Under realistic conditions especially for high-energy-density LMBs (>400 Wh kg −1 ), these phenomena will be exacerbated, thereby leading to poor electrochemical performance.Extensive efforts have been devoted to tackling the issues mentioned above, including the modification of surface with protective layers, [7][8][9][10][11] design of current collector structures, [12][13][14][15] introduction of functional electrolyte additives, [16][17][18][19] and application of solid-state electrolytes. [20][21][22] Despite the considerable success achieved in preventing dendrite growth to a certain extent at low Li plating capacities (<2 mAh cm −2 ), challenges still exist at high deposition capacities (>4 mAh cm −2 ). [23] Fundamentally, the formation of Li dendrites undergoes two steps involving nucleation and growth of the Li crystals. [24] As with other metal anodes, Li metal grows continuously on its early-formed nuclei during cycling. The final deposition morphology tightly relies on the preferential crystallographic orientation of Li-metal crystal. [25,26] Intrinsically, Li metal is a body-centered cubic structure, and ( 110), (200), and (211) crystal planes are normally the dominant crystallographic features. Among them, the (110) crystal plane is the most densely packed and thus has the lowest-energy surface, which is regarded as the preferential growth crystal plane of Li-metal anode. [27] Thermodynamically, Li dendrites will eventually be formed if the Li metal keeps growing along the (110) crystal plane. [28,29] Therefore, regulating Li metal's preferential growth orientation is essential. Recently, biomacromolecules have been proven effective in modulating inorganic crystal orientation and inhibiting Li dendrites. [30] Besides, a lateral growth model of Li deposition on single crystal Cu substrates was reported, and the acquired planar Li-metal layer exhibited improved cycle stability and high CE. [31] However, most of the approaches reported to date mainly operated at relatively low Li deposition capacities (<2 mAh cm −2 ), which are insufficient to boost the specific energy beyond 400 Wh kg −1 . To achieve the specific energy up to 400 Wh kg −1 , realistic conditions, including high areal capacity of both anode and cathode (>4 mAh cm −2 ) and lean electrolyte (<3 g Ah −1 ), are necessary. [32,33] Whereas, conditions of current investigations are low mass loading cathode (<3 mAh cm −2 ) and flooded electrolyte (>3 g Ah −1 ), which are far from realizing high cell-level energy Lithium (Li) metal, a promising anode for high-energy-density rechargeable batteries, typically grows along the low-surface energy (110) plane in the plating process, resulting in uncontrollable dendrite growth and unstable interface. Herein, an unexpected Li growth behavior by lanthanum (La) doping is reported: the preferred orientation turns to (200) from (110) plane, enabling 2D nuclei rather than the usual 1D nuclei upon Li deposition and thus forming a dense and dendrite-free morphology even at an ultrahigh areal capacity of 10 mAh...