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Preinserted Ammonium in MnO2 to Enhance Charge Storage in Dimethyl Sulfoxide Based Zinc-Ion Batteries
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Preinserted Ammonium in MnO2 to Enhance Charge Storage in Dimethyl Sulfoxide Based Zinc-Ion Batteries
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  • Wathanyu Kao-ian
    Wathanyu Kao-ian
    Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, Thailand
  • Jinnawat Sangsawang
    Jinnawat Sangsawang
    Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, Thailand
  • Mohan Gopalakrishnan
    Mohan Gopalakrishnan
    Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, Thailand
  • Suttipong Wannapaiboon
    Suttipong Wannapaiboon
    Synchrotron Light Research Institute, 111 University Avenue, Muang District, Nakhon Ratchasima 30000, Thailand
  • Athis Watwiangkham
    Athis Watwiangkham
    Department of Chemistry, Faculty of Science, Ubon Ratchathani University, Ubon Ratchathani 34190, Thailand
  • Siriporn Jungsuttiwong
    Siriporn Jungsuttiwong
    Department of Chemistry, Faculty of Science, Ubon Ratchathani University, Ubon Ratchathani 34190, Thailand
  • Jayaraman Theerthagiri
    Jayaraman Theerthagiri
    Core-Facility Center for Photochemistry & Nanomaterials, Department of Chemistry (BK21 FOUR), Research Institute of Natural Sciences, Gyeongsang National University, Jinju 52828, Republic of Korea
  • Myong Yong Choi*
    Myong Yong Choi
    Core-Facility Center for Photochemistry & Nanomaterials, Department of Chemistry (BK21 FOUR), Research Institute of Natural Sciences, Gyeongsang National University, Jinju 52828, Republic of Korea
    *Email: [email protected]
  • Soorathep Kheawhom*
    Soorathep Kheawhom
    Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, Thailand
    Center of Excellence on Advanced Materials for Energy Storage, Chulalongkorn University, Bangkok 10330, Thailand
    *Email: [email protected]
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ACS Applied Materials & Interfaces

Cite this: ACS Appl. Mater. Interfaces 2024, 16, 42, 56926–56934
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https://doi.org/10.1021/acsami.4c07239
Published August 30, 2024

Copyright © 2024 The Authors. Published by American Chemical Society. This publication is licensed under

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Abstract

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Nonaqueous zinc-ion batteries (NZIBs) featuring manganese dioxide (MnO2) cathodes position themselves as viable options for large-scale energy storage systems. Herein, we demonstrate the use of ammonium cation as a preintercalant to improve the performance of the δ-MnO2 cathode in wet dimethyl sulfoxide based electrolytes. Employing in situ X-ray absorption spectroscopy, Raman spectroscopy, and synchrotron X-ray diffraction, we reveal that the integration of ammonium cations promotes the formation of NH–O–Mn networks. These networks are crucial for manipulating the distortion of the MnO6 octahedral units during discharging, thereby mitigating charge disproportionation, which is a primary limitation to MnO2’s charge-storage efficiency. The modified MnO2, through this idea, displays a notable improvement in capacity (∼247 mAh/g) and can pass charge–discharge cycles up to 500 cycles with a capacity retention of 85%. These findings underscore the potential of modified MnO2 in advancing MnO2-based hosts for Zn-MnO2 batteries, marking significant progress toward next-generation energy storage solutions.

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Copyright © 2024 The Authors. Published by American Chemical Society

