2025/04/23 by Rahul Meena, Priya Pandey, Caterina Zuffa +17 · 1 voice
Chemistry · Engineering · Materials Science · #Crystallography and molecular interactions #Machine Learning in Materials Science #Surface Chemistry and Catalysis
paper · pdf · doi:10.1021/acs.cgd.5c00145
openalex publication_date 2025/04/23 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/22
High Resolution Image Download MS PowerPoint Slide The crystal structures of organic semiconductors are critical when they are integrated into optoelectronic devices, such as organic field-effect transistors (OFETs). In this study, we introduce a crystal engineering approach that leverages weak, nondirectional dispersion forces and steric effects, working together to govern the molecular packing. We investigated how the substitution at the peri-position affects the crystal structure in a series of oligorylene molecules. Upon elucidation of the crystal structures, we found a distinct difference between symmetrical and unsymmetrical derivatives. The unsymmetrical derivatives are prone to forming a sandwich herringbone (SHB) motif, while symmetrical derivatives exhibit a typical herringbone (HB) motif. In most of the rylene derivatives, substitutions at the peri-position triggered an “end-to-face” orientation within the HB structure, rather than an “edge-to-face” orientation, which occurs more often. Results from the Hirschfeld surface analysis provide evidence that the “end-to-face” orientation promotes C–H–π interactions between terminal methyl groups and the π-core of the molecules. While these C–H methyl ---π interactions contribute to the overall stability of the packing structure, they remain ineffective in enhancing the charge transport properties. In contrast, a particular derivative, tetramethyl perylene ( TMP ), exhibits a HB structure with an edge-to-face orientation, promoting both C–H---π and π---π interactions. These interactions are crucial for improving the charge carrier mobility, as evidenced by mobility values. For TMP, we could obtain the mobility value of 0.05 cm 2 V –1 s –1 in OFETs, whereas a slightly higher mobility of 0.2 cm 2 V –1 s –1 was observed with Field-Induced Time-Resolved Microwave conductivity (FI-TRMC) technique.