This efficiency is significantly higher than that of traditional chemical approaches such as CO 2 hydrogenation or reforming. [14] In addition, operations at high temperatures can achieve larger cur rent densities due to lowering resistances, increasing productivity and reducing system size/cost.Although SOEC electrodes with perov skite structures (e.g., La 0.8 Sr 0.2 CoO 3−δ ) have the potential to tolerate current density as high as 5 A cm −2 (see the Sup porting Information for details), prac tical electrode performances degrade quickly, even at low current densities (e.g., 500 mA cm −2 ). [15,16] Such fading is mainly attributed to intensified current densi ties, causing anode delamination due to extremely high oxygen partial pressures (P O2 ) at the anode-electrolyte interface. [17,18] Notably, compared with reverse devices (solid oxide fuel cells, SOFCs), the P O2 at the anode-electrolyte interface for SOECs are commonly several times higher, [19] and further increases more than 100 times under a large current density (>1 A cm −2 ). [20] Therefore, performance degradation is even more serious for SOECs. Such high P O2 can be attributed to inherent structural defects. Traditionally, using perovskite materials (e.g., La 0.6 Sr 0.4 CoO 3±δ (LSC)) as precursors, SOEC anodes prepared by screenprinting or wet powder spraying methods [21] mainly possess spongelike structures (as shown in Figure 1a, traditional electrode LSC (TELSC) is illustrated as an example). Such spongelike anodes typically possess enor mous pores distributed randomly in space and varied widely in size. [22] Although the inherent electronic and ionic conduc tivity provided by LSC should be sufficient for operations at high temperatures (e.g., 800 °C) and large current densities (e.g., 1-2 A cm −2 ), the properties advantages are greatly lim ited by the spongelike structure due to the sluggish oxygen generation and release kinetics. Specifically, here sluggish oxygen generation is ascribed to the limited interface areas for oxygen evolution reactions (OERs). [23,24] And the poor oxygen release is caused from tortuosity factors (typically, >3 [25] ), low porosities (typically, <30%), [26] and even blocked tunnels, thus suffocating generated gases and subsequently causing anode delamination at high current densities. [22] Currently, hierarchical micro/nanostructures with well oriented nanoarrays have shown superwetting behaviors in aqueous electrolyte environments and demonstrated high efficiencies for electrolyzing (e.g., water splitting and fuel cells). [27,28] Studies in medium or high temperature systems As a clean, efficient, and promising energy conversion device, solid oxide electrolysis cell (SOEC), which can achieve transformation from electricity to chemical fuels, has captured worldwide attention. A novel biomimetic honeycomb SOEC anode with super low tortuosity factor (≈1), ground-breaking porosity (≈75%), and high structural strength, has been successfully fabricated by freeze casting and infiltrating. This honeycomb anode demonstrat...