1. Introduction

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Due to their cost-effectiveness and environmental friendliness, the quest for sustainable energy solutions has brought zinc (Zn)-manganese dioxide (MnO2) rechargeable batteries into the spotlight. (1−3) Zn-MnO2 batteries are celebrated for their promising potential owing to their abundant availability and low cost compared to lithium-ion systems. (4,5) Despite their potential, these batteries face challenges such as hydrogen evolution and dendritic growth, limiting their practical application. (6−8) To address these issues, researchers have turned to nonaqueous electrolytes, including organic solvents, deep eutectic solvents, and ionic liquids. (9) These alternatives, notable for their nonprotonated nature, effectively prevent Zn dendrite formation by promoting the natural formation of a functional Zn–electrolyte interface, thereby enhancing the anode’s cycle life and performance. (10,11) However, utilization of these electrolytes in MnO2-based ZIBs encounters significant hurdles due to the high overpotential required for Zn-ion (Zn2+) intercalation at the MnO2 cathode. This matter leads to reduced voltage and specific capacity, limiting the batteries’ effectiveness for practical applications. (1)
Understanding of the charge-storage mechanism of MnO2 in nonaqueous media remains limited. Han et al. highlighted this by showcasing the reversible intercalation of Zn2+ into layered MnO2 (δ-MnO2) within an acetonitrile-based electrolyte, achieving a specific capacity of 123 mAh/g. However, this outcome falls short of MnO2’s theoretical capacity of 308 mAh/g, which is expected when the oxidation state of manganese is reduced by 1. (12) This discrepancy is attributed to the high charge density of the divalent Zn2+, which fosters a strong solvation effect with the solvent molecules, leading to substantial energy losses during desolvation processes. (13,14) Additionally, this high charge density intensifies the electrostatic interaction between Zn2+ ions and the oxygen atoms in MnO2, consequently impeding the solid-phase diffusion of Zn2+ and further compromising the material’s charge-storage efficiency. (15)
Innovative strategies to augment the charge-storage capacity of MnO2 have identified the addition of water as a remarkably effective method. (13,15−17) This method leverages the formation of a hydration shell around Zn2+ ions, which effectively reduces the “effective charge” of Zn2+. By diminishing the electrostatic interactions between Zn2+ ions and cathode materials, such an approach greatly facilitates the intercalation of Zn2+ ions into a variety of cathode materials, including vanadium oxides (V2O5, V6O13), vanadium phosphates (VOPO4, VPO4F), and Prussian blue analogues (KCuHCf). (13,17−20) Our research group has previously demonstrated the beneficial impact of water in a wet dimethyl sulfoxide (DMSO) electrolyte on the charge-storage capabilities of MnO2. (15) Our findings revealed a substantial increase in cathode capacity, from approximately 90 mAh/g to around 200 mAh/g at a current density of 50 mA/g, alongside improved stability with just 5 wt % water content. Despite these advancements in performance through hydration, it is suggested that optimizing the structural configuration of MnO2 could lead to further improvements in capacity.
Enhancing the performance of MnO2 as a cathode material for ZIBs can be achieved by various approaches. One method involves doping MnO2 with transition metals such as iron (Fe), cobalt (Co), and nickel (Ni). This strategy disrupts the periodic potential field inherent in MnO2, thereby improving Zn2+ ion mobility. (21) Another approach is to anchor MnO2 onto carbon supports, which not only enhances the electronic conductivity through a more robust electronic network but also helps in mitigating the dissolution of manganese. (22) When considering nonaqueous media, however, challenges extend beyond the solid-phase diffusion of Zn2+ and the poor electronic conductivity of MnO2. Such challenges encompass the desolvation process that solvated Zn2+ ions undergo prior to intercalation. Transition metal doping and the introduction of carbon supports, while beneficial, do not comprehensively address these multifaceted issues. Our investigation reveals that during the Zn2+ intercalation (discharging) process, there is a conspicuous substitution of solvated organic molecules with water molecules at the MnO2 interface. (15) This observation suggests the necessity for a functional junction capable of facilitating this exchange to enhance performance. In this context, the ammonium (NH4+) cation emerges as a promising solution. With its strong hydrogen-bonding capability and affinity for water, NH4+ can potentially alleviate the aforementioned hurdles. Despite some studies demonstrating the use of preinserted NH4+ species to enhance ZIB performance, the specific role and the effect of NH4+ in nonaqueous or wet nonaqueous ZIBs remains underexplored. (23−25)
In this study, we introduce a pioneering approach by incorporating NH4+ preintercalated manganese dioxide (NH4-MnO2) as the cathode material in wet nonaqueous ZIBs. Our goal of this work is to address the challenges of high overpotential and improve charge-storage efficiency. We utilize a DMSO-based electrolyte with an optimized concentration of Zn triflate (0.3 M) in a 5 wt % water–DMSO solution, adhering to rules established in our previous research. (15) This study aims to shed light on how NH4+ preintercalation influences the charge-storage dynamics of the MnO2 cathode. Our method is distinguished from others by employing an Mn-ion-free electrolyte, thus ensuring that the cathode’s specific capacity is unaffected by external Mn sources. To verify the successful synthesis and structural integrity of our materials, we conduct comprehensive characterizations using field emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM), energy-dispersive X-ray spectroscopy (EDS), X-ray photoelectron spectroscopy (XPS), X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), Raman spectroscopy, and electron paramagnetic resonance (EPR). We also employ advanced X-ray techniques, including in situ X-ray absorption spectroscopy (XAS) and synchrotron XRD, to examine the valency and structural evolution of Mn and Zn within the cathode under real-cell conditions. The innovative investigation is expected to significantly contribute to the development of MnO2-based cathodes, offering valuable insights for designing practical cathode materials for ZIB applications in the future.

2. Experimental Setup and Testing

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2.1. Materials

Zn foil (99.99%, thickness: 0.05 mm) was purchased from Shandong AME Energy Co. Ltd., China. Graphite foil (grafoil, thickness: 25 μm) was purchased from Shenzhen 3KS Electronic Material Co. Ltd., China. Polyimide tape was purchased from DuPont de Nemours, Inc. Ketjenblack EC-600JD electroconductive carbon black was purchased from Ketjen International. Solef 5130 (PVDF for Li-ion batteries) was purchased from Solvay. Ammonium persulfate ((NH4)2S2O8, 98%), anhydrous DMSO (99.9%), sodium carboxymethylcellulose (NaCMC, medium viscosity), and Zn triflate (Zn(CF3SO3)2, 98%) were procured from Sigma-Aldrich. Ammonia solution (NH3, 28%) was acquired from QReC. Potassium permanganate (KMnO4, 99.0%) was obtained from Ajax Finechem. Glass microfiber (WHA1820125, GF/A, pore size: 1.6 μm) was purchased from Whatman Plc.

