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ORIGINAL RESEARCH article

Front. Mater., 17 January 2022
Sec. Energy Materials

Improving the Sodium Storage Performance of Porous Carbon Derived From Covalent Organic Frameworks Through N, S Co-Doping

Xiaochen ZhangXiaochen Zhang1Zijian ZhangZijian Zhang1Xueqi ZhangXueqi Zhang1Haiquan SunHaiquan Sun2Quan HuQuan Hu2Haibao Wang
Haibao Wang2*
  • 1State Grid Beijing Chaoyang Electric Power Supply Company, Beijing, China
  • 2Beijing Smart-Chip Microelectronics Technology Co., Ltd., Beijing, China

Heteroatom doping, which has long been considered as one of the most efficient approaches to significantly enhance the sodium storage ability of carbonaceous anodes, has drawn increasing attention. Compared with single doping, dual doping can introduce more defects and accelerate ionic diffusion. In addition, the synergistic effect between the dual doped atoms can significantly improve the electrochemical performances. Besides, exploring novel precursors with excellent properties, which can induce porous structure and rapid pathways for electrons/ions in the resultant carbonaceous anode, is still full of challenges. Herein, nitrogen and sulfur–co-doped urchin-like porous carbon (NSC) was fabricated through a combined strategy including carbonization and subsequent sulfidation, using covalent organic frameworks (COFs) as precursors. Because of the dual doping–endowed rich defects, high electronic conductivity, and favorable capacitive behavior, the resultant NSC exhibited excellent sodium storage performances, delivering superior sodium storage capacity (483.5 mAh g−1 at 0.1 A g−1 after 100 cycles) and excellent cycling stability up to 1,000 cycles (231.6 mAh g−1 at 1.0 A g−1). Importantly, such remarkable electrochemical performances of the resultant carbonaceous anode may shed light on the efficient conversion of COFs to functional materials.

Introduction

Because of their excellent features including long life span, high energy density, and excellent stability, lithium-ion batteries (LIBs) have become the most successful commercial batteries, which have been widely applied in various portable electronics and electric vehicles. Unfortunately, the uneven distribution and limited lithium resources on Earth, combining the increasing price of raw materials, restrict its further development and application. In this context, the development of alternatives for LIBs that based on earth-abundant materials becomes urgent. Very recently, because of the natural abundance of sodium and the similar working mechanism between LIBs and sodium-ion batteries (SIBs), more and more attention has been put on the research of SIBs (Li et al., 2019a; Liu et al., 2019). Unfortunately, the sluggish reaction kinetics owing to the large Na+ radius (1.02 Å) leads to the degradation of SIBs upon cycling (Li et al., 2018a; Li et al., 2020a; Zheng et al., 2020; Li et al., 2022). In this context, exploring advanced electrode materials, featuring low-cost and high-performance, plays a significant role in the development of SIBs.

Compared with the extensive and in-depth studies on the cathode materials for SIBs, the research on anode materials is relatively insufficient (Xie et al., 2019; Xie et al., 2020; Fang et al., 2021). In general, alloy anodes with high theoretical specific capacities are often accompanied by the high volume change, resulting in the pulverization of active material on the electrode and further degradation on cycling (Li et al., 2021a; Li et al., 2021b). Besides, conversion anodes, mainly metal oxides/sulfides, suffer from high working voltage and poor electronic conductivity, restricting their electrochemical performances and improvement on the energy density of the full batteries (Li et al., 2018b; Li et al., 2020b; Zhang et al., 2020; Li et al., 2021c; Wan et al., 2021; Yang et al., 2021; Zhang et al., 2022a). Carbonaceous anodes with a typical insertion mechanism possess suitable working voltage, excellent interaction with the electrolyte, and high electronic conductivity, combined with structure fabrication, which renders them to be promising anodes for SIBs (Chen et al., 2019; Li et al., 2021d).

