Surface-Coated LiNi0.8Co0.1Mn0.1O2 (NCM811) Cathode Materials by Al2O3, ZrO2, and Li2O-2B2O3 Thin-Layers for Improving the Performance of Lithium Ion Batteries

In this paper, the precursor Ni0.8Co0.1Mn0.1(OH)2 is prepared by a co-precipitation method. By mixing this material with LiOH in proportion and sintering twice under 500℃ and 800 ℃, respectively, the cathode material of LiNi0.8Co0.1Mn0.1O2 (NCM811) for lithium ion batteries (LIBs) is synthesized. To improve the performance of this NCM811 material, Al2O3, ZrO2 and LBO (Li2O-2B2O3) are respectively used to coat it by a wet chemical method. The effects of Al2O3, ZrO2 and LBO thin coating layers (~20～200 nm) on the morphology, structure and electrochemical property of NCM811 are studied using XRD, SEM, TEM, XPS, and electrochemical measurements. Coin LIBs are assembled with the uncoated, Al2O3-coated, ZrO2-coated and LBO-coated NCM811 cathode materials for performance validation. The experiment results confirm that the charge-discharge specific capacity, Coulomb efficiency, water absorption stability, cycle characteristics and resistance stability of the NCM811 cathode material can be significantly improved by coating it with LBO particularly. Therefore, the surface coating to the particles of cathode materials using LBO is expected to be an effective and practical modification method to improve the electrochemical performance of LIBs.


INTRODUCTION
Electrochemical energy technologies, such as lithium-ion batteries, metal-air batteries, fuel cell, and water electrolysis, etc., have been recognized as one type of the most reliable and efficient options for clean and sustainable electricity energy storage and conversion Wang et al., 2018;Zhang H. et al., 2018;. For relatively mature lithium-ion batteries (LIBs), the cathode materials play a dominating role in the performance of LIBs. In order to further increase energy densities of the devices, high-nickel NCM-based materials such as LiNi x Co y Mn z O 2 (here x+y+z = 1 with x>y+z) family have been explored and used in LIBs. It seems that one of the most promising LIB cathode materials is LiNi 0.8 Co 0.1 Mn 0.1 O 2 (NCM811, where x = 0.8, y = 0.1, and z = 0.1), which shows higher specific capacity than other family members Li Q. et al., 2018).
In general, for high-nickel NCM-based materials, there are several shortcomings which have been identified. (1) Li + /Ni 2+ mixing when Ni 2+ content is increased. In high-nickel NCM-based material, part of Ni 2+ may occupy the Li + position, forming a cation mixing and then reducing the specific capacity of material. Furthermore, during the charging process, the lowvalence nickel ion in the transition metal (Co, Mn) layer can migrate to the lithium layer, occupying the lithium vacancies, affecting the diffusion of Li + . The voltage stability of the material is also relatively weak, which is easy to decline rapidly (Noh et al., 2013;Li et al., 2019;Zhang et al., 2019). (2) Poor thermal stability. Studies have shown that the higher the nickel content in the ternary material, the worse the thermal stability, causing safety issue (Aurbach, 2000;Ma et al., 2019). (3) Unstable surface structure. The excessive delithiation occurs in the surface structure with charging, and the layered structure of the highnickel NCM-based material changes to the spinel structure and the inert rock salt structure with a hicker inert NiO layer. Furthermore, the high-valent active transition metal ions on the surface layer can have side reactions with the electrolyte, causing the increase of polarization and then the decay of the capacity (Noh et al., 2006). (4) Too high surface alkali content. The nickel element in the NCM-based material is alkaline, which is easy to absorb water and CO 2 when exposed to air and reacts with residual lithium in the surface layer to form LiOH and Li 2 CO 3 , which can further increase the pH value of the material and seriously affect the electrochemical performance of the NCM-based material (Bi et al., 2016). In recent years, many improvements have been carried out for high-nickel NCM-based materials of LIB cathodes, including innovating the synthesis processes, doping modification, and matching of microstructure with electrolyte. There are mainly two methods to improve the performance of high-nickel NCM-based materials.
