To elucidate the influence of compositional and structural changes on the electronic structures of Co
xN (
x = 1, 2, 4, and 5.47), the density of states (DOSs) for Co
xN surfaces and the Bader charges for Co
xN bulk crystals were calculated. As depicted in Fig. S1 (Supporting information), the surface DOSs near the
Ef for Co
5.47N are higher than other Co
xN (
x = 1, 2 and 4) catalysts, indicating its good electronic conductivity. The Bader charge analysis of the bulk phase (Table S1 in Supporting information) further confirms that the monovalent state of Co (0.887) in CoN is the highest among all considered Co
xN. With gradual increase of Co content, the Bader charge of Co decreases to 0.555 for Co
2N and further splits into 0.313 and 0.173 for Co
4N. Especially in Co
5.47N, Co exhibits three distinct oxidation states (0.102, 0.144, and 0.270). The Co catalytic sites with multi-valence nature are expected to play different roles during the HER, OER, and ORR and finally synergistically affect its overall electrocatalytic activities, which should be an important characteristic for multifunctional electrocatalysis. Beside the stoichiometry of the catalyst, the formation of heterojunction not only leads to changes in the interfacial coordination environment but also induces charge transfer between the two phases, resulting in the appearance of an internal built-in electric field at the interface. These factors will intensify the diversity and the oxidation state of the active sites significantly, altering their d-band center and the adsorption/desorption characteristics with intermediates and thus contributing to the multi-functional electrocatalytic activities of the catalysts.
Figs. 1a–
c show the optimized geometries of VN, Co
5.47N, and Co
5.47N/VN catalysts. The VN (200) and Co
5.47N (111) surfaces have good lattice matching (
u = 7%,
v = 0.1%), and their interfacial binding energy is ‒1.491 eV/Å
2. This implies that the Co
5.47N/VN heterostructure possesses excellent interfacial stability, which is beneficial for maintaining the structural integrity of the catalyst during the catalytic process and thus its cyclic stability. The electron density difference (EDD) in
Fig. 1d illustrates a redistribution of spatial charge density due to the alteration of interfacial coordination environment, confirming an electron transfer from VN to Co
5.47N. Moreover, the computed WF in
Figs. 1e and
f reveal a lower WF value for VN (3.76 eV) compared to Co
5.47N (4.73 eV), and the macroscopic average electrostatic potential in the bulk VN region (0.72) is also higher than that of Co
5.47N (‒0.94) in
Fig. 1g. Hence, the electron transfer from VN to Co
5.47N induces an inherent electric field at the interface. This result is further substantiated by the Bader charge analysis. Relative to pristine VN surface, the average electron lost for V sites is ~0.05, while Co
5.47N gained 0.16 electrons (Table S2 in Supporting information). In addition, the Bader charges for Co and V sites near the interface both exhibit obvious changes with respect to those in pristine VN and Co
5.47N surfaces. The induced changes in oxidation states of the metal sites will result in their different bonding with the intermediates and thus affect the electrocatalytic mechanisms, which will be discussed in detail below. The electron localization function (ELF) can be used to analyze the electronic characteristics of active sites. In Co
5.47N surface, three different coordination environments for Co atoms are considered, namely isolated CoⅠ, CoⅡ coordinated with individual N atoms, and CoⅢ coordinated with two N atoms. Around CoⅠ and CoⅡ, the electron density is relatively more delocalized compared to CoⅢ (
Fig. 1h and Fig. S2 in Supporting information). The electron density distribution near the V sites in VN also exhibits notable delocalization characteristics. Conversely, the electron density distribution near the N sites in both VN and Co
5.47N displays strong localization. Upon the formation of the Co
5.47N/VN heterojunction, the changes in coordination environments result in obviously diverse ELF distributions near the metal sites at the interface. The electron density around CoⅠ, CoⅡ, CoⅢ, and V at the interface shows higher delocalization compared to the Co
5.47N and VN surfaces. Additionally, the ELF values near the N atoms at the interface experience significant reduction in
Figs. 1i and
j. The enhanced electron density delocalization near the active sites is beneficial for the adsorption and activation of intermediate species, as well as for facilitating charge transfer between them. This is advantageous for reducing charge transfer resistance at the solid-liquid interface and enhancing the activity of the reaction.