cyclability under low-Li-excess and lean electrolyte conditions. [20][21][22] The formation of a stable, dense, atomically thin solid electrolyte interphase (SEI) is critical to suppress the depletion of metallic Li and liquid electrolytes. However, the relatively thin SEI usually undergoes a repeated fracture and rebuilding process over cycling. [23,24] Transitioning from liquid electrolytes to more stable inorganic solid electrolytes offers a potential pathway to enable highly reversible Li-metal anode. [7,25,26] Careful cell and material design of anode-free Li metal || NMC full cells based on sulfide solid electrolytes has enabled thousands of full cycles without degradation. [27] Though solid electrolytes, such as the sulfide-based electrolytes, are unstable with Li metal, parasitic interfacial reaction ceases when a kinetically stable interphase layer is formed. [27] Moreover, the solid electrolyte usually displays a high stiffness and good ductility than the porous separator in liquid electrolyte cells; therefore, it performs as mechanically strong support to prevent the fracture of the interphase layer. [27,28] Despite these efforts, the interface between the Li-metal anode and solid electrolyte suffers from chemomechanical degradation under practical cycling conditions (e.g., high current density). [29][30][31] First, the Li stripping reaction creates voids at the Li-metal/solid electrolyte interface, inducing a loss of ionic contact (Figure 1a). [32] Moreover, high-rate Li plating induces nonuniformity in the stress and electric fields, leading to heterogeneous Li plating, and further deteriorating the interfacial contacts. [33][34][35][36][37] An impractically high stack pressure (e.g., >1.0 MPa) is constantly required during cell operation to smooth the surface of the planar Li-metal anode. [38] With a stack pressure of above 1.0 MPa, most solid-state cells were tested with pressure jigs and a rigid sleeve to avoid the side effects of Li-metal creep in the radial direction. [39] The complicated cell design increases the manufacturing cost and dilutes the celllevel energy. In contrast, the optimized stack pressure adopted by scalable Li-ion pouch cells is usually within the range of 0.05-0.5 MPa. [40] The design of a 3D Li-metal anode potentially enables a mild stack pressure since the high surface area of the anode scaffold provides more intimate ionic contacts (Figure 1b). In addition, a small local current at the interface benefits the interface stability. [41][42][43][44][45] However, this direction has Transitioning from a liquid electrolyte to an inorganic solid electrolyte offers a potential pathway to enable highly reversible lithium-metal anodes. However, the solid-electrolyte-protected lithium-metal anode suffers from poor interfacial ionic contacts and requires an impractically high stack pressure (>1.0 MPa) to maintain the interfacial contacts. It is demonstrated here that combining a hollow silver/carbon fiber scaffold and an inorganic/ organic composite electrolyte enables a highly revers...