(1) Element doping for improving the cationic mixing and lattice stability, such as doping Mg, Al, Zr, and other components into materials to improve the cycling performance (Nobili et al., 2012;Min et al., 2017). (2) Coating the material particles with electrochemically inert materials to prevent or suppress the side reactions between the cathode surface and electrolyte, and improve the particles' structural stability for enhancing the cyclelife of the corresponding LIBs. The commonly used physical protective coating materials are Al 2 O 3 (Chen et al., 2019), MgO (Yoon et al., 2012), CeO 2 , ZrO 2 (Li G. et al., 2018), Co 3 O 4 (Hao et al., 2019), etc. The common feature of these coatings is that their metal ions have only one stable valence state with high chemical stability under the electrochemical window conditions. Of course, the coating also have some shortcomings, because as the insulators of ions and electrons, they may have a negative impact on the transport of lithium ions, thereby affecting or reducing the Coulombic efficiency, power output, and other electrochemical properties of LIBs.
In addition to the above lithium-free metal oxides used as coating materials for cathode materials, some researchers have employed lithium-containing Li 2 ZrO 3 (Dong et al., 2015), Li 3 PO 4 (Song et al., 2011), Li 2 O-2B 2 O 3 (LBO) (Chan et al., 2005;Lim et al., 2014;Song et al., 2019) to coat cathode materials. These lithium-containing compounds, in particular, conductive LBO can maintain stable electrochemical properties at high oxidation potential. LBO coating has shown a good ionic conductivity, which makes the coated cathode materials more conducive to lithium ions, thus leading to better electrochemical properties. It has been reported in the literature that the surface coatings of LBO glass on LiNi 0.5 Mn 1.5 O 4 (Lim et al., 2014), LiNi 0.5 Co 0.2 Mn 0.3 O 2 , and LiMn 2 O 4 (Chan et al., 2005) cathodes can make remarkable improvements in charge-discharge behavior, cycle-life and other electrochemical properties. The influence of coating on the electrochemical properties of cathode materials is shown in Table 1. However, there are a few of researches reporting about the coating of LBO on LiNi 0.8 Co 0.1 Mn 0.1 O 2 (NCM811) cathode material.
In this work, NCM811 cathode material is prepared by a coprecipitation method. In order to improve the electrochemical properties, several materials such as Al 2 O 3 , ZrO 2 , and LBO are used, respectively, to coat NCM811 for LIB cathode materials. The microstructures and morphologies of the coated NCM811 materials are characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscope (TEM) and X-ray photoelectron spectroscopy (XPS). The coated NCM811 materials as the cathodes are assembled in coin LIBs for performance validation. The effects of different coatings on the electrochemical properties of NCM811 are studied by testing the charge/discharge curves and Coulomb efficiencies, cycle performance and DC resistances of the corresponding coin LIBs.

EXPERIMENT Preparation of NCM811 Material
According to a molar ratio of 8:1:1 (Ni: Co: Mn metal ions), nickel sulfate (NiSO 4 ·6H 2 O), cobalt sulfate (CoSO 4 ·7H 2 O), manganese sulfate (MnSO 4 ·2H 2 O) were, respectively, weighed and added into deionized water and stirred evenly, and a mixed solution with a total concentration of metal ions of 0.5 mol/L was prepared. The mixed solution was placed in the reactor, and 1 mol/L NaOH solution as the precipitator and 0.5 mol/L ammonia solution as the complexing buffer were added continuously. The whole reaction process was carried out in a N 2 atmosphere for insulating air. The pH value of the mixed solution was controlled from 10.5 to 11.5, and the temperature of reactor was controlled at 55 • C under a continuously stirring for 24 h. The obtained precipitates were filtered and washed with deionized water after 4 h of static aging, and then dried in a vacuum drying chamber at 95 • C for 24 h to obtain the gray-brown precursor Ni 0.8 Co 0.1 Mn 0.1 (OH) 2 . LiOH·H 2 O and this precursor were weighed according to the molar ratio of 1.04:1. The weighted mixture was then grinded evenly, calcined at 500 • C for 4 h and cooled for 1 h in a muffle furnace. Then the black LiNi 0.8 Co 0.1 Mn 0.1 O 2 (NCM811) powder was obtained by continuous calcination in a tube furnace protected by oxygen gas at 85 • C for 16 h.

