Since its discovery by Geim and coworkers in 2004 [1], graphene has attracted increasing attention because of its unique structure and properties . Graphene is a monolayer of carbon atoms with close-packed conjugated hexagonal lattices, in which the carbon bonds are sp 2 hybridized [30]. This unique structure endows graphene with remarkable physical properties. In graphene, electron-phonon scattering is so weak that the mobility of charge carriers can be improved significantly, even up to 200 000 cm 2 V −1 s −1 under ambient conditions, if the extrinsic disorder is eliminated [31]. This value exceeds the intrinsic mobility of any other semiconductor [31,32]. In addition, graphene possesses large theoretical specific surface area (2630 m 2 g −1 ) [33], high Young's modulus (∼1.0 TPa) [34], as well as good thermal (∼5000 W m −1 K −1 ) [35] and electrical conductivity [36].In order to fully understand and utilize the excellent physical and chemical properties of individual graphene sheets at a macroscopic level, it is desirable to fabricate various macroscopic graphene-based materials. As a fundamental twodimensional (2D) carbon structure, graphene sheets can be considered as basic building blocks to construct 3D graphene-based materials. A critical challenge in building graphene-based macroscale structures is to effect the transfer of the exceptional properties of graphene nanosheets to the macroscale structures by controlling the orientation and organization of the building blocks at the nanoscale. For example, the strong π-π stacking and van der Waals force between the planar basal planes of graphene sheets result in self-agglomeration of graphene, creating particulate graphite platelets which lose the unique ultrahigh surface area of graphene sheets. This adversely affects the potential applications of graphenebased macroscale structures in the fields of supercapacitors and batteries. To prevent self-aggregation, currently a number of strategies have been developed for fabricating porous macroscale structures, including the addition of ''spacers'' (i.e., surfactants, nanoparticles (NPs), polymers) [37][38][39][40][41][42][43][44][45][46], template-assisted growth [47], crumpling of graphene sheets [48,49], and so on. While the specific surface area of these graphene macroscopic structures is still lower than the theoretical specific