2.2. K-MnO2 and NH4-MnO2 Syntheses

Potassium-MnO2 (K-MnO2, δ-phase) was synthesized via a hydrothermal method. (15,26,27) First, 70 mL of deionized (DI) water was used to dissolve 1.896 g of KMnO4; the mixture was agitated at a medium rotating speed. After 30 min, 0.338 g of MnSO4·H2O was gradually added to the solution. Subsequently, the mixture was placed in an autoclave lined with PTFE and heated to 160 °C for 24 h. The autoclave was then allowed to cool naturally in the open air. Finally, the mixture was filtered, repeatedly cleaned with ethanol and DI water, and then vacuum-dried overnight at 60 °C.
For the NH4-MnO2 preparation, K-MnO2 was used as a precursor. Wang et al. used the method adapted from the TMA-MnO2 preparation. (28) First, 0.4 g of K-MnO2 was mixed with 100 mL of 0.5 M (NH4)2S2O8 under vigorous stirring at 60 °C for 12 h. Then, the filtered solid was dried at 60 °C in an oven. Subsequently, 0.4 g of the obtained powder (proton-intercalated MnO2) was neutralized using 100 mL of 10 wt % NH3 solution (NH4OH). The mixture was stirred at a medium rotating speed for 3 days. The product, NH4-MnO2, was obtained after being filtrated and dried at 60 °C overnight.

2.3. Cathode and Electrolyte Preparation

Both MnO2 (70 wt %), Ketjenblack (20 wt %), and NaCMC (10 wt %) were slurry mixed with deionized (DI) water to form an ink for the cathode coating. To ensure homogeneity, the mixture was shaken and agitated several times using an ultrasonic cleaner and magnetic stirrer. Subsequently, the ink was applied on the graphite foil using a doctor blade (AOT-FCM-250, AOT Electronic Technology) and left until dry for 2 h. Then, the coated cathode was rolled using a laboratory roller press machine (TOB-DG-100L). Finally, the cathode was vacuum-dried at 60 °C overnight. The average δ-MnO2 loading on the electrode was ∼2 mg/cm2. The electrolyte was prepared by simply mixing 5 wt % water in DMSO. Finally, Zn triflate was mixed with 5 wt % water in DMSO in a volumetric flask to form a 0.3 M Zn triflate solution.

2.4. Electrochemical Measurements and Material Characterizations

A button cell (CR2025) was used as the main configuration for the electrochemical measurement. Using a punching machine (TOB-CP60), the Zn foil (anode) and MnO2 (cathode) were cut into 15 mm diameter disks. A glass microfiber (19 mm in diameter) was used as a separator. The cell was assembled, and 250 μL of electrolyte was added to the cell. Finally, a coin cell crimping machine (TOB-MR120) was used to seal the cell. To determine the rate capability, cyclability, and discharging overpotential of the battery, both galvanostatic charge–discharge (GCD) and galvanostatic intermittent titration technique (GITT) were carried out using a battery analyzer (NEWARE, BTS4000-5 V10 mA). To investigate the redox behavior of the battery, cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS) were performed using a potentiostat (Squidstat, Admiral Instruments LLC). All of the electrochemical measurements were performed in a cell isolating the thermal safety chamber (Arbin instruments) at a regulated temperature of 30 °C.
Further, to speciate and analyze their properties, synthesized powders, namely, K-MnO2 and NH4-MnO2, were analyzed using TEM-EDS (JEOL Model JEM-2100), XPS (PHI VersaProbe 4), ex situ XRD (Cu Kα radiation, 40 kV, 15 mA, and λ = 1.5418 Å, Aeris Benchtop, Malvern Panalytical, U.K.), FT-IR (Thermo Fisher Nicolet iS5 FT-IR spectrometer), Raman (Thermo Scientific DXR Raman Microscopy), and EPR (BRUKER EMXmicro). To capture the morphology and the composition of the δ-cathode, FE-SEM (QuantaTM 250 FEG (FEI)) with EDX (PentaFET, Oxford Instruments) was employed. To determine the charge-storage mechanism and discern the difference between K-MnO2 and NH4-MnO2 cathodes, synchrotron XRD and in situ XAS results were collected at beamline 1.1, Synchrotron Light Research Institute (SLRI), Thailand. Synchrotron XRD was performed at 12 keV and calibrated λ of 1.033198 Å using the grazing incidence mode, which is well-suited for analyzing a thin film. In situ XAS was measured using a homemade cell (Figure S1), which was designed for the transmission XAS mode. To obtain high-quality XAS data, the amount of cathode material loading was carefully determined (2.0 mg/cm2). XAS results, namely, X-ray absorption near edge structure (XANES) and extended X-ray absorption fine structure (EXAFS), were interpreted using Demeter: XAS data processing and analysis version 0.9.26. (29)