Preparation of NCM811 Coated With Al 2 O 3 , ZrO 2 , and LBO by Wet Processes
For Al 2 O 3 coating, Al(NO 3 ) 3 ·9H 2 O was weighed for forming a solution of with 0.05 ml/L of Al 3+ . Then a total concentration of 1 mol/L Al(NO 3 ) 3 ·9H 2 O and CO(NH 2 ) 2 with a molar ratio of 1: 1.15 was prepared. The pure phase NCM811 was weighed in a beaker with a proper amount of deionized water added to disperse it into a uniform solution by ultrasound. Then, according to the amount of coated Al 2 O 3 of 1,000 ppm (Weight proportion of the coated substance calculated based on the content of substance Al 2 O 3 ), the quantitative solution of Al(NO 3 ) 3 ·9H 2 O was slowly added into NCM811 dispersion solution, and stirred for 1 h. The suspension of NCM811 deposited by Al(OH) 3 was obtained by heating at 85 • C in a water bath for 4 h under a rapid stirring. The obtained mixture was filtrated and washed with deionized water, then dried in a vacuum drying box at 100 • C for 24 h. Then a heat treatment at 500 • C was carried out for 4 h. Finally, the NCM811 coated with Al 2 O 3 was obtained by naturally cooling, grinding and calcinating in a muffle furnace at 800 • C for 8 h in air atmosphere. For ZrO 2 coating, an appropriate amount of NCM811 material was weighted and put into a beaker with deionized water, stirring for 1 h. Then, citric acid (C 6 H 8 O 7 ·H 2 O) and zirconium acetate (Zr(CH 3 COO) 4 ) with a molar ratio of 1:1 were dissolved in the deionized water. The sum molar concentration of these two compounds in solution was 0.1 mol/L. According to the designed weight content of 1,000 ppm ZrO 2 in NCM811 (calculated based on the content of substance ZrO 2 ), the mixed citric acid and zirconium acetate solution are slowly added to NCM811 suspension. The beaker was then heated in water at 55 • C with stirring for 8 h to form a solution. This solution was then evaporated until a gel was obtained. This gel was then dried in a vacuum drying chamber at 100 • C for 24 h to obtain a solid sample. After grinded, the product was heat treated at 500 • C for 4 h. Finally, the product of NCM811 coated with ZrO 2 was obtained by calcining it in a muffle furnace at 800 • C for 8 h in air atmosphere.
For LBO coating, LiOH·H 2 O and manganic acid (H 3 BO 3 ) were added to alcohol at a molar ratio of 1:2. The above substances were completely dissolved after being heated in a water bath at 85 • C for 4 h. After dissolution, the prepared uncoated NCM811 powder was added, and the quantity of the added NCM811 was controlled according to coated 1,000 ppm of LBO (calculated based on the content of substance LBO). The formed mixture was stirred until the alcohol was evaporated completely to form a solid sample. Then the solid sample was calcined in a muffle furnace at 500 • C for 4 h in oxygen atmosphere, and the heating rate of the muffle furnace was 5 • C/min. Then NCM811 with Li 2 O-2B 2 O 3 (LBO) coating was obtained by natural cooling, grinding and calcination at 800 • C for 8 h in a muffle furnace under air atmosphere.
In this paper, NCM811 without any coating is represented by A, and the samples of NCM811 coated with 1,000 ppm of Al 2 O 3 , ZrO 2 , and LBO are represented by B, C, and D, respectively. The preparation routes for samples of NCM811 coated by Al 2 O 3 , ZrO 2 , and LBO are shown in Figure 1.

Characterization of the Materials
The crystal structures of the samples were analyzed by Xray diffractometer (XRD) (D/max-250, made in Japan) with the Kα radiation of copper target obtained with a wavelength of 0.153 nm, a tube voltage of 40 kV, a tube current of 250 mA, a diffraction angle scanning range of 10-80 • and a scanning speed of 8 • /min. The morphologies of the samples were observed by FEI Quanta-200 (manufactured in the Netherlands) field emission scanning electron microscopy (FE-SEM) with a voltage of 5 kV. The morphologies of the samples were also analyzed by JFM-2100 transmission electron microscopy (TEM) (Japan Electronics Production). X-ray photoelectron spectroscopy (XPS) was carried out on an Escalab 250xi X-ray photoelectron spectrometer.

