molecules in soft self-organized supramolecular systems. [1,2] Extended π-conjugated systems are also of significant interest for application as charge carrier in organic semiconductors, [3] luminescent materials (e.g., AIEgens), [4] and for circular polarized emission in helical assemblies. [5] Therefore, tuning the organization of these π-conjugated rods in soft matter systems is fundamental and requires the understanding of their general design rules. Liquid crystals (LCs) are of great interest as stimuli-responsive and switchable optical materials in displays, photo nics [6] and in sensor applications. [7,8] Rod-like π-conjugated molecules with multiple end-chains, the so-called polycatenar molecules, have received significant interests as they provide a huge variety of different LC phases ranging from lamellar (smectic, Sm) via bicontinuous cubic (Cub bi) to columnar (Col) [9-11] and even micellar cubic phases. [3] This observation has contributed to the recognition of the importance of nano-segregation for LC phase formation and demonstrated the similarity of the fundamental self-assembly principles in lyotropic systems formed by amphiphiles, in LC phases and in the solid state morphologies of block copolymers. [12,13] Among the self-assembled structures of polycatenar molecules, the Cub bi phases [14,15] received special attention because of their potential for applications, as for example in 3D conducting [16] and photonic materials, [17] being the result of their interwoven net-* ]) as well. This work establishes rules for controlling the self-assembly of functional π-conjugated rods in soft matter and fluids.