been developed to grow 1D C 60 crystals including template method, slow evaporation, precipitation, liquid/liquid interface precipitation (LLIP), volatile diffusion, and gel-assisted method in general. While early attempts to grow C 60 crystals resulted in various morphologies, it was the use of crystalline C 60 fibers that had attracted particular interest because of their outstanding properties with high surface area and low dimensionality. [14] Although some methods were used to grow 1D fullerene crystals, it is still a great challenge to grow them with tunable sizes owing to their naturally 0D structures. Thus, to develop a method for the controlled growth of 1D C 60 crystals is still challenging and demanding for its promising applications, e.g., photodetector.As a recently developed medium for crystal growth, supramolecular gels derived from low-molecular-mass gelators (LMMGs), are a typical class of soft materials in which gelator molecules can be assembled into dynamic 3D networks via cooperative noncovalent interactions. [15][16][17][18][19][20][21][22] The gel matrix commonly entraps solvent molecules and prevents the macroscopic flow of the solvent within its networks. Sedimentation or aggregation of the crystals is suppressed in supramolecular gels and the arbitrary growths along faces in contact with the vessel walls or other crystals are also limited. Furthermore, the supramolecular gel could act as an inert matrix repressing heterogenous nucleation and making homogenous nucleation dominant. Or it affords an activated gel As a superstar organic semiconductor, fullerene (C 60 ) is versatile in nature for its multiple photoelectric applications. However, owing to its natural 0D structure, a challenge still remains unbeaten as to growth of 1D fullerene crystals with tunable sizes. Herein, reported is an efficient approach to grow C 60 as super-long crystalline fibers with tunable lengths and diameters in supramolecular gel by synergic changes of anti-solvent, gel length, crystallization time or fullerene concentration. As a result, the crystalline C 60 fibers can be modulated to as long as 70 mm and 70 000 in their length-to-width ratio. In this case, the gel 3D network provides spatial confinements for the growth of 1D crystal along the directional dispersion of anti-solvent. The fabricated fullerene device exhibits high responsivity (2595.6 mA W -1 ) and high specific detectivity (2.7 × 10 12 Jones) at 10 V bias upon irradiation of 400 nm incident light. The on/off ratio and its quantum efficiency are near to 540 and about 800%, respectively, and importantly, its photoelectric property remains very stable after storage in air for six months. Therefore, spatially confined growth of fullerene in supramolecular gels will be another crucial strategy to synthesize 1D semiconductor crystals for photoelectrical device applications in near future.
1D Fullerene CrystallizationAs a typical 0D carbon-based material, fullerene (C 60 ) is one of the important organic semiconductors and is versatile in nature on a...