3. Results and Discussion

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In Figure 1, the characterization results of the synthesized K-MnO2 and NH4-MnO2 powders are shown. As observed via TEM, both K-MnO2 (Figure 1A) and NH4-MnO2 (Figure 1D) reveal a flower-like nanostructure, similar to other forms of δ-MnO2 as seen in the literature. (30,31) EDS mapping of K-MnO2, in accordance with the TEM image, indicates an even distribution of Mn (Figure 1B) and K (Figure 1C) along the MnO2 grain; the latter refers to the intercalated K in the interlayer of MnO2. In Figure 1E, the distribution of Mn in NH4-MnO2 is displayed. It is noted that EDS of the NH4-MnO2 sample displays a weaker signal of K (Figure 1F) than that of N (Figure 1G), indicating the substitution of N-containing species at the K site. In addition, N species were also detected via the XPS technique (Figure S2). The deconvoluted peaks of the narrow scan during N 1s energy indicate the existence of N–H (399.85 eV) and N–H+ (401.63 eV). (32,33) In Figure 1H,I, the zoom-in TEM images display a clear interplanar spacing of MnO2, which is attributed to the 001 plane. Both the K-MnO2 and NH4-MnO2 samples show a similar interspacing distance of ∼0.69 nm. In Figure 1J, the XRD spectrum of K-MnO2 is well-matched with birnessite (ref code 96-901-0157, H4K0.23MnO2.776), signifying main characteristic peaks at 2θ of 12.35° (001), 24.9° (002), and 36.5° (11–1). The NH4-MnO2 sample exhibits peaks of 001 and 002 planes at a slightly lower angle compared to that of K-MnO2, indicating that after modification, the interspacing length between the MnO2 layers increased. According to the refined XRD spectra using the Rietveld refinement technique (Figure S3 and Table S1), the d-spacings of the 001 plane of K-MnO2 and NH4-MnO2 are 7.17 and 7.24 Å, respectively. An increase in interspacing is attributed to the presence of the interlayered NH4+ (ion radii: 1.40–1.67 Å), which is larger than the potassium (K) ion (ion radii: 1.38 Å). (34,35) In addition, the 11–1 peak (inset in Figure 1J, right) slightly shifted from its own position. Such a shift indicates that the geometrical distortion of MnO6 occurred when NH4+ was present.

Figure 1

Figure 1. Powder characterization results: (A) TEM image of K-MnO2, (B) Mn EDS mapping of K-MnO2, (C) K EDS mapping of K-MnO2, (D) TEM image of NH4-MnO2, (E) Mn EDS mapping of NH4-MnO2, (F) K EDS mapping of NH4-MnO2, (G) N EDS mapping of NH4-MnO2, (H) zoom-in TEM image of K-MnO2, (I) zoom-in TEM image of NH4-MnO2, (J) XRD results of K-MnO2 and NH4-MnO2, (K) FT-IR results, (L) structure of the synthesized NH4-MnO2, (M) deconvoluted Raman spectra of K-MnO2, and (N) deconvoluted Raman spectra of NH4-MnO2.

In Figure 1K, FT-IR results are shown. Thus, it is seen that there are about three regions of FT-IR spectra, i.e., wavenumber >700, 1350–1670, and 2950–3550 cm–1, which are ascribed to the stretching vibration of Mn–O, the stretching vibration of O–H, and the stretching vibration of N–H/O–H, respectively. (36) During 2950–3550 cm–1, additional peaks appeared in NH4-MnO2. In contrast, the K-MnO2 sample did not show such characteristics. These peaks are attributed to the presence of the N–H stretching vibration of NH4+ cations and their interaction with oxygen atoms from MnO2 or water molecules. At 1410 cm–1, the peak intensified, indicating the presence of the bending vibration of N–H along with the stretching vibrational mode of the water molecule in the MnO2 interlayer. (37) At this point, the existence of the NH4+ cation in the MnO2 interlayer is confirmed. In Figure 1L, the structure of the synthesized NH4-MnO2 is illustrated.
In Figure 1M,N, the deconvolution of the Raman results of K-MnO2 and NH4-MnO2 is illustrated. Herein, ν1, ν2, and ν3 are attributed to the Mn–O lattice vibration of the basal plane of the MnO2 sheets and the Mn–O lattice vibration and the symmetric stretching vibration of the Mn–O band in the MnO6 octahedra, respectively. (37−39) It is seen that after transforming K-MnO2 into NH4-MnO2, the contribution of ν1 to the Raman curve reduced, indicating that the binding force between the upper and lower layer of the MnO2 increased. This increase is due to the strong hydrogen bond formed between the oxygen atoms of MnO2 and the hydrogen atoms of the NH4+ cations in the interlayer of MnO2. Moreover, peak ν3 shifted to a higher wavenumber, denoting that the stability of Mn–O bonds within the MnO6 octahedra increased. It is noted that NH4+ cations act like a pillar and form NH–O–Mn, exhibiting a strong binding force between layers of MnO2 and slight distortion of MnO6 from its own shape having Mn(IV). In Figure S4, the EPR signal of NH4-MnO2 is seen to be weaker than that of K-MnO2. Thus, the modification did not increase the number of unpaired electrons or oxygen vacancies. (40,41)
In Figure 2, the electrochemical performance of wet nonaqueous ZIBs having K-MnO2 and NH4-MnO2 cathodes is shown. In Figure 2A, after potassium atoms were substituted with NH4+ cations, the initial discharge capacity of the MnO2 cathode and the cell voltage significantly increased (specific capacity from 195 to 247 mAh/g and cell voltage from 0.95 to 1.04 V at a current density of 50 mA/g). As for the rate capability test (Figure 2B), NH4-MnO2 displayed an average specific capacity of 207, 176, 164, 155, 141, and 111 mAh/g at current densities of 50, 100, 150, 200, 300, and 500 mA/g, respectively. These findings are superior to those of K-MnO2 (177, 150, 139, 129, 103, and 72 mAh/g at 50, 100, 150, 200, 300, and 500 mA/g, respectively). In Figure 2C,D, both the K-MnO2 and NH4-MnO2 samples exhibited higher average discharge voltages compared with that in the first cycle and were not much different from each other. However, at high current densities (300 and 500 mA/g), the NH4-MnO2 sample tends to have a higher rate capability. Due to the high overpotential of the Zn anode, a low voltage during the first cycle occurred, as observed in Figure S5. The first charging may be attributed to the formation of the SEI at the Zn anode, which mobilized the plating/stripping of Zn. Nevertheless, this issue is beyond the scope of this study. Thus, it will be discussed in future publications.

