Mini-review: progress on micro/nanoscale MnMoO4 as an electrode material for advanced supercapacitor applications

Zhu Zhu a, Yan Sun *a, Chunsheng Li *ac, Chen Yang a, Lin Li b, Jiahao Zhu a, Shulei Chou *b, Miaomiao Wang a, Didi Wang a and Yuanliang Li d
aSchool of Chemistry and Life Sciences, Suzhou University of Science and Technology, Suzhou City, Jiangsu Province 215009, P. R. China. E-mail: juzi147@163.com; lichsheng@163.com
bInstitute for Carbon Neutralization, College of Chemistry and Materials Engineering, Wenzhou University, Wenzhou, Zhejiang 325035, P. R. China. E-mail: chou@wzu.edu.cn
cXi’an Key Laboratory of Advanced Photo-electronics Materials and Energy Conversion Device, School of Science, Xijing University, Xi’an, 710123, P. R. China
dHebei Provincial Key Laboratory of Inorganic Nonmetallic Materials, Key Laboratory of Environment Functional Materials of Tangshan City, College of Materials Science and Engineering, North China University of Science and Technology, Tangshan City, Hebei Province 063210, P. R. China

Received 24th June 2021 , Accepted 17th August 2021

First published on 18th August 2021


Abstract

Manganese molybdate (MnMoO4) has attracted extensive attention as the electrode material for supercapacitors, owing to its high theoretical specific capacity, excellent redox activity, good structural stability, abundant reserves and low cost. However, its low actual specific capacity and poor electronic conductivity limit the industrial development and practical applications. In this mini-review, the microstructure, preparation strategies, plausible reaction mechanisms, drawbacks and corresponding improvement technologies of micro/nanoscale MnMoO4 materials are systematically summarized. In addition, the challenges and prospects of MnMoO4 for supercapacitors in future applications are discussed.


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Yan Sun

Yan Sun obtained her BS degree from the Liaoning Normal University in 2004, MS degree from Wenzhou University in 2007, and PhD degree from Nankai University (China) in 2010. She was promoted to a full Professor in North China University of Science and Technology in 2017. She has been teaching at Suzhou University of Science and Technology since 2019 and is leading a research team investigating functional micro/nanomaterials and their clean energy storage and conversion in supercapacitors, lithium-ion batteries, metal–air batteries, and sodium-ion batteries.

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Chunsheng Li

Chunsheng Li received his MS and PhD degree from the Institute of New Energy Materials Chemistry in Nankai University (Tianjin, China) in 2007 and 2010, respectively. He is a Professor at the North China University of Science and Technology, Hebei Province, since 2017. He works at Suzhou University of Science and Technology, and is mainly engaged in nanostructured materials for advanced applications in supercapacitors, lithium-ion batteries and metal–air batteries (Mg-air batteries, Zn–air batteries and Al-air batteries).

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Shulei Chou

Shulei Chou is a professor at the College of Chemistry and Materials Engineering, Wenzhou University. He obtained his BS (2003) and MS degree (2007) in Nankai University, China. He received his PhD degree from the University of Wollongong in 2010. His research has been focused on energy storage materials for battery applications, especially on novel composite materials, new binders, and new electrolytes for Li/Na batteries.

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Yuanliang Li

Yuanliang Li received his PhD degree in materials science from Tianjin University. Currently, he is a full associate professor at College of Materials Science and Engineering, North China University of Science and Technology. His current research interests include in situ measurement technologies, especially in electrode mechanisms.


