Conspectus
“Dynamic exciton”, an umbrella
term concept in photochemistry,
plays an important role in nature, science, and technology, especially
in photoinduced and electrically induced electron transfer (ET) between
a donor (D) and an acceptor (A). Typically, an exciton in molecular
D–A systems is considered a locally excited (LE) state of a
donor (D*) or an acceptor (A*) molecule, but let us extend the terminology
of “exciton” to an integrated class of LE, charge-transfer
(CT), and charge-separated (CS) states. The degree of CT (0–100%),
spin multiplicity, and D–A interaction (i.e., electronic coupling)
are pivotal factors in the “exciton”. Another important
aspect of the “exciton” is strongly related to the “dynamic”
aspect of the “exciton” by movement of atomic nuclei
(i.e., vibration, rotation, and fluctuation) and their collective
motions controlling behaviors of electrons and spins by the passage
of time. The concept of “dynamic exciton” should cover
a wide variety of the photochemical phenomena that are all essential
for the energy conversion devices and processes including various
kinds of living systems. In these, a huge amount of the nuclear motional
modes may cooperatively be entangled to electronic orbitals. Thus,
the idea behind “dynamic exciton” includes usage of
the cooperation between nuclear motions and the spin–orbital,
as electron–phonon coupling for innovative designs of the energy
conversion materials and assemblies. For this, it is particularly
important to examine how this wide variety of the motions plays roles
on electronic couplings, intermediate geometries and mobilities, exciton
energies, CT characters, and so on. We draw researchers’ attention
to this aspect of the vibronic effect, like the entropy role by collective
movement of side chains of the conjugated polymer to modulate the
electronic coupling time-dependently at the charge delocalization
and dissociation, which is reinforced three-dimensionally at the D/A
domain interface of organic photovoltaics (OPVs). In addition, to
realize the ultimate high-performance OPVs, the voltage loss must
be diminished; i.e., the energy difference between the band gap and
the open circuit voltage is caused in part by interfacial charge recombination
via vibrational relaxation. Attaining efficient excited-state migration
with prevention of the vibrational relaxation at the D/A interface
would possibly overcome the voltage loss issues at the primary CT
event, when we understand the roles of low-frequency disorder movements
by the phonon on the vibrational relaxation in the solid state. Importantly,
conversion of the excited state-to-CS state in organic OPVs is an
opposite process to that of the CS state-to-excited state in organic
light-emitting diodes (OLEDs). Specifically, intramolecular D–A
linked systems and intermolecular D–A systems hold a prominent
position in both OPVs and OLEDs, and an intrinsic similarity is seen
in the mutual interplay among LE, CT, and CS states of such systems
facilitated by the dynamic effects. These facts encourage ...