Figure 2

Figure 2. Results of electrochemical performance: (A) GCD results at the first cycle, (B) rate capability, voltage profile vs specific capacity using GCD of (C) K-MnO2 and (D) NH4-MnO2, (E) CV results, (F) GITT results, and (G) cyclability results.

In Figure 2E, CV results at a scan rate of 0.2 mV/s are shown. It is seen that both the K-MnO2 and NH4-MnO2 samples display at least two reduction peaks and two oxidation peaks. This outcome indicates that there are at least two redox reactions involved in the charge-storage mechanism of MnO2 in this electrolyte. When compared with K-MnO2, the NH4-MnO2 sample exhibited better redox kinetics, as can be seen via the higher current density trend along the IV-axis. In addition, the intensity of both oxidation and reduction peaks increased, thus indicating the improved diffusion limit of ions involved in the charge-storage reaction when NH4+ was introduced.
In Figure S6, peaks 1, 2, 3, and 4, which appeared in the CV results, were analyzed using Dunn’s methodology. (42) Thus, all peaks of the K-MnO2 samples revealed b-values of 0.673, 0.607, 0.688, and 0.723, respectively. In contrast, the b-values of the NH4-MnO2 sample were 0.690, 0.661, 0.691, and 0.750, respectively. It is seen that all b-values <0.75 signify that the charge-storage mechanism of both the K-MnO2 and NH4-MnO2 samples was a mixture of capacitive-controlled and diffusion-controlled behavior. The NH4-MnO2 sample exhibited slightly higher b-values in every peak compared to that of the K-MnO2 sample, indicating faster charge-storage kinetics upon charging and discharging.
Further, GITT was conducted using a rest period of 2 h and a discharging current density of 100 mA/g for 5 min. In Figure 2F, the results are given. During 0–20 h of GITT, the voltage profiles of K-MnO2 and NH4-MnO2 were almost similar to each other, indicating the similar diffusivity of guest ions in these samples upon the start of discharging. After 20 h of GITT, the size of the discharging overpotential of K-MnO2 started to overcome that of the NH4-MnO2 sample. In Figure S7, the plot of calculated diffusivity versus state of charge (SOC) signifies a significant improvement in the diffusivity of guest ions in the MnO2 structure when NH4+ was presented. In addition, EIS results (Figure S8 and Table S2) demonstrate the minimized charge-transfer resistance of the cathode. When NH4+ is introduced onto MnO2, the diffusion of guest ions can be mobilized, thus improving the kinetics of these ions upon the intercalation reaction. Such an outcome results in higher specific capacity and superior rate performance of the cathode having preintercalated NH4+ and agrees well with the GCD and CV results.
In Figure 2G, both the cycling stabilities of the K-MnO2 and NH4-MnO2 samples are measured and illustrated. Initially, the K-MnO2 and NH4-MnO2 samples displayed specific capacities of 118 and 169 mAh/g, respectively (current density 200 mA/g). After 500 cycles, the specific capacity of the K-MnO2 and NH4-MnO2 samples decreased to 96 and 143 mAh/g, yielding capacity retention of 81 and 85%, respectively. The results show that in terms of stability, both the K-MnO2 and NH4-MnO2 samples are found to be about the same. Nevertheless, in terms of specific capacity, the NH4-MnO2 sample clearly outnumbered K-MnO2.
In Figure 3A, the synchrotron XRD (λ = 1.033 Å) results of K-MnO2 and NH4-MnO2 after the fifth cycle are shown. Hence, XRD spectra reveal both birnessite characteristics and chalcophanite (ZnMn3O7·3H2O) characteristics at the charged state of the K-MnO2 and NH4-MnO2 samples. (43,44) XPS results of the charged K-MnO2 cathode display a trace of Zn2+ remaining in the cathode (Figure S9). In addition, EXAFS results (Figure S10 and Table S3) of both K-MnO2 and NH4-MnO2 are well-matched with the ZnMn3O7·3H2O structure, as in the literature. (43,45) Thus, the formation of chalcophanite after the first charge/discharge was confirmed. After discharging, the intensity of the chalcophanite characteristic peaks decreased. Further, characteristics of Zn oxide (ZnO; 2θ of 21.1, 22.9, 24.1, 31.5, 37.1, 40.9, and 44.0°) were observed in the XRD spectra of both the K-MnO2 and NH4-MnO2 samples at the discharged state, indicating the formation of ZnO upon discharging at the cathode. (46) In Figure S11, small white pellets were detected via FE-SEM in the discharged cathode. However, these ZnO precipitates were found to be highly reversible (Figure S12). Such a by-product reflects that the dissociation of water, i.e., proton (H+), could be involved in the charge storage of these cathodes. The remaining hydroxide anions could result in the formation of hydroxozincate; accordingly, an oversaturated content of hydroxozincate at the cathode–electrolyte interface led to the formation of ZnO. (47) Although the XRD results cannot provide clear information regarding the phase transformation of K-MnO2 and NH4-MnO2 after discharging, it can be inferred that their “birnessite-like” characteristics still existed. In Figure S13, the Raman spectra of the discharged cathodes indicate the existence of ν1, ν2, and ν3, which are characteristic of the layers of the MnO6 octahedra. (48)