1. Introduction

Based on the growing resources crisis and environmental pollution issues, the exploration of efficient conversion technologies and advanced energy storage devices is as important as the rational utilization of various renewable energies to promote the sustainable development of society.1–5 At present, electrochemical capacitors with fast charge/discharge rate, wide operating voltage range, long cycle-life and economical maintenance cost, have been considered as one of the most popular and practical means for storing and delivering electrical energy.6–10Fig. 1 shows the plot of the power density versus energy density for different electrochemical energy storage technologies.6 Supercapacitors with considerable power delivery performance bridge the gap between traditional capacitors and batteries, but their energy density is much lower than that of secondary lithium-ion and sodium-ion batteries.11–14 It is necessary to improve the electrochemical performances of supercapacitors to meet the higher requirements of future life and production, ranging from wearable electronic devices to electric vehicles and industrial equipment, by deepening our understanding of the nano-scale electrochemical interface.15–18
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Fig. 1 The power density versus energy density of various energy storage devices.6 Copyright 2020, Elsevier.

Compared with the electric double layer capacitor (EDLC), the pseudocapacitor exhibits higher specific capacitance, which is the consequence of its electrode materials’ surface possessing rapid redox reaction.19–22Fig. 2a and b illustrate the schematic diagrams of EDLC and pseudocapacitor.7 For the pseudocapacitor, transition metal oxides are recognized as ideal functional materials by virtue of their special structure and physical/chemical properties,23–25 including MnMoO4,26 CoMoO4,27,28 NiMoO4,29,30 ZnMoO4,31 Co3O4,32 Mn2O3,33 NiCo2O4,34,35 and MnCo2O4,36etc.


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Fig. 2 The schematic diagrams: (a) EDLC, and (b) pseudocapacitor.6 Copyright 2020, Multidisciplinary Digital Publishing Institute. (c) The number of published papers, and (d) the SCI citation times with the topics on “MnMoO4” and “Supercapacitor”. Data were derived from the Web of Science on March 30, 2021.

Among these transition metal oxides, MnMoO4, showing superior structural stability, good redox activity, cost-effective and environmental friendliness, has been investigated to expand the practical applications.37–39 Currently, MnMoO4 as an electrode has received extensive attention, which can be proved by the number of published articles and SCI citation times on the topic increasing significantly between the years of 2012–2020 (Fig. 2c and d). The material mainly possesses the following advantages: (1) α-MnMoO4 belongs to a monoclinic structure in the space group of C2/m with the lattice parameters of a = 10.469 Å, b = 9.516 Å, c = 7.143 Å, α = 90.0°, β = 106.28° and γ = 90.0°.40–42 MnMoO4 exhibits a good structural stability (compared with Co-based molybdates and Ni-based molybdates) by calculation, which is attributed to its special structure and lower cohesive energy.26,43 (2) MnMoO4 possesses a high theoretical capacity, originating from the synergistic effect of Mn and Mo (manganese ions contribute redox activity, and molybdenum ions offer electronic conductivity).44 (3) It is of strategic and practical significance to develop and utilize molybdenum resources, because 56% molybdenum mines of the world are in China under the survey data in 2016.45

Herein, this mini-review provides a systematic overview of the latest advances in the microstructures in favor of the outstanding electronic conductivity, superior interface reaction kinetics and the excellent diffusion kinetics to improve the electrochemical performance of MnMoO4 for supercapacitor, especially for the specific capacitance, rate capability and cycling stability. Furthermore, the morphology modification, heterostructure fabrication, electrochemical properties and plausible reaction mechanisms of MnMoO4 in recent years have been summarized. Finally, the remaining challenges and the future optimization direction of MnMoO4 materials are put forward, which furnishes guidance that serves the commercialization of novel MnMoO4-based electrodes.

2. The structure and synthesis of MnMoO4 materials

2.1 Crystal structure of MnMoO4

In general, anhydrous MnMoO4 has three polymorphs: the first phase is α-MnMoO4, the second phase is ω-MnMoO4, and the third phase is isostructural with α-CoMoO4.42,46–49 Among these, α-MnMoO4 is stable under normal temperature and pressure, and ω-MnMoO4 can be converted into α-MnMoO4 upon heating overnight in the air at 600 °C.50 Meanwhile, the α-MnMoO4 lattice is composed of corner-shared MnO6 octahedra and MoO4 tetrahedra.42 Mn and Mo occupy the centers of octahedral MnO6 and tetrahedral MoO4, respectively, as shown in Fig. 3.43 In particular, the synergistic distortion in α-MnMoO4 results in the generation of extra channels for the kinetic processes, and thus paves a good way for promoting adequate reactions between the electrode material and electrolyte.
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Fig. 3 The crystal structure of α-MnMoO4.43 Copyright 2017, American Chemical Society.

