“…Coronene is a rigid molecule and able to form one‐dimensional crystals with mechanical flexibility and controllable size by solution self‐assembly, which is reliable and easy‐to‐implement (Figure 1 a–g) [13b] . Structurally, strong face‐to‐face cofacial parallel stacked π–π interactions along the growth direction [010] (Figure 1 d,e,k), and weak edge‐to‐face T‐shape π‐π interactions along the [001] direction coexist, bringing only very weak dispersive interactions along the [10 ] direction (Figure 1 d,e,l, Figure S20,S21 and Table S3 for energy frameworks analysis), [6b, 14] which represents a remarkably bendable nature of the (10 ) plane, [1f, 8j, 9c, 15] consistent with the experimental facts that the crystals show elasticity when applying force at (10 ) plane and show brittleness when applying force at (001) plane (Figure 1 b,c,f,g, Movie S3, Figure S3,S17). However, the inherent herringbone packing motif without effective two‐dimensional π‐π overlap determines limited charge transport, [13a, 16] resulting in a conductivity less than 10 −12 S cm −1 [17] .…”