Figure 3

Figure 3. Charge-storage mechanism determination results: (A) synchrotron XRD results of K-MnO2 and NH4-MnO2 at charge/discharge state (after fifth cycle), (B, C) XANES spectra measured via in situ XAS technique, (D, E) density functional theory (DFT)-optimized models and plots of the partial density of states (PDOS), (F) zoom-in image of the XANES results, (G) in-situ EXAFS of K-MnO2 upon discharging, (H) in-situ EXAFS of NH4-MnO2 upon discharging, (I) schema of the stabilization of MnO2 using NH4+ cations, and (J) EXAFS of K-MnO2 and NH4-MnO2 at a discharged state.

In situ XAS technique was carried out in order to probe the structural evolution of Mn in the K-MnO2 and NH4-MnO2 samples in a real-cell environment. Mn K-edge XANES spectra (Figure 3B,C) highlight the decrease in the absorption edge energy of Mn, which corresponds to the decrease in their oxidation number upon discharging. In comparison with MnO2 and Mn2O3 references, Mn(IV) and Mn(III), the absorption edge energy of both K-MnO2 and NH4-MnO2 changed within the gap of the absorption edge energy of MnO2 and Mn2O3: Mn within these cathodes tended to change from an oxidation number of almost +4 to about +3. Such an evolution indicates that the charge-storage redox reaction of these cathodes mainly relied on the valency evolution of Mn in the solid phase. (49) Both K-MnO2 and NH4-MnO2 display an evolution in the white-line area and a local vibration dynamic during the postedge region during discharging. Although the white-line part in K-edge results of Mn cannot directly exhibit the information on Mn 3d orbitals, the intensity of such a part can be used for indicating the situation in 3d orbital in case the neighboring atoms of Mn are O. (50,51) The decrease in the white-line intensity upon discharging signifies the decrease of unoccupied 3d orbitals of Mn, which corresponds to the progressive formation of the intercalated state of the guest ions from the electrolyte onto the MnO2 layers. (52)
In accordance with crystal field theory, the electronic configuration of Mn was investigated using density functional theory (DFT). Details of the simulation and the DFT-optimized models (Figure S14) are given in the Supporting Information (SI). In Figure 3D,E, the plot of the partial density of states (PDOS) is shown. After the intercalation of Zn2+, the energy of the d orbital (εd-Mn) of the K-MnO2 shifts −0.28 eV. In contrast, the NH4-MnO2 displays the εd-Mn shift of −0.19 eV, implying that the d orbitals of Mn in the NH4-MnO2 possess higher stability. Such a result was also confirmed by analyzing the pre-edge part of the XANES spectra (Figure 3F). As such, this pre-edge part is ascribed to the excitation of 1s–3d orbitals. The curves, marked at two points, correspond to the orbitals of Mn 3d, which bonded with 2p orbitals of the neighboring O, viz., t2g and eg. The height of these peaks corresponds to the unoccupied degree of such orbitals. (53) Upon discharge, it is seen that the intensity of the eg peak of K-MnO2 decreased dramatically. Evolution of the K-MnO2 sample indicates that Mn(III) having t2g3eg1 was formed upon discharging, thus resulting in the splitting of eg into different energy levels. Hence, the Jahn–Teller (JT) distortion of MnO6 units occurred. (54) It is noted that the NH4-MnO2 sample did not show a severe drop in the size of the eg peak. This outcome denotes that the splitting in the energy of the eg orbital of Mn in the NH4-MnO2 sample was minimal compared to that of the K-MnO2 sample, demonstrating that MnO6 in the presence of the NH4+ cation can retain its own shape upon reduction in the oxidation number of Mn.
In Figure 3G,H, in situ EXAFS results of the K-MnO2 and NH4-MnO2 samples are shown. The spectra display two shells (Mn–O and Mn–Mn). The Mn–O shell corresponds to the bonding between the center atom (Mn) and neighboring O atoms that bonded with Mn. The Mn–Mn shell represents other Mn atoms nearby. As the discharging of the battery progressed, the intensity of Mn–O and Mn–Mn shells of both the K-MnO2 and NH4-MnO2 samples decreased. Such behavior corresponds to the degree of decentralization in the distribution of Mn–O bonding distance and Mn–Mn distance in the cathode. (55) In comparison with the NH4-MnO2 sample, the K-MnO2 sample displayed a more drastic reduction in its intensity. In addition, upon discharging, it is clearly seen that the peak position of the Mn–O shell and Mn–Mn shell of the K-MnO2 sample shifted to the left and right, respectively: this shift indicates that the MnO6 unit in the MnO2 layers started to elongate, which is the nature of MnO6 units when the oxidation number of Mn reduces from +4 to +3. In contrast, the peak position of Mn–O and Mn–Mn shells of the NH4-MnO2 sample was almost unchanged. (55) Such behavior occurs due to the formation of hydrogen bonds: NH–O–Mn interaction, which results in a “preinserted stress” toward O of MnO6 (Figure 3I). Upon discharging, the hydrogen-bonding network created by NH4+ had a role in manipulating the distortion of the remaining MnO6(IV) and MnO6(III) in the cathode. As a result, the geometrical differences between MnO6(III) and MnO6(IV) are minimized. The disproportionation issue that occurred in the K-MnO2 sample hindered the transport of guest ions during the intercalation reaction, resulting in poor kinetic of the cathode. (53,55) Hence, the introduction of the NH4+ cation can mobilize the ion migration and accelerate surface kinetic via the improved surface of MnO2 caused by hydrogen-bond networking, which promotes reduced charge disproportionation.
To clarify the speciation of the inserted species in the cathode during discharging of the battery, in situ XAS at the Zn K-edge energy was employed. In Figure 3J, the Zn K-edge EXAFS results of the discharged K-MnO2 and NH4-MnO2 are shown. The spectrum of the K-MnO2 sample displayed two shells at 1.53 and 2.91 Å, which correspond to the Zn–O bonding distancing and Zn with other metal atoms. NH4-MnO2 exhibits shells at 1.56 and 2.94 Å. The EXAFS fitting was used in order to specify the species of such a structure (Figure S15 and Table S4). K-MnO2 spectrum fitted in well with ZnO, which indicates that proton insertion highly contributed to the charge storage of the K-MnO2 sample. (46) In the NH4-MnO2 sample, its spectrum is well-matched with Zn in the chalcophanite structure; Zn insertion is more likely to contribute to charge-storage reaction rather than proton insertion. (43) Typically, migration of Zn2+ having a +2 oxidation number is hindered by a strong electrostatic impulsion between guest Zn2+ and the host structure. Consequently, a proton possesses a +1 charge and, being much smaller in size, can take the place of Zn2+ in the situation, whereby Zn2+ are not free to move, as in nonaqueous media. (56) Improvement in the mobility and surface kinetics of the cathode, influenced by the NH4+ cation, has a crucial role to play in determining charge-storage pathways and results in superior specific capacity.