Fabrication of Coin LIBs and the Electrochemical Performance Measurements
In a typical fabrication of LIBs, NCM811, or a coated NCM811 sample, conductive carbon black (Super-P) and polyvinylidene fluoride was weighed at a mass ratio of 90:5:5 and placed in an agate mortar. After it was grinded and mixed uniformly, an appropriate amount of polypyrrolidone (NMP) was added and grinded for 2 h until the slurry was reached to a flow state. The slurry was then evenly coated on a 12 µm thick aluminum foil to form an electrode sheet. In order to remove the NMP solvent, the electrode sheet was placed in a vacuum oven and dried at 120 • C for 12 h. Then the dried electrode was punched and cut into a 14 mm disc. After weighed, this disc electrode (serves as the cathode) was placed in the vacuum drying box at 60 • C for 8 h, and then removed and placed in the glove box protected by argon. The prepared cathode sheet, separators (produced by Shenzhen Xing-yuan Material Co., Ltd., 16 µm thick), negative lithium foil (lithium sheet with diameter of 15 mm and thickness of 0.3 mm), electrolyte (model RT, produced by Guangzhou Tianci High-tech New Materials Co., Ltd.) were assembled into a R2032 coin LIB. All coin LIBs made from NCM811 and the coated NCM811 by Al 2 O 3 , ZrO 2 , and LBO were assembled in an argon glove box with oxygen and hydrogen peroxide content <1 ppm.
For water adsorption testing, the tested cathodes of NCM811 and NCM811 coated by Al 2 O 3 , ZrO 2 , and LBO were placed in a humidity of 10% RH and stored in an ambient temperature of 25 • C. The total storage time was 72 h, and the water contents of the electrodes were measured at an 8 h interval. The moisture values of the electrodes were measured by a moisture tester (CA200/VA200, Mitsubishi Chemical Company, Japan). The temperature of the tester was controlled at 170 • C.
The measurements of electrochemical performance of the coin LIBs were carried out using an electrochemical testing system (Land CT2001A, Wuhan land electronic Co., Ltd.). The current densities of the first charge and discharge are both 18 mA/g (0.1C). In the charge-discharge cycling tests of coin LIBs, the charging current density was 90 mA/g (0.5C) and the discharging current was 180 mA/g (1C), respectively. The tested voltage range was 2.8-4.3 V (vs.Li/Li + ), and the static time between the charging and discharging processes was 30 min. All the tests were carried out at 25 • C. DC resistance tests followed the instruction of HPPC test method in a Freedom Car Battery Testing Manual (Belt, 2010). This work used 0.5C current to charge coin batteries to different SOC states (100% SOC), and then used a charge current of 1C and charging time of 10 s to obtain DC resistances of the coin LIBs at 100% SOC states. Figure 2 Shows the XRD spectra of uncoated and differently coated NCM811 materials. It can be seen that the pure phased and differently coated NCM811 materials have good a hexagonal α-NaFeO 2 layered structure and a R-3m space point group. The main peaks in the XRD spectra of the coated materials are identical, which indicates that the coated materials do not change the layered structure. In addition, the peaks of 006/102 and  108/110 can be observed from XRD spectra, indicating that the pure NCM811 and the coated NCM811 samples both have a good crystallinity and an ordered layered structure (Li et al., 2014). No characteristic peaks of the coated materials of Al 2 O 3 , ZrO 2 , and LBO can be found in the XRD spectra of the coated NCM811 materials. There were no obvious differences in the location and intensity of the diffraction peaks between pure phase material and the coated materials, and no new diffraction peaks can be observed. These can be explained by that the coated material layer does not change the original lattice structure of the bulk material, and that the coated materials of Al 2 O 3 , ZrO 2 , and LBO are amorphous, and only adhere to the surface of the bulk materials as the coating layers.

