Although a wide variety of three-dimensional porous electrode architectures have been created for supercapacitors to markedly enhance the charge and mass transfer associated with cycling, their low volumetric energy densities limit applications in many energy storage systems. In this work, we report a unique electrode architecture consisting of Ni 3 S 2 nanosheet-onto-Ni 3 S 2 -nanorods grown on nickel foam and prepared using a simple one-step hydrothermal method. When tested as an electrode for a supercapacitor (using a three-electrode configuration), this material exhibited excellent rate capability and cycling stability at high cycling rates. The obtainable capacitance decreased by o42% as the current density was increased from 20 to 240 mA cm − 2 , and the capacity retained 89.3% of its initial value after 5000 cycles at a cycling rate of 120 mA cm − 2 . Further, an asymmetric supercapacitor consisting of the Ni 3 S 2 nanosheet-onto-Ni 3 S 2 -nanorods electrode and an activated carbon (AC) electrode displayed a volumetric energy density as high as~1.96 mWh cm − 3 , with the potential to bridge the performance gap between thin-film Li batteries and commercial AC//AC supercapacitors. The outstanding electrochemical performance is attributed to the good mechanical adhesion and electrical connection with the substrate, high contact area with the electrolyte and alleviated structural pulverization during the ion insertion/desertion process. It is predicted that the architectural Ni 3 S 2 -nanosheet-on-nanorods array prepared with this facile method offers great potential promise in large-scale energy storage device applications. NPG Asia Materials (2016) 8, e300; doi:10.1038/am.2016.126; published online 26 August 2016
INTRODUCTIONThe demand for clean energy and emerging ecological concerns have greatly stimulated research on the development of new, low-cost and environmentally friendly energy conversion and storage systems. To this end, supercapacitors have attracted much interest in the past decades because they can supply high power density and long cycle life. However, a major shortcoming of the existing supercapacitors is their low energy density (typically 5-10 Wh kg − 1 ), which is significantly lower than that of lithium ion batteries (120-180 Wh kg − 1 ). [1][2][3][4] Higher energy density (E = 0.5 CV 2 ) can be achieved by increasing the cell voltage (V) and the specific or volumetric capacitance (C). [5][6][7] In general, the cell voltage and the specific capacitance are determined primarily by electrode properties, such as composition, structure, morphology, particle size and porosity, among others. 3 In addition to exploration of new electrode materials, much effort related to improved energy density of supercapacitors has been directed toward construction of novel architectures for full utilization of active electrode materials.