2.2 Fabrication methods for MnMoO4

It is well known that the synthesis route greatly affects the electrochemical behaviors of energy storage, because the morphology and surface area of the electrode materials are highly dependent on the fabrication conditions.41,50 Up to now, the common preparation methods for micro/nanoscale MnMoO4 include solid-phase method,51,52 combustion synthesis,53 sonochemical route,16 sol–gel,54–56 co-precipitation,31,57,58 hydrothermal/solvothermal reaction,59–61 and microwave irradiation-assisted technique.62,63 Among the above available technologies in preparing nanomaterials, the hydrothermal/solvothermal reaction is regarded as one of the most efficient processes of soft chemistry. The closed reaction system facilitates the reduction of distractions from external factors, and promotes the interaction of Mn and Mo raw materials in super-critical status with high pressure.64–66 For the precipitation strategy, it is difficult to avoid the agglomeration of nano-product particles resulting from relatively high deviations of the local concentration and temperature in the reactant solutions. To solve these issues, the microwave irradiation-assisted method has been widely applied to prepare MnMoO4 micro/nanoparticles, owing to its obvious advantages, such as high penetration depth, low thermal gradient effect and fast synthesis speed.67,68 For example, Muralidharan and his colleagues synthesized α-MnMoO4 nanorods through co-precipitation (Cp-MnMoO4) and microwave hydrothermal route (MH-MnMoO4), respectively.69 The Cp-MnMoO4 nanorods with a diameter of ∼200 nm and a length of ∼1.6 μm deliver a specific capacitance of 143 F g−1 at a current density of 1.0 A g−1. Meanwhile, the tube-like MH-MnMoO4 (diameter: ∼600 nm and length: ∼1.6 μm) composed of 5–6 pieces of nanorods (diameter: 100–200 nm) achieves a specific capacitance of 551 F g−1 at 1.0 A g−1 using 2 M NaOH as the electrolyte. As the above data show, the MH-MnMoO4 exhibits higher specific capacitance than that of Cp-MnMoO4. This is due to the tube-like morphology possessing a larger surface area and richer electroactive sites.69,70 Moreover, our group obtained several MnMoO4 nanomaterials with different morphologies via the microwave irradiation method: (1) MnMoO4 microrods, which were self-assembled from tens of MnMoO4 nanosheets with a thickness of 30–60 nm and a length of 4–10 μm.71 (2) MnMoO4 nanospheres with a diameter of 50–80 nm.72 (3) Three-dimensional (3D) MnMoO4 nanoflowers/graphene composites,73 as presented in Fig. 4a–c. (4) MnMoO4 nanowires/graphene composites, as depicted in Fig. 4d–f.74 The synthesis routes and experimental condition factors (fabricating temperature, reaction time and concentration) affect the shape and size of the products, and the morphologies and dimensions of the MnMoO4 particles can be effectively controlled by further optimizing these parameters.
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Fig. 4 (a–c) Scanning electron microscopy (SEM) images of the MnMoO4 nanoflowers/graphene composites.73 Copyright 2021, CN 112875756 A. (d–f) SEM images of the MnMoO4 nanowires/graphene composites.74 Copyright 2021, CN 112875757 A.

