3.1. The Crystal Structure of the Cathode Material with ZnO Coating
Table 1 represents the zinc content of ZnO-coated LiNi
1/3Co
1/3Mn
1/3O
2 cathode powder measured by vacuum induction-coupled plasma mass analysis and ICP analysis. The samples without ZnO coating, denoted as a, and those with 1 % and 2 % ZnO coating, denoted as b and c, respectively, show that the ZnO content closely matches the design values.
Figure 1 displays the XRD spectra of LiNi
1/3Co
1/3Mn
1/3O
2 cathode materials with different ZnO coatings. From
Figure 1, it can be observed that the ZnO coating does not alter the crystal structure of the LiNi
1/3Co
1/3Mn
1/3O
2 material. The XRD spectra of the three materials are very similar, indicating a typical layered oxide structure, namely nano-NaFeO
2 structure, belonging to the R-3m space group with no noise. The characteristic peaks of ZnO are not detected in the spectra, likely due to the difficulty of detection caused by the low ZnO content. Only when the ZnO coating exceeds 4 %, the characteristic peaks of ZnO are observed.
Suggest that the XRD spectra intensity ratio of (003) and (104) diffraction peaks, denoted as I003/I104, can be used to indicate the degree of cation mixing in the nickel-cobalt-manganese ternary layered material structure. If I003/I104 is greater than 1.2, it indicates a lower degree of cation mixing, a more stable layered structure, and superior electrochemical performance[
10]. The calculated values of I003/I104 for a, b, and c are 1.5, 1.3, and 1.4, respectively, indicating that the layered structure of the three materials is very good and the degree of cation mixing is extremely low. Additionally, use the (I106 + I102)/I101 ratio to indicate the order of the hexagonal lattice. A smaller value represents a higher order of the hexagonal lattice. The calculated values of (I106 + I102)/I101 for a, b, and c are 0.44, 0.48, and 0.48, respectively. Although the (I106 + I102)/I101 value of a is the smallest, after ZnO coating, it indicates a decrease in the crystal lattice order of the material, suggesting the possibility of some Zn atoms entering the lattice.
Table 2 shows that the binding energies of Zn 2p3/2 and Zn 2p1/2 in sample c are 1022.1 eV and 1045.4 eV, respectively, which are similar to the previously reported values for ZnO (1022.5 eV and 1045.5 eV) [
11]. This indicates that the major zinc species present on the surface after the ZnO coating are zinc ions. As a result, the binding energies of excessive metallic Ni
2+, Co
3+, and Mn
4+ increase.
Table 2 also demonstrates the matching of the energy values of peak 1 and the binding energies of Ni
2+, Co
3+, and Mn
4+, while peak 2 represents the increased binding energy. In sample c, energy values of 642.7 eV corresponding to 70 % manganese, 781.9 eV corresponding to 25 % cobalt, and 856.7 eV corresponding to 33 % nickel are observed. XPS chemical shifts reflect different bonding environments of elements, so the presence of high binding energy components of excessive metals could be due to value appreciation or the formation of new compounds, such as LiAlCoO
2, where the addition of Al leads to an increased binding energy of Co [
12].
Table 3 presents the molar ratio test results of surface elemental compositions for the three materials. Assuming that Zn
2+ from ZnO is entirely diffused into the material, the Zn/Co molar ratios for 1 % and 2 % ZnO coatings would be 0.035 and 0.071 on average, respectively. However, based on the surface Zn/Co molar ratios obtained from XPS testing in
Table 3, it can be inferred that Zn
2+ did not fully diffuse into the LiNi
1/3Co
1/3Mn
1/3O
2 lattice but mostly distributed on the particle surface.
Furthermore, on the surface of LiNi
1/3Co
1/3Mn
1/3O
2, the transition metal ratios deviated from the chemical formula composition, with higher nickel and manganese contents. There are also findings regarding the difference between surface composition and crystal interior of the cathode material [
14], but after ZnO coating, the nickel and manganese contents increased on the surfaces of materials a and b compared to material a alone. Moreover, these contents increased as the coating amount increased. These changes are clearly associated with the presence of ZnO on the material surface. The analysis indicates that, after ZnO coating, the surface of the material exhibits increased nickel and manganese contents, which further increase with higher coating amounts. Therefore, it is presumed that the high binding energy portion of surface transition metals is possibly attributed to the formation of a complex oxide (Zn, Ni, Mn)O through the combination with zinc.
