The crystalline phase and chemical composition of calcined powder samples are identified by XRD. The results prove that the precursor is successfully converted into the desired oxidation products. As shown in
Fig. 2a, Co-MOF and Ni-MOF are converted into pure spinel Co
3O
4 and NiO, respectively, which corresponds to the standard patterns (PDF#43-1003 and PDF#47-1049) well. Furthermore, the NiCoO-n products obtained by corresponding Ni-Co-MOF-n match the standard pattern of NiCo
2O
4 and Co
1.29Ni
1.71O
4 with spinel structure (PDF#20-0781 and PDF#40- 1191), and almost no other phases or impurities are detected. Pure NiO can be observed in NiCoO-n, which indicates that Ni atoms have been well integrated into Co
3O
4 lattice. The results are consistent with the SAED. To investigate more detailed elemental composition and valence of obtained N-Co
3O
4, N-NiCoO-n and N-NiO products, X-ray photoelectron (XPS) measurements are conducted. The survey spectrums in Fig. S9 (Supporting information) once again substantiate the subsistence of Ni, Co, C, N and O in these products. Ni 2p spectrums comprise two main peaks including Ni 2p
3/2 and Ni 2p
1/2. Fitting peaks at 853.85 and 871.09 eV correspond to Ni
2+, while those at 855.66 and 872.88 eV correspond to Ni
3+ (
Fig. 2b) [
34]. In these four spectra, the amount of Ni
3+ is higher than Ni
2+, which can form the active redox center Ni
2+/Ni
3+, and with the increase of Ni content, the Ni
2+ fitting peak intensity of 2p
3/2 increases. It is possible that the formation of NiO gradually exhausts the Co positions on the surface of N-NiCoO-n hexagonal nanoplates [
42]. Similarly, the Co 2p spectrums in
Fig. 2c consist of two spin orbit double peaks with the characteristics of Co
2+ (781.50 eV for 2p
3/2, 796.67 eV for 2p
1/2) and Co
3+ (779.51 eV for 2p
3/2, 794.78 eV for 2p
1/2) and two satellite peaks [
43]. As the Ni content increases, the Co
2+ fitting peaks intensity of 2p
3/2 decreases. The O 1s spectrums (Fig. S10 in Supporting information) show three different oxygen characteristics. Specifically, the binding energies of the three fitting peaks are 529.88 eV, 531.21 eV and 532.70 eV respectively, which can be attributed to metal oxygen (O
1), oxygen defect (O
2) and chemisorption oxygen (O
3) [
44,
45]. The N 1s spectrums (
Fig. 2d) can also be divided into three fitting peaks centered on the binding energy of 399.30, 400.50 and 403.60 eV, corresponding to pyridine nitrogen (N
1), pyrrole (N
2) and Pyridine-N-oxide (N
3), respectively [
46]. It is reported that the combination of pyridine nitrogen (N
1) and pyrrole nitrogen (N
2) contributes to better pseudocapacitors [
14]. In order to obtain the specific surface area of the samples, the porous texture of N-Co
3O
4, N-NiCoO-n and N-NiO is indagated by N2 adsorption-desorption isotherms. The specific surface area values for all samples are summarized in Table S1 (Supporting information). As shown in Fig. S11 (Supporting information), the isotherms are all of type IV curves with hysteresis loops at a relative pressure of 0.8–1.0, meaning that there are a large number of mesopores in nitrogen-doped metal oxides. The pore size distribution (Fig. S12 in Supporting information) for the BarrettJoyner-Halenda adsorption branch of five products further displays sharp peaks was observed around 3.50 nm and a broad peak begin to appear around 20 nm. These results clearly indicate the presence of micro, mesopores and even macropores in the products.