3. Research status of MnMoO4

3.1 Key parameters affecting the electrochemical performances of MnMoO4 materials

3.1.1 The electronic conductivity. The actual low specific capacitance of MnMoO4 hinders its wide applications, which is associated with its poor electronic conductivity and slow reaction kinetics. α-MnMoO4 is a n-type semiconducting material with a band gap of 1.96 eV.75 The narrow band gap allows electrons in the valence band to be more easily excited to the conduction band under an applied external voltage. Although Mo atoms with a smaller electron contribution do not participate in the redox reactions of the MnMoO4 electrochemical activity under alkaline condition, Mo atoms mainly offer electrical conductivity to improve the electrochemical properties of MnMoO4.43,76 In addition, the unsatisfactory electronic conductivity of MnMoO4 as an electrode material restricts the current response over a wide voltage range,77,78 mainly through the form of compounds with special microstructure to make up for this deficiency.
3.1.2 The interface reaction kinetics. The transfer rate of the electrons/ions and the redox ability of the active material largely determine the storage capacity of the Faradaic supercapacitors, especially for the high-rate cycling and low-temperature properties (Fig. 5).23,79,80 MnMoO4 particles with more regular morphologies are assembled from smaller ones with large surface areas, which is advantageous for the acceleration of reaction kinetics and the increase in the charge storage.41,81,82 Many feasible means are facilitated to improve the reaction kinetics of MnMoO4, such as reducing the size of active materials, adjusting the morphology and designing the novel microstructures.50,83
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Fig. 5 (a) Principles of the MnMoO4 nanowires/graphene electrodes in the supercapacitor. (b) The transfer of electrons/ions at the MnMoO4 nanowires/graphene electrodes during charge and discharge.
3.1.3 The diffusion kinetics. The particle size of MnMoO4 is one of the significant parameters for influencing the ion diffusion kinetics of the supercapacitor, which is a crucial direction to regulate the diffusion and transport of the ion/electron, leading to high specific capacity and excellent rate capability electrode materials.84–86 In general, owing to the reducing particle size, the internal active space of the MnMoO4 electrode can be adequately occupied, and the rapid ion diffusion improves the reaction kinetics.87–89 In addition, ion diffusion within the MnMoO4 host material depends on the diffusion distance and ion diffusion coefficient (τ = L2/D, where τ, D and L are the ion diffusion time, ion diffusion coefficient and diffusion length, respectively), suggesting that the particle size minimization can directly shorten the diffusion distance and therefore enhance the rate capability.90,91 For instance, Minakshi et al. fabricated bulk-like α-MnMoO4 with the size of 10–20 μm using a precipitation technique that displayed a specific capacitance of 200 F g−1 at 1.6 A g−1.92 In addition, Ramaraj and co-workers prepared MnMoO4 nanorods with a diameter of ∼160 nm and length of 2.3 μm through a co-precipitation method, showing a high discharge capacity of 424 F g−1 at 1.0 A g−1.93 Another example includes the α-MnMoO4 nanorod electrodes with a diameter of ∼30 nm and length of 75 nm, which were synthesized via a microwave-assisted method by Harichandran et al. and yielded a higher specific capacitance of 733 F g−1 at 1.0 A g−1.63 In all, these results distinctly reveal that the effective decreasing particle size is beneficial for the ion diffusion kinetics of MnMoO4 electrodes, thus enabling a good specific capacitance and rate capability.

3.2 Strategies to improve the performances of the MnMoO4 electrodes

3.2.1 Morphology modification. Morphology modification has been regarded as an effective approach to enhance the specific capacity and cycling performance of MnMoO4 electrodes for supercapacitors, owing to the larger specific surface area and greater pore size caused by various structures.94 In this mini-review, the electrodes assembled by MnMoO4-based materials will be systematically divided into the following three categories with different dimensionalities:95

