Perylenediimide (PDI) and its derivatives have garnered
significant
attention as promising n-type semiconductors to replace fullerenes
as acceptors in organic photovoltaic cells (OPVs). However, the aggregation
tendencies and rapid excimer formation of PDIs have hindered their
efficiency in OPVs. To address this issue and enhance solubility while
fine-tuning their electronic properties, researchers have explored
fluorination strategies. In this study, we investigate the structure–function
relationship of two crystalline N,N-bis(2′,2′,3′,3′,4′,4′,5′,5′,6′,6′,7′,7′,8′,8′,8′-pentadecafluorooctan-1-yl)perylene(3,4:9,10)bis(dicarboximide)
(FPDI) polymorphs, namely, FPDI-α and FPDI-β. Their crystal
structures show that the π systems of the FPDI molecules in
FPDI-α adopt an orthogonal geometry, while those in FPDI-β
are parallel and slip-stacked. We report their excited state dynamics
using transient absorption and fluorescence microscopy and time-resolved
electron paramagnetic resonance spectroscopy. Upon photoexcitation,
both crystal polymorphs exhibit the formation of a lowest excited
singlet (S1) state with substantial charge transfer (CT)
character. This S1-CT state in FPDI-α decays in τ
= 350 ps to form the FPDI triplet state via spin–orbit charge-transfer
intersystem crossing in near-quantitative yield, while the S1-CT state in FPDI-β decays back to the ground state in τ
= 140 ps. This study illustrates the influence of different packing
motifs on photoinduced intermolecular CT processes in single crystals
of the same molecule and contributes to an understanding of the role
of fluorination in optimizing PDI-based molecular materials for CT
state formation in the solid state.