To further enhance the sodium storage performances of carbonaceous anodes, porous structure constructing and heteroatom doping represent efficient approaches to provide high transportation pathways for electrons/ions, optimize the electronic architecture, and modify the charge distribution in the carbonaceous skeleton (Li et al., 2019b). As for the morphology controlling, three-dimensional (3D) porous carbon, two-dimensional (2D) carbon sheets, one-dimensional (1D) carbon fibers, and zero-dimensional (0D) carbon have been reported to deliver efficient sodium storage (Zhang et al., 2017; Li et al., 2021a). Particularly, 3D porous carbon, endowing with large surface area, convenient transportation pathways, self-buffering volume, and high electronic conductivity, is considered as a promising anode candidate for high-performance SIBs (Zhang et al., 2017; Chen et al., 2019; Li et al., 2019c). For instance, an in situ template carbonization method was developed to fabricate a novel hierarchical 3D porous carbon, which shows favorable pseudocapacitive behavior as well as high sodium storage performance in both half and full cells (Wang et al., 2018a). Besides, Elizabeth et al. (2016) developed a porous carbon using prawn shells as the precursor, and the coexistence of macropores, mesopores, and micropores in the resultant carbonaceous anodes offers facile and transport channels for Na+, leading to the excellent performance of SIBs. As shown, the typical examples clearly demonstrate the structure advantages of the 3D porous carbons for high sodium storage performances, including hierarchically porous structure, rich pores, and high ionic/electronic conductivity.

Except for the construction of 3D porous structure, heteroatom doping, which can induce abundant defects and increase electronic conductivity of the target carbonaceous anodes, is also a feasible strategy to boost the electrochemical performance of carbonaceous anodes (Li et al., 2019b; Li et al., 2019d). Nitrogen (N), possessing a similar covalent radius with carbon, has become the star doping atom due to the fact that the introduction of N into the carbonaceous skeleton can further increase the electronic conductivity, causing the bias of electron cloud from the N atoms to the carbon atoms (Li et al., 2021e). Moreover, sulfur (S) doping, which is an efficient supplement for N doping, has also shown great promise for improving the electrochemical performances of carbonaceous anodes, resulting from the abundant defects after S doping (Li et al., 2018c; Zhang et al., 2021). Li et al. (2021a) developed a self-template method and prepared the N and S–co-doped layered carbon, where the high contents of doped heteroatoms and the improved ionic/electronic conductivity result in remarkable sodium storage. The above examples typically prove the feasibility of structure control and heteroatom doping for improving the electrochemical performances of the target electrode (Li et al., 2018d; Li et al., 2018e; Li et al., 2019e; Lu et al., 2021). In this regard, smart design and rational fabrication of a 3D porous skeleton with N and S co-doping, featuring rich defects, low charge-transfer polarization, and abundant active sites, are believed to obtain carbonaceous materials with high electrochemical performances (Zhang et al., 2017; Hong et al., 2019; Wang et al., 2020; Wang et al., 2021; Zhang et al., 2022b; Zhang et al., 2022c). However, exploring novel precursors with unique properties for the construction of 3D porous skeleton and subsequent heteroatom doping is challenging.

In this work, covalent-organic framework (COF), a new type of crystalline polymers composed of nonmetal elements (H, C, N, and O) through covalent bonding, is selected as the precursor due to their adjustable pore sizes and structures (Zhang et al., 2017). Through facile carbonization and subsequent sulfidation, N and S–co-doped urchin-like porous carbon (NSC) can be obtained. The COFs-induced urchin-like morphology and porous structure and stable inner structure, combining the heteroatoms doping induced favorable ionic/electronic conductivity and rich active sites, result in expressive sodium storage performance, showing great potential for the fabrication of high-performance SIBs.

Experimental

Synthesis of COFs

In a typical synthesis, 1,3,5-triformylphloroglucinol (63 mg), p-paraphenylenediamine (48 mg), 3 M aqueous acetic acid (0.5 ml), dioxane (1.5 ml), and mesitylene (1.5 ml) were mixed, which was then added into a Pyrex tube. After sonicating for 10 min, the sealed tube containing the uniform dispersion was heated at 120°C for 3 days. After the tube cooled down to room temperature, the red product was collected through centrifugation and washing with anhydrous acetone several times. Afterward, the product was dried under vacuum overnight to receive the desired COFs.

