the active carbon, typically 50-200 F cm −3 (corresponding to 100-300 F g −1 ), [7] the energy density of commercial SCs is limited to 10 Wh L −1 . [8] In order to improve the energy density of SCs, researchers have made tremendous progress in the past decade in developing high-capacitive active materials, including graphene, conductive polymers, metal oxides, and metal hydroxides. [9] However, most of these materials were tested with thin electrodes (mass loading of active materials on current collector less than 1 mg cm −2 , thickness of electrode lower than 10 µm), [10] which cannot achieve a high energy density at a device level because the majority of the volume is occupied by inert materials such as current collectors. When the thickness of the electrode is increased to practical levels required to ensure a high energy density (mass loading of active materials more than 10 mg cm −2 , thickness of electrode higher than 100 µm), the volumetric capacitance often drops significantly due to the low electric and ionic conductivities of thick electrodes. [11] As such, there has been a significant tradeoff between the volumetric capacitance and the thickness of electrodes.A promising solution to mitigate the tradeoff is to assemble the active materials into 3D porous and conductive scaffolds with interconnected ion-diffusion channels. Sun et al. demonstrated the self-assembly of Nb 2 O 5 nanoparticles and holeygraphene into the 3D porous composite electrode, which showed ultrahigh-rate energy storage at a mass loading of more than 10 mg. [11a] Shang et al. reported the vacuum filtration of metal-oxide-immobilized CNTs and holey-graphene into 3D scaffolds, which also pertained to a high capacitance of 143 F cm −3 at an ultrahigh thickness of 420 µm (mass loading 35 mg cm −2 ). [12] Recent developments of highly conductive 2D pseudo materials also show promise to address this issue. MXene, a class of 2D transition metal carbides and nitrides, are highly conductive and high-capacitive materials. [13] Electrodes made of MXene showed superior high-rate performance to those made of conductive polymers, carbon, and metal oxides. Yet, the volumetric capacitance of MXene deteriorated seriously from 900 to 350 F cm −3 when the thickness of the electrode was increased from 5 to 75 µm. [14] Another type of 2D materials, 2D metal-organic frameworks (MOFs), displayed a high Increasing the electrode thickness of energy-storage devices can enhance the areal capacitance, but often results in a significant decrease in the volumetric capacitance. This tradeoff between the volumetric capacitance and electrode thickness, which is ascribed to the poor ion and charge transport in thick electrodes, has been a major obstacle to realizing high-energy-density of devices. Herein, an inverse opaline metallic membrane (IOMM) is reported as a stable and high-rate electrode, which displays a linear increase in volumetric capacitance as a function of electrode thickness. The IOMM is fabricated through simple self-assembly, photopolymerizati...