Figure 2 shows the XRD patterns of the synthetic pristine NCM622 and TiO2 coating of NCM622 samples. For all the prepared anode samples, 10 strong diffraction peaks were observed in the XRD spectra from 10º to 70º, which correspond to the characteristic peaks (003), (101), (006), (102), (104), (105), (107), (108), (110) and (113) of the typical hexagonal crystalline α-NaFeO2 structure of the R3 space group. No other peaks of impurities was detected, indicating that the addition of TiO2 does not change the phase structure of NCM622 material. The absence of diffraction peaks of TiO2 may be due to the samll amount of TiO2 coating. Sharp and distinct splits between the two sets of split peaks (006)/(102) and (108)/(110) show that the as-prepared samples have a well-developed layered structure. This suggests that the crystal structure of NCM622 is not affected by the TiO2 coating.
Table 1 shows the computed lattice parameters, as well as the intensity ratio of I003/I104. Obviously, with the increase of coating content of TiO2, a and c axes show slightly expansion. The c/a values of all five samples are over 4.9, which indicate that the all obtained NCM622 samples have a layered structure. The larger value of c/a not only represents the better crystallinity of the material, but the 5 wt% TiO2-NCM622 has the largest c/a value and also has the most excellent electrochemical properties.
In addition, the I(003)/I(104) values of bare MCM622, 2%wt, 5%wt, 8%wt TiO2-NCM622 are 1.65, 1.81, 1.83, 1.88, respectively, shown in Table 1. It reveals that as the coating amount of TiO2 increases, the degree of cation mixing in the material increases. Generally, the ratio of I(003)/I(104) indicates the cation mixing of layered structure; when the I(003)/I(104) ratio > 1.2, the materials have a good layered structure with small cation mixing [21, 24].
Table 1
The lattice parameters (a and c) and I(003)/I(104) of the NCM622 and TiO2-coated NCM622 samples
Sample | Lattice parameters | I(003)/I(104) |
a (Å) | c (Å) | c/a |
NCM622 | 2.8619 | 14.1927 | 4.9592 | 1.65 |
2wt% TiO2-NCM | 2.8642 | 14.2036 | 4.9590 | 1.81 |
5wt% TiO2-NCM | 2.8726 | 14.2497 | 4.9606 | 1.83 |
8wt% TiO2-NCM | 2.8769 | 14.2623 | 4.9575 | 1.88 |
The structural and elemental analysis of the 5wt%TiO2-coated NCM622 sample was performed by XPS testing. In Fig. 3(a), the XPS full spectrum of the 5 wt% TiO2-NCM622 sample shows the presence of Ni, Co, Mn, C, O, and Ti elements. As shown in Fig. 3(b), the three peaks at 284.8, 286.4, and 289.3 eV in the C 1s spectrum correspond to C-C, O-C, and O-C = O, respectively, and the XPS spectrum was corrected by the C-C peak (284.8 eV). From the O 1s spectra of Fig. 3(c), it can be seen that there are three distinct peaks located near 529.3, 531.6 and 532.5 eV, which correspond to lattice oxygen, C-O and oxygen in C = O, respectively. Figure 3(d-f) shows the XPS spectra of the elements Ni, Co, and Mn. The peaks located at 855.08 and 872.68 eV correspond to Ni 2p3/2 and Ni 2p1/2, respectively, and the peaks located at 861.58 and 879.18 eV are their satellite peaks, respectively. In the XPS spectrum of element Co, the Co 2p3/2 peak is 780.28 e V and the Co 2p1/2 peak is 795.18 eV, indicating that the valence state of Co is + 3. The main peak of Mn 2p3/2 at 642.58 eV and the Mn 2p1/2 peak observed at 653.98 eV point to the valence state of Mn being + 4. In the spectrum of Ti 2p (Fg.3g) at the binding energies of 458.2, 463.9, and 472 eV correspond to the satellite peaks of Ti 2p3/2, Ti 2p1/2, and TiO2, respectively, suggesting that Ti may exist in the form of TiO2 in the TiO2-coated NCM622 sample [26–27].