Synthesis of NC and NSC

To synthesize the NC, the received COFs were directly carbonized at 600°C for 4 h under N2 protection with a heating rate of 5°C min−1. Generally, the carbonized step was used to stabilize the carbonaceous skeleton, facilitating the following sulfidation treatment. Typically, NC and S powder with a mass ratio of 1:10 was mixed and then heated at 500°C, 600°C, and 700°C for 2 h under flowing N2 to obtain the NSC-500, NSC-600, and NSC-700, respectively.

Besides, the structure characterizations of the as-prepared samples and electrochemical methods used in this work can be found in Supporting Information (SI).

Results and Discussion

As illustrated in Figure 1A, 1,3,5-triformylphloroglucinol and p-paraphenylenediamine were reacted in a Pyrex tube for 3 days at 120°C, leading to the formation of the desired COFs through Schiff-based reaction (Kandambeth et al., 2012). Besides, the further conversion from the COFs to porous carbon doped with N and S was realized through subsequent carbonization and sulfidation (Li et al., 2018c). In addition, the morphologies of the pure COFs, NSC-500, NSC-600, and NSC-700 were observed through field-emission scanning electron microscopy (FESEM, Figures 1B–F), from where we can detect that the morphologies of NSC-500, NSC-600, and NSC-700 maintain well compared with their precursors after the carbonization and subsequent sulfidation process. Specifically, the pure COFs possess urchin-like morphology with porous structure (Figures 1B,C), which is unique among COFs reported (Zhang et al., 2017; Zhang et al., 2018). As for the elemental mapping, the coexisted C, N, and S were found to be uniformly dispersed in the NSC-600, thus demonstrating the successful conversion and co-doping (Figure 1G) (Zhang et al., 2021; Sun et al., 2021). Further detailed observations on the structure of NSC-600 in TEM and HRTEM (Figures 1H–J) further confirm its urchin-like structure and homogeneous dispersion. Generally, the urchin-like sphere morphology, combined with the abundant N and S co-doping, can not only provide fast transportation pathways for the electrons/ions but also offer rich sites toward sodium storage, boosting the electrochemical performances (Augustyn et al., 2014; Dahbi et al., 2016; Wang et al., 2018b).

FIGURE 1
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FIGURE 1. Illustration of the conversion from as-prepared COFs to desired NSC (A). FESEM images of pure COFs (B,C), NSC-500 (D), NSC-600 (E), and NSC-700 (F). Elemental mapping of NSC-600 (G). TEM (H,I) and HRTEM (J) images of NSC-600.

To detect the crystal structure of the as-prepared carbonaceous materials, X-ray diffraction (XRD) measurements were conducted (Figure 2A). As seen, two broad peaks corresponding to (002) and (110) planes of the graphitic frameworks can be found at around 25.0 and 43.5°, respectively (Chen et al., 2019). Besides, the (100) peak gradually increases with the increase of sulfidation temperature, meaning the increased graphitic structure in the carbonaceous skeleton (Zhang et al., 2017). Furthermore, the coexistence of disordered carbon and the graphitic domain was further confirmed by the Raman spectra (Figure 2B), where two typical peaks ascribing to D and G bands can be clearly found at around 1,370 and 1,580 cm−1 (Wang et al., 2019). As known, the D band represents the characteristic feature of disordered structure in the carbonaceous skeleton, whereas the G band corresponds to the graphitic domain (Zhang et al., 2017). Moreover, the graphitization degree of the carbonaceous matrix can be estimated through the ID/IG value. After calculation, the ID/IG values for NC, NSC-500, NSC-600, and NSC-700 are 0.86, 0.92, 0.94, and 0.98, showing a slight decrease in the graphitization degree with the increasing of sulfidation temperature, which should be ascribed to the N and S co-doping–induced abundant defects in the carbonaceous skeleton (Li et al., 2019c; Wang et al., 2018a). In addition, the surface chemical components of fabricated samples were further observed through X-ray photoelectron spectroscopy (XPS). Generally, signals from C 1s, N 1s, and S 2p can be clearly observed for all the three NSC samples, whereas only C 1s and N 1s were presented for NC (Figure 2C). Besides, the bonding states of the C, O, and S of NSC-600 were further revealed through their high-resolution spectra (Figures 2D–F). Figure 2D illustrates the C 1s spectra of NSC-600 and the detected four peaks, with binding energies at 283.4, 284.3, 286.2, and 286.6 eV, should be assigned to the C-N, C-S, and O-C=O, respectively (Li et al., 2021a). Figure 2E illustrates the N 1s spectra of NSC-600, where graphitic N, pyridinic N, and pyrrolic N, respectively, are found at around 402.5, 399.5, and 397.2 eV, revealing the N atoms still remained in the carbonaceous matrix after carbonization and sulfidation (Li et al., 2019b). As for the S 2p spectrum (Figure 2F), three peaks at around 162.7, 164.0, and 166.9 eV correspond to thiocarbonyl-sulfhydryl, -C-S-C-, and thiophenes, respectively, demonstrating the S doping (Li et al., 2021a). For comparison, the high-resolution elemental spectra of NSC-500 and NSC-700 are shown in Supplementary Figure S1 (SI), which displays similar deconvolved features with those of NSC-600, resulting from their analogous composition and structure.

