“… 6 , 41 , 44 − 54 It still stabilized at ∼4.0 mAh/cm 2 after 20 cycles (see Figure 10 e), which is also a quite high areal capacity. It is found when using the loading of 10.1 mg/cm 2 , the capacity density based on electrodes can reach 881 mAh/cm 3 for maximum volumetric and 189 mAh/g for maximum gravimetric, which are much higher than those of previous metallic current collector electrodes such as np-Cu/SnO 2 , 6 np-Cu/MnO 2 , 41 NP Cu@Cu 2 O, 45 Cu/Si/Ge NW@Ni-CF, 46 ZnCo 2 O 4 @Ni-CF, 50 NiO@Ni-CF, 51 ZnCo 2 O 4 –ZnO–C@Ni-CF, 52 Co 3 O 4 @Co 3 S 4 @Ni-CF, 53 graphite anodes (1.3 g/cm 3 , and calculated with a theoretical capacity of 372 mAh/g) on the Cu foil (18 μm thick for half cells), as well as the volumetric energy density of Si–C electrodes on Cu foil (∼734 mAh/cm 3 , see the calculations, Figure 10 f and Table S2 in Supporting Information ). 54 It should be pointed out that, when using a copper foil with a thickness of ∼10 μm in commercial use, the theoretical gravimetric capacity density and volumetric capacity density of graphite anode will increase to 164 mAh/g and 414 mAh/cm 3 .…”