RESULTS AND DISCUSSION
From the SEM images shown in Figure 3, it can be seen that the appearances of uncoated and the coated NCM811 samples are basically similar, and they are spheroids bound by the secondary solid particles. The particle size range of the secondary sphere is 3-16 um. Figure 4 shows the TEM images of NCM811 and the coated NCM811 samples. Figure 4A is a NCM811 sample without any coating. The surface of the uncoated material is smooth and there is no coating layer that can be observed. Figure 4B is a TEM image of the NCM811 coated with Al 2 O 3 . The surface of NCM811 has a coating layer with a thickness of 20-80 nm. Figure 4C is a TEM image of the NCM811 coated with ZrO 2 . The thickness of the coating layer is 20-120 nm. Figure 4D is a TEM image of the NCM811 coated with LBO. The coating layer is 50-200 nm thick. For the layered cathode material, the coating layer can reduce the undesired reaction between cathode material and electrolyte and suppress lattice distortion caused by the dissolution of transition metal ions into electrolyte during charging (Zuo et al., 2017). It is expected when NCM811 is coated by a layer, the cathode could be protected, benifiting batttery performance.
In order to further confirm the composition of NCM811 and NCM811 coated by Al 2 O 3 , ZrO 2 , and LBO, the prepared samples were characterized by XPS, as shown in Figure 5. The characteristic binding energies of Co2p 3/2 , Mn2P 3/2 , and Ni2P 3/2 can be seen from Figures 5A-C, which are 780.04, 641.99, and 854.69 eV, indicating that the valence states of Co, Ni and Mn are +2, +3, and +4, respectively (Tan et al., 2015). The characteristic peak of 73.8 eV can be found only for NCM811 coated with Al 2 O 3 (Sample B) (Figure 5D), which corresponds to the characteristic binding energy of Al2p 3/2 of Al 2 O 3 (Wen et al., 2018). The XPS spectrum of Zr3d include two peaks: Zr3d 5/2 (181.75 ev) and Zr3d 3/2 (184.25 ev), which are in good agreement with the values in literature (Huang et al., 2009). Boron can only be detected on sample of NCM 811 coated with LBO, as shown in Figure 5F. The characteristic binding energy of B1S is 191.83 eV. This is consistent with the binding energy of LBO (Li 2 O-2B 2 O 3 ) in literature . XPS results show that Al 2 O 3 , ZrO 2 , and LBO have been successfully coated on the surface of MCM811, respectively.
From Figure 6 and Table 2 above, it can be seen that the first charge specific capacity of coin LIB made of the uncoated NCM811 sample (A) is 229.2 mAh/g, the first discharge specific capacity is 201.7 mAh/g and the first charge-discharge Coulomb efficiency is 88.00%, respectively. The first charge specific capacity of coin LIB made of the NCM811 coated by Al 2 O 3 (B) is 226.3 mAh/g and the first discharge specific capacity is 199.2 mAh/g. The first charge-discharge Coulomb efficiency is 88.02%. These data indicate that the first charge-discharge specific capacity of NCM811 is negatively affected by Al 2 O 3 coating, but the first charge-discharge Coulomb efficiency is slightly increased. For the coin LIB made of NCM811 coated with ZrO 2 (C), the first charge specific capacity is 225.7 mAh/g, the first discharge specific capacity was 198.7 mAh/g, and the first charge-discharge Coulomb efficiency was 88.04%, respectively. The first charge and discharge capacities of NCM811 coated with ZrO 2 is slightly lower than that of NCM811 without any coating, but the first charge and discharge Coulomb efficiency is increased slightly, which is consistent with that of Al 2 O 3 coating. The first charge specific capacity of coin LIB made of NCM811 coated with LBO (D) is 230.0 mAh/g, the first discharge specific capacity is 204.3 mAh/g, and the first charge-discharge efficiency is 88.83%, respectively. These results are higher than those of both coated by Al 2 O 3 and ZrO 2 . It is presumed that this may be due to the lack of electrochemical activity of both Al 2 O 3 and ZrO 2 coating, which may hinder the insertion/removal of some Li + ions, resulting in a slight decrease in the specific capacities of charge/discharge. However, the surface interface structure of NCM811 can be stabilized by Al 2 O 3 or ZrO 2 coating layer, and the reaction between the electrode material and the electrolyte can be restrained to some extent. As a result, the Coulomb efficiencies of charge/discharge are improved. In addition to the advantages of normal surface coatinging layer, LBO as a fast ionic conductor has a good ionic conductivity and certain electrochemical activity when it is coated on the surface of NCM811. It is conducive to the transport of lithium ions during charging and discharging. This is an important reason why LBO coating layer has a better electrochemical performance than Al 2 O 3 and ZrO 2 coatings. The first charge capacity, discharge capacity and Coulomb efficiency of NCM811 coated with LBO (D) are slightly higher than those of NCM811 without any coating, and also better than those of NCM811 coated with Al 2 O 3 and ZrO 2 .
