“…Additionally, the binding energy of Ni 0 for Ni@DC-0.03, Ni@DC-0.04, Ni@DC-0.05, and Ni@DC-0.06 is 852.1, 852.4, 852.7, and 853.2 eV, respectively. The upward shift indicates that the electronic environment of Ni is regulated by the electron shift from Ni to the defective carbon species. − Furthermore, as seen in Figure b, the C 1s peaks at 285.7 and 289.8 eV are related to C–O and CO 3 2– groups, respectively, , indicating that the carbon layer surface is rich in oxygen-containing functional groups. It is noteworthy that the strongest signal peaks are all around the binding energy (BE) of 284.0 eV, demonstrating that the carbon layer of the Ni@DC- x is always dominated by sp 2 , and the carbon layer is rich in defects. , In detail, the binding energies of sp 2 C for Ni@DC-0.03, Ni@DC-0.04, Ni@DC-0.05, and Ni@DC-0.06 are 284.2, 283.9, 283.6, and 283.2 eV, respectively, suggesting that the binding energy of sp 2 C decreases with the increment of carbon defects.…”