Organic photovoltaic devices have improved dramatically,
and small
molecular systems with simple synthesis such as squaraines are prime
candidates for cost-effective commercialization. Squaraines have a
rich set of excited states, which depend substantially on the morphology
of a bulk heterojunction (BHJ) device active layer. Therefore, squaraines
provide an excellent opportunity to study the influence of active
layer mixing, aggregation, and the cascade of exciton diffusion from
point-of-photoexcitation to point-of-charge generation, which drives
the efficiency of devices. This work provides a focused investigation
into the energy transfer properties of photoexcited charge-transfer
H-aggregates (CT-HA) in squaraines, which are predominantly formed
in squaraine-fullerene BHJ devices. The work explores the relaxation
pathway from CT-HA to charge transfer at the BHJ interface, and explains
the higher device efficiencies previously observed as squaraine/fullerene
mixing increases through chemical modification of the squaraine. Leveraging
transient absorption measurements, we scrutinize the excited state
spectroscopy and kinetics in both neat and PCBM blended thin films
for two squaraines, DBSQ(OH)2, which mixes well with fullerenes,
and DHSQ(OH)2, which tends to phase separate. Transient
absorption spectroscopic features are assigned to populations of monomer,
dimer H-aggregate and CT-HA. CT-HA states are targeted through excitation
wavelength selection, and subpicosecond spectroscopic changes and
kinetics show the depopulation and repopulation of various excited
states. From these measurements we infer the energy transfer from
the initially photoexcited state across space and through a landscape
with an energy-distribution cascade, and with a Dexter mechanism,
despite the fluorescence suppression of H-aggregation. For all fullerene
BHJ blends, we observe evidence of an excited state complex between
fullerene and squaraine. Specifically, for DBSQ(OH)2 blended
films, the energy transfer to these complexes occurs within 100 fs,
with apparent charge separation occurring some ten times faster than
for DHSQ(OH)2 films, a result which aligns with an observation
of increased efficiency devices as measured in prior work.