more stable interface against Li metal among SSEs. [3][4][5][6] The latter opens the door for safe use of Li metal anodes that have a high theoretical capacity (3860 mAh g −1 ) and a lowest electrochemical potential (−3.04 V vs standard hydrogen electrode), which is expected to maximize the energy-density advantage of SSLBs. [7] However, the large interfacial resistance between the rigid garnet solids and Li metal anodes is a huge challenge for fabricating high-performance SSLBs. [5,8] Although high-pressure treatment or vacuum evaporation have been used to deposit Li metal onto garnet solid to minimize the interfacial resistance, their complicated operations and procedures greatly limit the technological applications. Currently, melting Li metal integrated with garnet electrolytes, with the assistance of an intermediate layer between the garnet and Li metal, has been widely reported to overcome the lithiophobicity of garnet and consequently facilitated the interfacial resistance. [5] The intermediate layers mainly include Al 2 O 3 , Si, Au, Sn, ZnO, and polymers. [9][10][11][12][13][14] Although the interfacial resistance has been significantly decreased, numerous SSLBs reported to date are still unable to operate at high current densities (generally less than 0.5 mA cm −2 , see Table S1, Supporting Information), which would specifically inhibit the practical applications in power backups, portable power tools, or electric vehicles require much higher power densities. The poor power density of SSLBs is still neglected by battery community to date, at least, the current state-of-the-art interfacial modification strategies is a key bottleneck for the high-power SSLBs. The intermediate layers without sufficient ionic conductivity, such as Al 2 O 3 , ZnO, and polymers, may result in a unfavorable polarization resistance during operation under high current density, [9,15,16] while the other intermediate layers like Au and Sn are electronically conducting, [10,11,17] thus tending to result in Li penetration across the layer. And even worse, volume changes are inevitable when lithiating these inorganic layers with molten Li metal through the alloying-conversion reactions. [10] An ideal intermediate layer should, in principle, not only change the garnet from lithiophobic to lithiophilic, and also could be a fast and stable Li + conducting interphase when operating under high rate conditions.