energy density. [3] Fortunately, the exploration of novel configurations of K-based energy storage systems is expected to provide key breakthroughs in overcoming performance bottlenecks. [4] An anode-free battery archi tecture tactfully eliminates active anode materials by pairing a fully preintercalated cathode with a bare anode current collector, thereby endowing the full-cell with increased energy density. [5] Pint et al. constructed an anode-free Na-metal battery using sodiated pyrite as the cathode and Al foils modified with a carbon nucleation layer as the anode current collector, achieving an energy density of ≈400 Wh kg −1 . [4a] Meanwhile, Luo et al. reported an anode-free porous Al||presodiated TiS 2 full-cell with increased energy density. [6] Recently, Mitlin et al. devised an innovative anode-free Na-metal battery comprising a Na 2 (Sb 2/6 Te 3/6 Vac 1/6 ) current collector and Na 3 V 2 (PO 4 ) 3 cathode, obtaining a capacity decay of only 0.23% per cycle. [7] Despite these achievements, anode-free K-metal batteries have rarely been explored.Besides possessing advantages over Cu in terms of cost and weight, Al foil can function as an anode current collector in anode-free K-metal batteries. [8] However, commercial Al current collectors are electrochemically potassiophobic and exhibit high nucleation resistance, inducing uneven electrochemical K deposition. [9] This results in poor reversibility during the plating/stripping process, which is reflected by a low Coulombic efficiency (CE). As anode-free K-metal batteries possess a finite K inventory in the cathode, the low CE might eventually result in capacity plunge and battery failure. [5,10] Therefore, it is of core significance to modulate the nucleation-growth behavior of K on an Al current collector through scalable and delicate surface modification. [11] Various conceptual models have been proposed to reveal the electrochemical growth behavior of metals that are complementary toward each other. [12] Recently, a film growth model was established to explain the growth of metals from a new perspective. [13] In this model, the electrochemical plating of K can be analogized as thin-film growth in vacuum and is governed by the surface energy of the substrate. [14] Based on this model, it is feasible to tune the surface energy of an Al current collector to ameliorate the nucleation-growth behavior Potassium (K)-metal batteries have emerged as a promising energy-storage device owing to abundant K resources. An anode-free architecture that bypasses the need for anode host materials can deliver an elevated energy density. However, the poor efficiency of K plating/stripping on potassiophobic anode current collectors results in rapid K inventory loss and a short cycle life. Herein, commercial Al foils are decorated with an ultrathin graphenemodified layer (Al@G) through roll-to-roll plasma-enhanced chemical vapor deposition. By harnessing strong adhesion (10.52 N m −1 ) and a high surface energy (66.6 mJ m −2 ), the designed Al@G structure ensures a highly...