpendicularly
cross-stacked pentacene systems. The null-excitonic character was
experimentally verified by the observation of similar spectral characteristics
in the crystalline and monomeric solution state for 6,13-bisaryl-substituted
pentacene derivatives. The partitioned influence of aryl and pentacene
fragments on interchromophoric noncovalent interactions and photophysical
properties, respectively, resulted in the emergence of pentacene centric
Kasha’s ideal null exciton, providing novel insights toward
design strategies for cross-stacked chromophoric assemblies. Identifying
the Greek cross (+)-stacked architecture-mediated null excitons with
a charge-filtering phenomenon for the first time in the ever-versatile
pentacene chromophoric systems can offer an extensive ground for the
engineering of functional materials with advanced optoelectronic properties.