From Figure 7 and Table 3, it can be seen that the water values of the electrode made of NCM811 (A) without any coating rises from 215.1 ppm to 670.2 ppm when it is stored at room temperature for 72 h at a relative humidity of 10% RH. It can be found that the water contents of the uncoated, Al 2 O 3 , ZrO 2 , and LBO-coated NCM811 electrodes are increased by 455.1, 274.5, 312.0, and 255.1 ppm after 72 h of storage, respectively. The water absorption of all the coated NCM811 cathodes during storage is less than that of the uncoated one. The lower water content in the cathode is beneficial to both the better discharge capacity and Coulomb efficiency of LIB (Li et al., 2016). The NCM811 cathode coated with LBO has the smallest moisture increment and has the best storage stability.
From Figure 8, it can be seen that after 100 cycles, the LIB capacity retentions of pure NCM811, NCM811 coated by    retentions. In Comparison of the data of capacity retention rate after 100 charge/discharge cycles in Figure 8 with the data in the literature listed in Table 1, it can be found that the cathode material in this work shows a higher capacity retention rate after the same number of cycles, thus demonstrating a better cycle performance. Compared with Al 2 O 3 -coated and ZrO 2 -coated NCM811 materials, NCM811 coated with LBO has a better cycling performance. The improved electrochemical performances of the coated samples are attributed to the protective function of the coating layer. The improved cycling performance of the coated cathode materials is attributed to the reduced electrolyte decomposition reactions and the alleviation of the impedance (see Figure 9) due to the existence of coating layers (Wang et al., 2013). The existence of coating layer is also conducive to preventing the excessive expansion of the active material particles, thus making the structure of the electrode stable and conducive to the stability of the charging and discharging processes (Zhou et al., 2019). Internal resistance of a battery is an importance parameter that can have a significant effect on its electrochemical performance such as cycling and power characteristics. Different cathode materials can give different internal resistances, leading to different electrochemical performances of the batteries (Shao et al., 2010). From Figure 9, it can be seen that the initial DC internal resistances of the coin LIBs composed of uncoated NCM811 (A) is 62.4 m , and the resistance increases to 92.3 m after 100 cycles. The initial DC internal resistance of the coin LIBs made of NCM811 coated with Al 2 O 3 (B) is 63.6 m , and the resistance value increases to 86.6 m after 100 cycles. The initial DC resistance of the coin LIB made of NCM811 coated with ZrO 2 (C) is 66.2 m , which increases to 89.1 m after 100 cycles. The initial DC resistance of the coin LIB made of NCM811 coated with LBO (D) is 64.9 m , which increases to 82.5 m after 100 cycles. Although the initial DC resistances of the coated NCM811 materials are slightly higher than that of uncoated one, the increasing trends of the resistances are slower than that of uncoated one. These slow increases can be beneficial to the stability of the electrochemical performance during the cycling. In comparison, NCM811 coated with LBO has the best resistance stability. Compared with Al 2 O 3 and ZrO 2 coating materials without electrochemical activity, LBO coating with NCM811 has obvious electrochemical performance advantages. LBO is a fast ionic conductor, which not only makes NCM811 higher capacity, but also the LBO coating is conducive to the migration and transfer of lithium ions between the electrode interfaces, reducing the irreversible loss of lithium ions in the process of charging and discharging, so that the lithium-ion battery has a better capacity retention and a smaller resistance increase in the process of cycling.