(1) One-dimensional (1D) structures. The advantages of 1D structures for a stable structure and effortless strain relaxation are providing fast axial electron transport and shortening ion diffusion pathways.96,97 For instance, Mai and co-workers synthesized hierarchical MnMoO4/CoMoO4 heterostructured nanowires via a simple refluxing method, and the 1D MnMoO4 nanowires and 1D CoMoO4 nanorods were used as the backbone material and shell material, respectively. The hierarchical structure is beneficial to give sufficient active sites for the redox reactions. Consequently, the specific capacitance of the 3D composite nanowires can reach 187 F g−1 at 1.0 A g−1, which is higher than that of pure MnMoO4 (9.7 F g−1), CoMoO4 (62.8 F g−1) and MnMoO4/CoMoO4 composite with a non-three-dimensional structure (69.2 F g−1). Surprisingly, the as-prepared 3D MnMoO4/CoMoO4 nanocomposite displays an exceptional reversibility with 98% of the initial capacitance retained after 1000 cycles.98 In addition, Lu et al. fabricated 1D porous MnMoO4 nanotubes via a single-spinneret electrospinning technique with an annealing process in air. The tube-like microstructure of MnMoO4 aims to improve the contact between the electrolyte and electrode to optimize the electrochemical properties. Therefore, the aforementioned MnMoO4 nanotubes electrode exhibits a specific capacitance of 620 F g−1 at 1.0 A g−1, and retains 91% of the specific capacitance after 10[thin space (1/6-em)]000 cycles.26

(2) Two-dimensional (2D) structures. By supplying more active sites on the larger surfaces and higher utilization of the whole active planar materials to result in fast charge-transfer processes, the specific capacitance and cycling stability are promoted to some extent.99–102 Mu et al. produced ultrathin 2D manganese molybdate (MnMoO4·nH2O) nanosheets that anchored on nickel foam (NF) surfaces through a one-step hydrothermal reaction. These nanosheets present a specific capacitance of 1271 F g−1 at a scan rate of 5 mV s−1, and retained 84.5% of its initial specific capacitance after 2000 cycles at a current density of 10.0 A g−1.101

(3) 3D structures. Remarkably, on the basis of the previous research works, the 3D structures combine the merits of functional 1D and 2D structures, and possess their unique features of the sturdy structure, synergistic effects between different elements, preeminent permeabilities and many channels for Faraday reactions, which has attracted intense attention.103–105 For example, Feng and co-workers developed 3D hierarchical MnMoO4/NiWO4 microspheres (self-assembled by MnMoO4 nanoflakes and NiWO4 nanoparticles) using a hydrothermal method, which delivered a capacitance of 598 F g−1 at 1.0 A g−1 and the capacitance retention of 82% after 5000 cycles. It is because the 3D microspheres afford vast open space and electroactive sites for Faradaic reactions to heighten the specific capacity and cycle stability.103 Furthermore, Gu and co-workers reported a facile hydrothermal and calcination method to obtain 3D NiCo2O4@MnMoO4 core/shell nano-flowers that demonstrate a specific capacitance of 1118 F g−1 at 1.0 A g−1, and a long-term cycling stability of 87.85% after 5000 cycles.104

In summary, these valuable consequences reveal that the sequence of the specific capacity and cycle property from better to average is 3D > 2D > 1D by only considering the influence of the microstructures of the MnMoO4-based materials, while neglecting the difference of the diverse sorts of electrolytes. As a consequence, MnMoO4-based materials with 3D structures overcome the restrictions of materials with single or two dimensionalities, which offer functional properties of excellent surface area for effective ion/charge transport pathways, minimized electrode polarization and alleviated the volume expansion/shrinkage, leading to high specific capacitance and superior cycle stability to show significant potential in supercapacitor applications.106–111 Finally, the morphology adjustment of the electrode materials suggests a future direction for more research studies in further enhancing the electrochemical performances.

