“…The diameter of the semicircle represented the charge transfer resistance ( R ct ), and the R ct values for A4CA1, A4CA2, A4CA3, and A4CA4 were calculated to be 33.37, 17.32, 14.12, and 21.50 Ω, respectively, implying the smallest charge transfer resistance of the A4CA3 cathode, agreeing with the IR data in Figure e. As depicted in Figure g, the multiple virtues of high specific capacity, charming rate capability, and extensive potential range of 0.2 to 1.8 V endowed the Zn//A4CA3 device an uppermost energy density of 190.4 Wh kg –1 under a power density of 99.3 W kg –1 at 0.1 A g –1 with a reserved energy density of 83.1 Wh kg –1 under 18 kW kg –1 at 20 A g –1 , outstripping that of Zn//A4CA1 (71.7 Wh kg –1 ), Zn//A4CA2 (145.4 Wh kg –1 ), and A4CA4 (183.0 Wh kg –1 ), and even outweighing many reported aqueous ZIHSC devices constructed by different kinds of carbon materials (as listed in Table S3), such as Zn//BN-ZIC-3 (115.7 Wh kg –1 ), Zn//CSGC-700 (111.1 Wh kg –1 ), Zn//LDC (97.6 Wh kg –1 ), Zn//3DPC (156 Wh kg –1 ), Zn//HHPC-6 (117.6 Wh kg –1 ), Zn//PHCA (129.3 Wh kg –1 ), Zn//N-HCNbs-6 (109 Wh kg –1 ), Zn//NPCN 750 (143 Wh kg –1 ), Zn//PCNs-2 (119 Wh kg –1 ), and Zn//CFe0.2 (120.2 Wh kg –1 ) . Significantly, for the A4CA3-based ZIHSC device, a notable capacity of 117.7 mA g –1 with a capacity sustenance of 93.8% and nearly 100% Coulombic efficiency was achieved after 10,000 long-term charge–discharge cycles at a high current density of 10 A g –1 (Figure h), further affirming the eminent durability of the A4CA3 cathode.…”