CONCLUSION
In this paper, the precursor Ni 0.8 Co 0.1 Mn 0.1 (OH) 2 is prepared by a co-precipitation method. Using this precursor, a cathode material of LiNi 0.8 Co 0.1 Mn 0.1 O 2 (NCM811) for lithium ion battery (LIB) is synthesized by mixing Ni 0.8 Co 0.1 Mn 0.1 (OH) 2 and LiOH and sintering twice. Al 2 O 3 , ZrO 2 , and LBO are used to coat on NCM811 to form the coated cathode materials by a wet chemical method. The effects of Al 2 O 3 , ZrO 2 , and LBO coatings on the morphologies, structures, compositions, and electrochemical properties of NCM811 are studied by both the physical characterization and electrochemical measurements. XRD results show that the coating layers do not change the original lattice structure of bulk NCM811. The materials of NCM811 without any coating and coated with Al 2 O 3 , ZrO 2 , and LBO all have a good hexagonal α-NaFeO 2 layered structure. The results of SEM, TEM, and XPS show that the prepared NCM811 with particle sizes of 3-16 µm can be successfully coated by Al 2 O 3 , ZrO 2 , and LBO with the coating-layers thicknesses of 20-200 nm.
To validate the effects of coating layers on the material properties, coin LIBs are assembled with the uncoated NCM811, Al 2 O 3 -coated, ZrO 2 -coated, and LBO-coated NCM811 materials as the cathodes. Experiment results show that although the first charge-discharge specific capacities of NCM811 coated with Al 2 O 3 and ZrO 2 are slightly smaller than those of uncoated NCM811, their Coulomb efficiencies of the first charge-discharge are increased after the coating. However, the first charge capacity (230.0 mAh/g), the first discharge capacity (204.3 mAh/g) and coulomb efficiency (88.83%) of NCM811 coated with LBO show the higher performance than those of uncoated one.
Regarding the water adsorption, the cathodes made of materials of pure NCM811, coated with Al 2 O 3 , ZrO 2 , and LBO, respectively, are stored at room temperature with 10% RH humidity for 72 h, and the changes of water contents of the cathodes during storage are measured, and the results show that the water contents of the uncoated NCM811, Al 2 O 3 , ZrO 2 , and LBO-coated NCM811 cathodes are increased by 455.1, 274.5, 312.0, and 255.1 ppm, respectively. The water absorption performances of the coated NCM811 cathodes during storage are better than that of the uncoated NCM811 one. The NCM811 cathode coated with LBO has the smallest moisture increment, suggesting that it has the best storage stability.
For studying cycling performances, the capacity retentions of the pure NCM811, coated with Al 2 O 3 , ZrO 2 , and LBO based LIBs are tested to be 99.50, 99.77, 99.84, and 99.91% of the initial capacities after 50 charge/discharge cycles, and the corresponding cathode resistances are increased by 19.6, 14.0, 13.6, and 12.2 m , respectively. These results demonstrate that the cycle performance and resistance stability of the NCM811 material can be significantly improved by the coating. The cycle performance and resistance stability of NCM811 coated with LBO are better than those of NCM811 coated with Al 2 O 3 and ZrO 2 .
Based on the experiment observation and data analysis, it can be concluded that the charge-discharge specific capacity, Coulomb efficiency, water absorption stability, cycle characteristics and resistance stability of the NCM811 cathode material can be significantly improved by coating it using LBO particularly. Considering that the amount of coating material is small, the coating process is relatively simple, and the improved electrochemical performance of NCM811, the cost would not be increases significantly. So in conclusion, the surface coating to the particles of cathode materials using LBO is an effective and practical modification method to improve the electrochemical performance of LIBs. In future study of the coating modification of NCM811, the performance stability at high temperature and the performance at long cycle should be further improved.

DATA AVAILABILITY STATEMENT
The datasets generated for this study are available on request to the corresponding author.

AUTHOR CONTRIBUTIONS
HZ designed experiments, carried out experiments, and analyzed experimental results. JX analyzed experimental results. JZ designed experiments, carried out experiments, and wrote the manuscript.