fluorinated solvent and additives. [5] Assisted with solid electrolyte interface (SEI)-forming additives allows for a stable cycling performance with a high Coulombic efficiency, as the negative electrode is protected from co-intercalation reactions of relatively large pyrrolidinium cations. [6] Nevertheless, slow electrode kinetics relating to Li intercalation/de-intercalation and notorious safety issue have been becoming the very bottleneck in improving power densities of these dual-ion batteries while achieving high energy density.To address the problem of low power density for dual-ion batteries, the electrochemical intercalation must be replaced, at least for one electrode, with means of physical adsorption. Accordingly, the electrodes must be abundant with a high specific area and excellent mechanical properties, e.g., graphene and few-layer graphite. [7] Without considering the desolvation/ dendrite issues for Li ions during the fast charge/discharge, the cations in electrolyte absorbing/desorbing onto a graphene surface can supply a high power density. Herein, we propose a dual-ion battery by selecting an electrolyte of (EMIm) + (PF 6 ) − ionic liquid using graphite as positive and reduced graphene oxide (RGO) as negative electrodes. The power density yields as high as 1333 W kg −1 , by simultaneously maintaining a competitive energy density of 70 Wh kg −1 (see Figure 1). The manifested harvesting of optimum performance excels as integration of an intercalation/de-intercalation mechanism and a fast surface absorption/desorption mechanism in a cell. Figure 2A shows the cyclic voltammetry (CV) curve of the graphite electrode at a scan rate of 5 mV s −1 . Although metallic lithium is usually used as the reference electrode or symmetry system without reference electrode, [8] herein the influence of interaction between Li and working electrode was excluded, as well as the complex reactions between two working electrodes. [5] This configuration thereof guarantees liable electrochemical characterization. As indicated by the arrows, a broad peak (1.6-2.0 V) and a small peak (1.46-1.6 V) appear with the potential increasing, unraveling a PF 6 − insertion process. Whereas the potential shifts negatively, two broad and small peaks ranging from 2.0 to 0.8 V were observed, revealing the de-insertion of anions from the graphite electrode. The occurrence of these redox peaks for ion uptaking and releasing in the CV curve describes a stage formation mechanism, in which multiple coordination possibilities exist for the anion in the graphite. These staging effects are well accepted for electrochemical lithium insertion into graphite and for TFSI − into graphitic carbons. [9] It is noted that the peak potential range of the charge process is narrower than that of the discharge process. The main peak in the charge process is consistent with a large current, whereas the curve of the discharge process consists For an electrochemical energy storage cell, it is challenging to synergistically harvest high energy density and hig...