4. Conclusions

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In this paper, the results demonstrate that the addition of preintercalated ammonium ions could successfully enhance the performance of wet nonaqueous ZIBs, utilizing MnO2 as a cathode material. The simultaneous presence of both distorted Mn(III) and undistorted Mn(IV) in the cathode structure is identified as a major impediment to ion migration, adversely affecting the surface kinetics of the MnO2 cathode. The introduction of ammonium, however, characterized by its robust hydrogen-bonding capability, effectively addresses the charge disproportionation challenge by forming NH–O–Mn networks. This structural innovation facilitates a more uniform geometric distortion between MnO6(IV) and MnO6(III), thereby optimizing both surface kinetics and ion transport. Such enhancements greatly elevate the role of Zn2+ insertion over proton reactions, contributing to the remarkable increase in the specific capacity. The MnO2 cathode, modified with ammonium ions, achieved an unprecedented capacity of 247 mAh/g, confirming its durability over 500 cycles with a capacity retention of 85%. These findings offer valuable insights for future MnO2 cathode development, promoting the design and application of high-performance ZIBs.

Data Availability

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The authors declare that all data supporting the findings of this study are available within the paper and its Supporting Information file.

Supporting Information

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The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acsami.4c07239.

  • The electrochemical cell for the in situ XAS measurement, XPS of the NH4-MnO2 powder, Rietveld refinement results of the XRD spectra, EPR, GCD, CV, and Dunn’s analysis, diffusivity, EIS, XPS of the K-MnO2 cathode, Mn K-edge EXAFS, FE-SEM of the discharged cathodes, operando XRD of K-MnO2, Raman spectra, DFT-optimized models and description of DFT calculations, and Zn K-edge EXAFS (PDF)

