The solid-solid interfacial impedance between the garnet electrolyte and Li metal anode is one of the major challenges for garnet's application in all-solid-state batteries. The areal specific resistance (ASR) is investigated by ab initio calculations in this article, to predict the intrinsic ASR as lower limitation. The Li ion migration across the interphase is divided into two steps: 1) Li "intercalation" from Li-metal to the LLZO, forming a Li-rich interphase beneath the surface of LLZO, and 2) Li migration in the Li-rich interphase within LLZO. The first step is investigated by climbing image nudged elastic band (CI-NEB), resulting in barrier energy lower than 0.37 eV compared to experimental 0.34 eV of the garnet bulk phase. The second step is investigated by ab initio molecular dynamic simulations (AIMD), indicating that the Li-rich interphase's conductivity is lower by about 1-2 orders of magnitude compared to the bulk phase. As a result, the sum theoretical intrinsic ASR is as low as 0.01 cm 2 , suggesting high ASR in practicable battery arises from surficial impurity Li 2 CO 3 rather than intrinsic ionic resistance. However, difficulties of removing Li 2 CO 3 lie in that Li 7 La 3 Zr 2 O 12 can thermodynamically decompose into reactive Li 2 O to form high resistant Li 2 CO 3 .With the rapid application and promotion of lithium ionbased electric or hybrid electric vehicles, the demand on safety and energy density is becoming more and more critical. As the flammable organic liquid electrolyte is the main case of the urgent safety problem, the solid electrolytes (SEs) without flammable organic small molecular liquid gradually attracts wide attention, including inorganic ceramic electrolytes and dry organic polymer electrolytes. [1] On the other hand, since the energy density upgrade of cathode could not fully meet the requirements, Li metal anode with a high capacity of 3860 mAh g −1 (about 1 order of magnitude higher than its graphite counterpart of 372 mAh g −1 ) is revived as a silver bullet for the demanding energy density. However, the lithium metal anode shows poor compatibility with traditional organic liquid electrolyte owing to a continuously evolving Li/electrolyte interface during charge/discharge. This insurmountable hurdle becomes soluble with suitable SEs, since a long-term stable interface of Li/SE is more accessible with the help of nonflowable solid electrolyte. Requirements on SEs include higher conductivity than 10 −4 S cm −1 at room temperature as the threshold for running a regular cell, [2] negligible electronic conductivity, wide electrochemical stability window, and high chemical and electrochemical stability with electrodes. Among the existing SEs including Li 3 N, [3] Na superionic conductor (NASICON), [4] perovskite, garnet, thio-γ -Li 3 PO 4 related system [5] (including glass and glass-ceramic states), thio-Li superionic conductor (LISICON), [6] and Li 10 GeP 2 S 12 , [7] garnet structured Li ionic conductors attract dominated interests in recent years [8,9] mainly owing to an a...