Figure 4(a-d) shows the SEM images of the four samples, which all display uniform secondary spherical particles with the size of about 6–8 µm, indicating that the TiO2 coating don’t change the morphology of the samples. Figure 4(e,f) shows the high-resolution TEM of 5 wt% TiO2-NCM, and more uniform TiO2 coating layer on the individual particles can be observed. The sol-gel method can form the uniform layer of TiO2 on the surface of NCM622. The thickness of TiO2 layer is about 5 nm. This nanoscale uniform coating layer can isolate the direct contact between the electrolyte and the active material, reduce the side reactions, and thus improve the electrochemical stability. Moreover, the coating layer can alleviate the structural collapse of the active material due to the volume change caused by delithiation/lithiation during the charging and discharging process, and improve the stability of the layered structure. The EDS results of the 5 wt% TiO2-NCM622 indicte that the distribution of nickel, cobalt, manganese, oxygen, and titanium elements on the sample surface, shown in Fig. 4(g).
Figure. 5 shows the cyclic voltammetry (CV) curves of 5 wt% TiO2-NCM622 samples in the voltage range of 2.5–4.5 V with a scan rate of 0.1 mV/s. The samples with different capping contents have similar CV curves. The oxidation peak appearing near 3.9 V and the reduction peak near 3.6 V correspond to the redox reaction of Ni2+/Ni4+, and the redox peak located in the first-cycle corresponds to the plateau appearing in the first charge/discharge curve. In addition, the oxidation peak moves from the high-voltage position in the first turn to the low-voltage direction in the second and third turns, indicating that the first charging and discharging process is an electrochemical activation process for the material to carry out in order to make the cation arrangement more orderly. Thus is advantageous for the detachment and embedding of lithium ions in the subsequent charging and discharging process, which is manifested by the subsequent decrease in the oxidation peak voltage in the second and third turns [28–30].
The constant current charge-discharge curves, cyclic stability, rate performance of pristine NCM622, 2 wt%, 5 wt% and 8 wt% TiO2-NCM samples are shown in Fig. 6(a-d). In Fig. 6(a-d), apparently, all samples exhibit a plateau region in the first discharge curve, related to the redox reaction between Ni2+/Ni4+, Co3+/Co4+ brought about by deintercalate and intercalate of Li+ ions in the crystal lattice. The first cyclic discharge capacity of the 5 wt% TiO2-NCM622 at 0.3 C is 183.5 mAh g-1, which is higher than that of the pristine NCM622 of 179.2 mAh g-1, and the average Coulombic efficiency (CE) of 5 wt% TiO2-NCM622 can reach 100%. After 100 cycles, the pristine NCM622 show a discharge capacity of 145 mAh g-1, whereas 5 wt% TiO2-NCM622 can maintain a dischaege capacity of 163.9 mAh g-1. The above results indicate that the 5 wt% TiO2-NCM622 has excellent reversible specific capacity than the pristine NCM622.
Figure 6e shows the cycling stability of the pristine NCM622, 2 wt%, 5 wt% and 8 wt% TiO2-NCM samples after 100 cycles at 0.3 C. The cycling stability after 100 cycles at 0.3 C is shown in Table 2, where the 5 wt% TiO2-NCM622 consistently maintains higher capacity and better cycling stability. For the NCM622 electrode, the reversible specific capacity decreases to 145 mAh g-1 after 100 cycles, whereas the 5 wt% TiO2-NCM electrode, still release a reversible specific capacity of 163.9 mAh g-1 after 100 cycles, with a total capacity retention rate of 89.3%.
The multiplicity performance of the samples is shown in Fig. 6(f). In general, the TiO2-NCM electrodes exhibit better rate performance, compared with bare NCM622. The 5 wt% TiO2-NCM622 sample exhibits best multiplicity performance, with a discharge specific capacity of average 70 mAh g-1 at a rate of 10.0 C, compared with ~ 35 mAh g-1 for bare NCM. The 8 wt% TiO2-NCM622 sample exhibits worst rate performance, indicating larger coating content of TiO2 is dverse to the enhancement of electrochemical performance. The appropriate TiO2 coating of NCM622 has lowest cation mixing and highly ordered lamellar structure, which is conducive to the dislodgement and embedding of Li-ions, and the diffusion kinetics of Li-ion is faster, thus the sample has best rate performance. The as-synthesized 5 wt% TiO2-NCM622 exhibits best electrochemical performance compared with other TiO2-coated NCM622 electrodes, as shown in Table 2.
Table 2
The discharge specific capacity and coulombic efficiency of NCM622 and TiO2-coated NCM samples at 0.3 C.
