standard hydrogen electrode). [6][7][8][9][10] Unfortunately, the uneven plating/stripping of Li metal causes uncontrolled Li dendrite growth, which induces a series of problems. First, the continuous growth of Li dendrites may puncture the separator and cause short circuit, consequently resulting in serious safety issues. [11][12][13][14] Second, Li dendrite growth can consume electrolyte and dendritic Li may lose its electronic contact with electrode (called "dead Li") during Li stripping process, accordingly reducing the Coulombic efficiency (CE) and leading to capacity fading. [15][16][17] In addition, different from the other anode materials, the relative volume change of Li metal anodes is infinite due to its "hostless" nature, leading to internal pressure changes and interfacial fluctuations. The solid electrolyte interface (SEI) layer on the surface of the electrodes, which may not accommodate the volume change, will be repeatedly break and form during continuous cycling. [18][19][20] Moreover, the broken SEI will greatly exacerbate the uneven Li electrodeposits nucleate and accelerate the growth of Li dendrites. [21,22] These severe problems impede the practical applications of Li metal anodes and the approach to solve these multifaceted problems would be imperative.To tackle these critical issues, tremendous efforts have been taken to improve the stability of Li metal anodes and the SEI from different perspectives. In order to stabilize the SEI layer, various electrolyte additives, such as Cs + and Rb + ions, LiF, Li 2 S 8 , and LiNO 3 , were used. [23][24][25] Introducing nanoscale interfacial layers has also been intensively investigated (such as interconnected carbon nanospheres [26] and hexagonal boron nitride [27] ), where repeated deposition/stripping of Li under the layers exhibited stable CE. However, the above-mentioned methods based on Li foil (2D Li metal anodes) could not effectually prevent the huge volume change upon stripping/plating of Li metal. Thus, the internal pressure changes and interfacial fluctuations still happened during cycling. [28] To solve this problem, the 3D porous current collectors were used as host structures for Li metal in recent studies, such as 3D porous copper current collectors, [29][30][31][32][33] 3D nickel foam host, [34] and graphene [35,36] electrode. As a major part of Li metal batteries, the current collector has direct influence Lithium metal is the most promising anode material for high-energy-density batteries due to its high specific capacity of 3860 mAh g −1 and low reduction potential of −3.04 V versus standard hydrogen electrode. However, huge volume change, safety concerns, and low efficiency impede the practical applications of Li metal anodes. Herein, it is shown that the nitrogen-doped graphene modified 3D porous Cu (3DCu@NG) current collector can mitigate the above problems. The N-doped graphene, coating on the surface of 3D current collector, not only contributes to a uniform Li + flux, but also leads to a scattered distribution of electrons t...