FIGURE 2
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FIGURE 2. XRD patterns (A,B) Raman spectra and XPS spectra (C) of NC, NSC-500, NSC-600, and NSC-700. High-resolution C 1s (D), N 1s (E), and S 2p (F) spectra of NSC-600.

The sodium storage ability of fabricated carbonaceous anodes was compared through various electrochemical tests, including galvanostatic discharging/charging, electrochemical impedance spectroscopy (EIS), and cyclic voltammetry (CV). First, the initial three curves of the NSC-600 electrode at the scan rate of 0.2 mV s−1 from 0.005 to 3.0 V are depicted in Figure 3A. The irreversible cathodic peak at around 0.88 V presented in the first cathodic scan, which is disappeared in the subsequent scans, should be ascribed to the decomposition of electrolyte to passivate the surface as well as the generation of solid electrolyte interface (SEI) (Eshetu et al., 2019; Cheng et al., 2021; Fan et al., 2021). In addition, another broad cathodic peak in the low voltage from 0.71 V to 0.005 V should be ascribed to the intercalation of Na+ into the carbonaceous skeleton (Kumar et al., 2016). In the following anodic scans, only one anodic peak can be found, ascribing to the deintercalation of Na+ (Zhang et al., 2018). After the first scan, only one pair of cathodic/anodic peaks at low voltage can be detected, manifesting reversible sodium storage, and the well-maintained CV shape reveals its good reversibility (Li and Zhang, 2018; Li et al., 2019f). Accordingly, the discharge/charge profiles of NSC-600 shown in Figure 3B further confirm its excellent electrochemical reversibility from the almost overlapped profiles. Notably, the difference on discharge profiles between the first cycle and subsequent cycles can be ascribed to the formation of SEI film due to electrolyte decomposition, structure variations and activation of electrode materials. Particularly, the first discharge/charge reversible capacities for the NSC-600 electrode are 987.5 and 497.4 mAh g−1, thus acquiring an initial Coulombic efficiency of 50.4%. In general, the decomposition of electrolyte with the generation of SEI, the trapped Na+ in electrode, and its large surface area induced some irreversible reactions contributes to the low Coulombic efficiencies (Li et al., 2020a; Zou et al., 2020). Comparatively, Supplementary Figures S2–S4 (SI) shows the discharge/charge profiles of NC, NSC-500, and NSC-700 at 0.1 A g−1, and the corresponding Coulombic efficiencies are calculated to be 51.0%, 42.8%, and 39.4% for NC, NSC-500, and NSC-700, respectively.

FIGURE 3
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FIGURE 3. (A) CV curves at 0.2 mV s−1 and (B) discharge/charge profiles of different cycles at 0.1 A g−1 for NSC-600 electrode. Electrochemical impedance spectra after five cycles (C), cycling performances [0.1 A g−1, (D)], Coulombic efficiencies (E), rate performance (F), and long-term cycling performance [1.0 A g−1, (G)] of NC, NSC-500, NSC-600, and NSC-700.