3.2. Electrochemical Characteristics
Swag-type batteries assembled with materials a, b, and c underwent charge-discharge testing at room temperature and 55 ℃. Initially, a cycling test was conducted at a rate of 0.1 C for two weeks, followed by cycling at a rate of 0.5 C.
Figure 2 represents the initial charge-discharge curve at 0.1 C, and
Figure 3 shows the capacity retention curve after 50 cycles at 0.5 C.
For material a, the initial discharge capacity at 0.1 C is 183/16498 mAh/g, with an initial Coulombic efficiency of 89.4 %. After 50 cycles, the capacity of battery a decreased from 126.8 mAh/g to 125.8 mAh/g, resulting in a capacity retention of 99.2 %. The inclusion of ZnO at different amounts in batteries b and c resulted in a decrease in the initial discharge capacity compared to battery a. This could be attributed to ZnO being electrochemically inactive and not participating in the battery reaction. The ZnO coating layer formed on the surface may hinder the diffusion of lithium ions, thereby reducing the initial discharge capacity.
The 0.5 C discharge capacity of battery b is similar to battery a, while battery c exhibits relatively lower discharge capacity. This suggests that the benefits of ZnO coating were not evident in the room temperature discharge.
The initial charge-discharge curves at 55 °C and 0.1 C for batteries a, b, and c are depicted in
Figure 4. At 55 °C, the charge-discharge capacity of battery a increased to 232.9/155.4 mAhg-1 compared to the capacity at room temperature. This can be attributed to faster ion diffusion, allowing for more Li
+ insertion/extraction. However, the initial cycle efficiency was low at 66.7 %, indicating increased side reactions on the surface of the active material, in addition to some Li
+ consumption associated with the thickened solid-electrolyte interface (SEI) layer. These additional reactions on the surface of the active material are considered major side reactions, leading to electrolyte decomposition, metal dissolution, or oxidation within the active material, which can cause structural degradation [
15].
Batteries b and c, on the other hand, exhibited slightly decreased discharge capacities of 134.6 mAhg-1 and 158.3 mAhg-1, respectively, but with improved initial efficiencies. They achieved efficiencies of 67.8 % and 74.0 %, respectively. This suggests that the appropriate amount of ZnO coating can suppress some side reactions by preventing direct contact between the electrode material and the electrolyte, thereby enhancing the initial efficiency.
The initial charge-discharge curves for batteries a, b, and c are presented in
Figure 5. In the oxidation curve, a reaction was observed around 3.7~3.9 V, and battery a exhibited a reaction even at 3.6 V. However, in the reduction curve, the corresponding reaction peak was not observed, indicating its irreversibility. This reaction can be attributed to byproduct reactions on the surface of the active material or SEI formation and growth. Battery b showed a small irreversible reaction peak near 3.6 V in the oxidation curve, while this peak was less distinct in battery c, indicating the lowest irreversible capacity.
This is consistent with the initial efficiency results and suggests that an appropriate amount of ZnO coating modifies the surface state of LiNi1/3Co1/3Mn1/3O2 material, suppressing irreversible reactions around 3.6 V.
The cycling lifespan curves at 55 °C/0.5 C for batteries a, b, and c are shown in
Figure 6. The initial cycling discharge capacity for battery a is 129.7 mAh/g, and the capacity retention after 50 cycles is 96.7 %. The initial cycling capacities for batteries b and c are 127.2 mAh/g and 136.9 mAh/g, respectively, and the capacity retentions after 50 cycles are 95.8 % and 96.4 %, respectively. The differences in capacity retention among the three materials are not significant, with all of them being approximately 96 %. This indicates that the cycling lifespan of the LiNi
1/3Co
1/3Mn
1/3O
2 material is excellent under typical cutoff voltage and low-rate conditions (C/2, below 4.2 V), and the ZnO coating did not alter this characteristic.