Sample | Discharge Specific Capacity (mAh g− 1) | Columbic Efficiency (%) |
1st | 100th |
NCM622 | 179.2 | 145 | 80.9 |
2 wt% TiO2-NCM | 181.9 | 151 | 83.0 |
5 wt% TiO2-NCM | 183.5 | 163.9 | 89.3 |
8 wt% TiO2-NCM | 178.7 | 135.3 | 75.7 |
To verify the electrochemical performance of the modified material under higher voltage, the cyclic performance of NCM622 and 5 wt% TiO2 NCM622 electrodes was tested under the cutoff voltage of 4.6 V at a higher rate of 0.5 C, as shown in Fig. 7. The initial discharge capacities of NCM and 5 wt% TiO2-NCM622 electrodes are ~ 200 and 205 mAh g-1, respctively. The cycling performance of the 5 wt% TiO2 NCM622 electrode is improved, compared with bare NCM622. After 150 cycles, the 5 wt% TiO2-NCM622 electrode shows a specific capacity of 107.3 mAh g-1, which is higher than that of 80.8 mAh g-1 of the bare NCM622. Therefore, after TiO2 coating, the harmful effects of the modified material under higher voltage are also suppressed to a certain extent, similar to the reslts measured at a cut-off voltage of 4.3 V. However, under the higher cutoff voltage, the capacity retention of NCM622 and TiO2 coating of NCM622 after 150 cycles is unsatisfied, indicating only TiO2 coating of NCM622 cannot totally suppress the interface reaction between the cathode and electrolyte and reduce the interface resistance[8, 31].
To further investigate the electrochemical kinetics of the samples, the electrochemical impedance spectroscopy (EIS) tests were performed in the range of 0.01 Hz-100 KHz. As shown in Fig. 8(a), the Nyquist plots of pristine NCM622, 2 wt%, 5 wt%, and 8 wt% TiO2-NCM622 samples all contain two cross-sections, which are the high-frequency region and low-frequency region cross-sections, respectively. The semicircle in the high-frequency region corresponds to the charge transfer resistance (Rst), and the larger the diameter of the semicircle is, the larger the charge transfer resistance is. The specific Rst values are shown in Table 4. It can be found that the 5 wt% TiO2-NCM622 electrode has the smallest charge transfer resistance. The straight line in the low-frequency region corresponds to the Warburg resistance (Aw) of the diffusion of Li-ion inside the electrode, and the larger the slope is, the larger is the Warburg resistance, as in Fig. 8(b). The Warburg coefficients of the three electrodes, NCM622, 2 wt% TiO2-NCM, 5 wt% TiO2-NCM, and 8 wt% TiO2-NCM, are 38.29, 28.71, 23.93, and 52.65 Ω s-1/2, respectively, by fitting, which proves that the 5 wt% TiO2-NCM622 has a faster electrochemical kinetics.
Table 4
The Charge transfer resistance (Rst) of NCM and TiO2-coated NCM samples
Sample | NCM622 | 2 wt% TiO2-NCM | 5 wt% TiO2-NCM | 8 wt% TiO2-NCM |
EIS(Ω) | 191 | 142 | 113 | 258 |
Table 5 shows a comparison of the partial electrochemical performance of TiO2-coated NCM with the previously reported electrochemical performance of partial coating NCM cathodes in LIBs.
Table 5
Comparison of electrochemical performances of part of coated LiNi0.6Co0.2Mn0.2O2 (NCM) with previously work reported for LIBs.
Samples | Rate (C) / Cutoff voltage (V) | Cycles | Capacity (mAh g–1) / Retention (%) |
ZrO2 modified NCM [17] | 0.1 / 2.8–4.5 | 100 | 154.8 / 82.5 |
TiO2-modified NCM [23] | 1.0 / 2.5–4.3 | 100 | 163.6 / 85.9 |
Li2SnO3 coating NCM [26] | 1.0 / 3.8–4.5 | 100 | 136.2 / 85.94 |
AlPO4 coating NCM [20] | 1.0 / 2.8–4.3 | 50 | 135.5 / 86.2 |
Mn3(PO4)2 coating NCM [22] | 0.5 / 3-4.3 | 50 | 149 / 93.3 |
5wt% TiO2-NCM (This work) | 0.3 / 3-4.3 | 100 | 163.8 / 89.3 |
5wt% TiO2-NCM (This work) | 0.5 / 3-4.6 | 150 | 107.3/53.5 |