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Author Information

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  • Corresponding Authors
    • Myong Yong Choi - Core-Facility Center for Photochemistry & Nanomaterials, Department of Chemistry (BK21 FOUR), Research Institute of Natural Sciences, Gyeongsang National University, Jinju 52828, Republic of KoreaOrcidhttps://orcid.org/0000-0001-5729-5418 Email: [email protected]
    • Soorathep Kheawhom - Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, ThailandCenter of Excellence on Advanced Materials for Energy Storage, Chulalongkorn University, Bangkok 10330, ThailandOrcidhttps://orcid.org/0000-0002-3129-2750 Email: [email protected]
  • Authors
    • Wathanyu Kao-ian - Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, Thailand
    • Jinnawat Sangsawang - Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, Thailand
    • Mohan Gopalakrishnan - Department of Chemical Engineering, Faculty of Engineering, Chulalongkorn University, Bangkok 10330, ThailandOrcidhttps://orcid.org/0000-0003-4537-7170
    • Suttipong Wannapaiboon - Synchrotron Light Research Institute, 111 University Avenue, Muang District, Nakhon Ratchasima 30000, ThailandOrcidhttps://orcid.org/0000-0002-6765-9809
    • Athis Watwiangkham - Department of Chemistry, Faculty of Science, Ubon Ratchathani University, Ubon Ratchathani 34190, Thailand
    • Siriporn Jungsuttiwong - Department of Chemistry, Faculty of Science, Ubon Ratchathani University, Ubon Ratchathani 34190, ThailandOrcidhttps://orcid.org/0000-0001-5943-6878
    • Jayaraman Theerthagiri - Core-Facility Center for Photochemistry & Nanomaterials, Department of Chemistry (BK21 FOUR), Research Institute of Natural Sciences, Gyeongsang National University, Jinju 52828, Republic of Korea
  • Author Contributions

    W.K.-i. and S.K. were responsible for conceptualization. W.K.-i., S.W., and S.K. were responsible for methodology. W.K.-i., J.S., and S.W. performed the experiments. W.K.-i., M.G., S.W., S.J., J.T., M.Y.C., and S.K. performed the formal analysis. W.K.-i. performed visualization. S.K. was responsible for funding acquisition. S.K. supervised the study. W.K.-i. and S.K. wrote the original draft. All authors wrote, reviewed, and edited the manuscript.

  • Notes
    The authors declare no competing financial interest.

Acknowledgments

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The Program Management Unit for Human Resources & Institutional Development, Research, and Innovation (B16F640166) is acknowledged. W.K.-i. thanks Chulalongkorn Academic Advancement into its second Century Project for Postdoctoral Fellowship. M.Y.C. acknowledges the support of the Korea Basic Science Institute (National Research Facilities and Equipment Center) grant funded by the Ministry of Education (Nos. 2019R1A6C1010042 and 2021R1A6C103A427).

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  8. Huaizheng Ren, Sai Li, Liang Xu, Lei Wang, Xinxin Liu, Lei Wang, Yue Liu, Liang Zhang, Han Zhang, Yuxin Gong, Chade Lv, Dongping Chen, Jianxin Wang, Qiang Lv, Yaqiang Li, Huakun Liu, Dianlong Wang, Tao Cheng, Bo Wang, Dongliang Chao, Shixue Dou. Tailoring Water‐in‐DMSO Electrolyte for Ultra‐stable Rechargeable Zinc Batteries. Angewandte Chemie 2025, https://doi.org/10.1002/ange.202423302
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  • Abstract

    Figure 1

    Figure 1. Powder characterization results: (A) TEM image of K-MnO2, (B) Mn EDS mapping of K-MnO2, (C) K EDS mapping of K-MnO2, (D) TEM image of NH4-MnO2, (E) Mn EDS mapping of NH4-MnO2, (F) K EDS mapping of NH4-MnO2, (G) N EDS mapping of NH4-MnO2, (H) zoom-in TEM image of K-MnO2, (I) zoom-in TEM image of NH4-MnO2, (J) XRD results of K-MnO2 and NH4-MnO2, (K) FT-IR results, (L) structure of the synthesized NH4-MnO2, (M) deconvoluted Raman spectra of K-MnO2, and (N) deconvoluted Raman spectra of NH4-MnO2.

    Figure 2

    Figure 2. Results of electrochemical performance: (A) GCD results at the first cycle, (B) rate capability, voltage profile vs specific capacity using GCD of (C) K-MnO2 and (D) NH4-MnO2, (E) CV results, (F) GITT results, and (G) cyclability results.

    Figure 3

    Figure 3. Charge-storage mechanism determination results: (A) synchrotron XRD results of K-MnO2 and NH4-MnO2 at charge/discharge state (after fifth cycle), (B, C) XANES spectra measured via in situ XAS technique, (D, E) density functional theory (DFT)-optimized models and plots of the partial density of states (PDOS), (F) zoom-in image of the XANES results, (G) in-situ EXAFS of K-MnO2 upon discharging, (H) in-situ EXAFS of NH4-MnO2 upon discharging, (I) schema of the stabilization of MnO2 using NH4+ cations, and (J) EXAFS of K-MnO2 and NH4-MnO2 at a discharged state.

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  • Supporting Information

    Supporting Information


    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acsami.4c07239.

    • The electrochemical cell for the in situ XAS measurement, XPS of the NH4-MnO2 powder, Rietveld refinement results of the XRD spectra, EPR, GCD, CV, and Dunn’s analysis, diffusivity, EIS, XPS of the K-MnO2 cathode, Mn K-edge EXAFS, FE-SEM of the discharged cathodes, operando XRD of K-MnO2, Raman spectra, DFT-optimized models and description of DFT calculations, and Zn K-edge EXAFS (PDF)


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