To detect the kinetics difference of the four samples, EIS measurements on the cycled cells were carried out, and Figure 3C displays the corresponding Nyquist plots. Generally, the resistance of SEI film can be detected from the small semicircle in the high-frequency region, the charge transfer resistance (Rct) is related to the large semicircle in the medium-frequency region, and the ionic diffusion in the bulk electrode can be estimated from the straight line in the low-frequency region (Augustyn et al., 2014; Li et al., 2019b). Interestingly, the Rct values dramatically decrease after the S doping, meaning the increased charge transfer in the NSC. Specifically, the Rct values are 1,216, 536, and 756 Ω for NSC-500, NSC-600, and NSC-700, respectively. The variations on the Rct values should be ascribed to their different doping contents of N and S, which have been illustrated in Supplementary Table S1 (SI). Particularly, the N and S contents in NSC-500 are 15.68 and 10.24 at%, respectively. After increasing the sulfidation temperature to 600°C, the contents of N and S increase to 17.85 and 12.90 at%. Further increasing the sulfidation temperature to 700°C results in the decrease of doping contents of N and S to 7.86 and 11.92 at%, respectively. In this context, the rich defects and decreased energy barrier for the charge transfer resulted from the high heteroatom doping contents in the carbonaceous skeleton leading to the low Rct (Li et al., 2021e; Sun et al., 2021).

Comparison of the sodium storage ability among NC, NSC-500, NSC-600, and NSC-700 at 0.1 A g−1 is shown in Figure 3D. Specifically, the NSC-600 delivers the highest reversible capacity after 100 cycles (414.4 mAh g−1), along with excellent cycling stability. The other three samples also demonstrate stable cycling, but the specific capacities are low, with reversible capacities of 194.5, 245.7, and 277.1 mAh g−1 after 100 cycles, respectively, for NC, NSC-500, and NSC-700. Besides, the high electrochemical reversibility of the electrodes was also manifested through their Coulombic efficiencies (Figure 3E). Figure 3F displays the rate capabilities of the as-prepared four samples, and the NSC-600 shows superior rate capability than the other three samples, delivering reversible capacities of 381.6, 323.9, 273.7, 250.6, 225.6, and 204.4 mAh g−1 at 0.1, 0.5, 1.0, 2.0, 4.0, and 6.0 A g−1, respectively. Furthermore, a reversible capacity of 381.7 mAh g−1 can still be received after the current density returns to 0.1 A g−1, showing remarkable rate capability. Moreover, further increasing the current density to 1.0 A g−1, the cycling of NSC-600 electrode can still be maintained well, displaying a reversible capacity of 223.4 mAh g−1 after 1,000 cycles, which is the highest among the three NSC samples (182.9 mAh g−1 for NSC-500 and 161.2 mAh g−1 for NSC-700) (Figure 3G). The corresponding discharge/charge profiles of NSC-500, NSC-600, and NSC-700 are shown in Supplementary Figure S5 (SI), and all the profiles show typical features of carbonaceous anodes. As shown above, the NSC exhibits superior sodium storage performance, including superior cycling stability, high specific capacity, and good rate capability. Theoretically, the urchin-like porous structure and high N, S doping contribute to the optimization of electronic/ionic conductivity, resulting in the improvement of sodium storage performance (Zhang et al., 2018; Hong et al., 2019).

To explore the dynamics mechanism upon redox reactions and the origin of the improvement on the sodium storage activity of NSC-600, CV measurements at various scan rates (0.2–1.4 mV s−1) were performed to detect the charge storage kinetics (Figure 4A). From the CV curves obtained at various scan rates, the cathodic peak slightly shifts to the low voltage and the anodic peak shifts to the high voltage, indicating a weak polarization of electrode (Augustyn et al., 2014). According to the following equations, the charge storage in the electrode dominated by capacitance or diffusion can be determined (Li et al., 2021e).

i=avb(1)
log(i)=blog(v)+log(a)(2)

FIGURE 4
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FIGURE 4. CV curves (A) of NSC-600 electrode at the scan rate of 0.2–1.4 mV s−1. The plots of Log(i) versus Log(v) to obtain the b values of the marked peaks in the CV curves (B). The variations of b values upon discharging and charging (C). Contributions at various scan rates from capacitance and diffusion (D).

