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(A) Rate capability: current density vs. specific capacitance. (B) Cyclic voltammetry (CV) curve of three samples at 100 mv s⁻¹. (C) Nyquist plots of three samples; the inset is a magnification of the high-frequency range data and fitting equivalent circuit. (D) Galvanostatic charge–discharge (GCD) curve of APPy-850-SC at current densities of 1, 2, 4, 6, 8, and 10 A g⁻¹. (E) CV curve of APPy-850-SC at a scan rate of 20–200 mV s⁻¹. (F) Cycling stability and coulombic efficiency of APPy-850-SC at 6 A g ⁻¹ for 10,000 cycles. The inset shows photographs of two blue LEDs.

(A) Rate capability: current density vs. specific capacitance. (B) Cyclic voltammetry (CV) curve of three samples at 100 mv s⁻¹. (C) Nyquist plots of three samples; the inset is a magnification of the high-frequency range data and fitting equivalent circuit. (D) Galvanostatic charge–discharge (GCD) curve of APPy-850-SC at current densities of 1, 2, 4, 6, 8, and 10 A g⁻¹. (E) CV curve of APPy-850-SC at a scan rate of 20–200 mV s⁻¹. (F) Cycling stability and coulombic efficiency of APPy-850-SC at 6 A g ⁻¹ for 10,000 cycles. The inset shows photographs of two blue LEDs.

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Carbon-ionic liquid (C-IL) supercapacitors (SCs) promise to provide high capacitance and high operating voltage, and thus high specific energy. It is still highly demanding to enhance the capacitance in order to achieve high power and energy density. We synthesized a high-pore-volume and specific-surface-area activated carbon material with a slit m...

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