where i and v represent the response current and scan rate, respectively (Li et al., 2018c; Li et al., 2017). Particularly, the value of b is the typical index for the electrode kinetics upon discharging/charging (Li et al., 2021b; Li et al., 2018b). The value of b approaching 0.5 demonstrates a diffusion-dominated process, whereas the value of 1.0 manifests the redox process is controlled by capacitive behavior (Li et al., 2021a). Through plotting log(i) versus log(v) and further fitting, the b values are 0.89 and 0.92 (Figure 4B) for the cathodic and anodic peak marked in the CV curves, showing its favorable capacitive feature upon sodium storage, which results from its structure advantages including urchin-like morphology, porous structure, rich defects, and high doping contents (Li et al., 2021e). Further observation on the variations of b values upon discharging and charging is illustrated in Figure 4C. For both the discharging and charging, the variations of b demonstrate that the electrochemical process near the cathodic/anodic peak areas is dominated by capacitance, and the charge storage in areas away from the cathodic/anodic peak is controlled by capacitance (Li et al., 2021f). It is easy to understand that the variations of b values at different voltage range result from their different sodium storage mechanisms as the intercalation of Na+ in the low voltages is promoted by diffusion, and capacitive controlled adsorption of Na+ happens in high voltages (Li et al., 2021a; Li et al., 2021f). In addition, the charge storage contributions can be further separated into diffusion and capacitive parts through the following equations.

iv=k1v+k2v1/2(3)
i(v)v1/2=k1v1/2+k2(4)

where k2v1/2 and k1v correspond to the diffusion and capacitive contributions for the charge storage, respectively (Li et al., 2021d). After detailed fitting and calculation, the contributions from capacitance and diffusion for the NSC-600 electrode are 78.1%, 81.9%, 84.9%, 87.1%, 89.8%, 91.6%, and 93.7%, respectively, at scan rates of 0.2, 0.4, 0.6, 0.8, 1.0, 1.2, and 1.4 mV s−1 (Figure 4D), manifesting favorable capacitive dominated electrochemical process, which contributes to its stable sodium storage performance (Augustyn et al., 2014).

Conclusion

In summary, carbonaceous skeleton co-doped with N and S was synthesized through a simple combined strategy of carbonization and subsequent sulfidation, employing novel COFs as precursors. The unique urchin-like morphology and porous structure induced efficient interaction between electrolyte and electrode; the heteroatom doping–endowed rich defects and improved electronic/ionic conductivity result in excellent sodium storage performance of the designed carbonaceous skeleton, with high reversible capacity (483.5 mAh g−1 at 0.1 A g−1 up to 100 cycles) and excellent rate capability (231.6 mAh g−1 at 1.0 A g−1 up to 1,000 cycles). This work manifests the feasibility of structure controlling and heteroatom doping to enhance the sodium storage ability of carbonaceous anodes, which shed light on the conversion of COFs to various functional materials for efficient energy storage and conversion.

Data Availability Statement

The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.

Author Contributions

XiZ: Conceptualization, Methodology, Writing original draft. ZZ: Methodology, Data curation, Investigation. XuZ: Data curation. HS: Visualization, Investigation. QH: Formal analysis. HW: Supervision, Writing–review and editing.

Conflict of Interest

HS, QH, and HW were employed by Beijing Smart-Chip Microelectronics Technology Co., Ltd. XiZ, ZZ and XuZ were employed by State Grid Beijing Chaoyang Electric Power Supply Company.

Publisher’s Note

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.

Supplementary Material

The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/fmats.2021.820671/full#supplementary-material

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Keywords: nitrogen, sulfur co-doping, covalent organic frameworks, carbonaceous anodes, sodium storage, high performance

Citation: Zhang X, Zhang Z, Zhang X, Sun H, Hu Q and Wang H (2022) Improving the Sodium Storage Performance of Porous Carbon Derived From Covalent Organic Frameworks Through N, S Co-Doping. Front. Mater. 8:820671. doi: 10.3389/fmats.2021.820671

Received: 23 November 2021; Accepted: 06 December 2021;
Published: 17 January 2022.

Edited by:

Likun Pan, East China Normal University, China

Reviewed by:

Jinliang Li, Jinan University, China
Xiaojie Zhang, Huaiyin Institute of Technology, China

Copyright © 2022 Zhang, Zhang, Zhang, Sun, Hu and Wang. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Haibao Wang, whb11_22@163.com

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