3.2.2 In situ growth of MnMoO4 on the conductive metal substrate. The conductive metal substrate with a 3D porous structure is generally considered a good deposition material because of its stable structure and good electronic conductivity.83 For instance, the 3D fan-like α-MnMoO4 nanostructures with an average radius of 5 μm were in situ grown on a Cu coil prepared by Wang and his colleagues via a precipitation process.112 The 3D fan-like α-MnMoO4 displays a specific capacitance of 562 F g−1 at 1.0 A g−1 and a long-term cycling stability with 99.8% of the initial capacitance retained after 1000 cycles using 2 M KOH as the electrolyte. The commendable electrochemical behaviors of the as-prepared nanoribbon-based α-MnMoO4 electrode result from the novel 3D hierarchical nanostructures. Based on the above study, Xu et al. reported a hydrothermal route to prepare the MnMoO4 ultrathin nanosheets on nickel foam (NF@MnMoO4).113 The vertically ordered MnMoO4 nanosheets, grown on NF, generate a large amount of 3D network channels, as illustrated in Fig. 6a–f. The cavities of the as-gained MnMoO4 nanostructures are convenient for the OH insertion and the electron diffusion. Additionally, the interconnected porous structure of the MnMoO4 nanosheets can store part of the electrolyte, which contributes to the improvement in the possibility of charge transfer at the electrode–electrolyte interfaces. The NF@MnMoO4 electrode has a specific capacitance of 4609 F g−1 at 1.0 A g−1 and retained 92.4% capacitance over 20[thin space (1/6-em)]000 cycles in 3 M KOH electrolyte (Fig. 6g–j). The electrochemical properties of the α-MnMoO4 materials in situ grown on the conductive substrates are revealed to be much better compared with the materials without substrates. This is because the conductive metal substrates can effectively avoid the agglomeration of MnMoO4 micro/nanoscale particles, and prevent “dead volume” caused by the polymer binder in electrode sheets.
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Fig. 6 (a–c) SEM images of the NF@MnMoO4 nanosheet arrays at different magnifications. (d–e) Transmission electron microscopy (TEM) images of the NF@MnMoO4 nanosheet arrays. (f) High-resolution transmission electron microscopy (HRTEM) image of a single MnMoO4 nanosheet. (g) Cyclic voltametric (CV) curves of the NF@MnMoO4 nanosheet electrode at different scan rates. (h) Galvanostatic charge–discharge (GCD) curves of the NF@MnMoO4 nanosheet electrode. (i) Specific capacitances of the NF@MnMoO4 electrodes for various reaction conditions at different current densities. (j) Cycling retention of the NF@MnMoO4 electrode at a constant scan rate of 100 mV s−1.113 Copyright 2020, American Chemical Society.
3.2.3 Designing composites with transition-metal oxides. Recently, the 3D multi-component core–shell arrays with large specific surface areas, high porosity and numerous active sites have been extensively researched for supercapacitors.114 The core part can afford an efficient transfer path to ions or electrons, and maintains sufficient stability during the electrochemical reactions. Meanwhile, the shell part possesses a larger specific surface area and furnishes more active sites in electrochemical reactions. The combination of MnMoO4 and transition-metal oxide to form 3D heterostructures is beneficial to improve the specific capacitance and redox reversibility of composites. To date, 3D core–shell nanocomposites have been demonstrated to significantly improve the low specific capacity of MnMoO4.115 For example, Yuan et al. prepared a 3D NiCo2O4@MnMoO4 core–shell nanocolumn via a two-step hydrothermal route.116 The NiCo2O4@MnMoO4 hybrid electrode has a high specific capacitance of 1169 F g−1 at 2.5 mA cm−2, as well as a good reversibility with cycling efficiency of 92.58% after 5000 cycles at 30 mA cm−2. Lv et al. created the MnCo2O4@MnMoO4 core–shell nanoarrays through a facile hydrothermal reaction,117 and the MnCo2O4 nanosheets were grown on nickel foam to serve as the core, while MnMoO4 nanosheets served as the shell. The MnCo2O4@MnMoO4 electrode delivers a specific capacity of 885 C g−1 at a current density of 3.0 A g−1 and remarkable reversible capacity with 95% retention over 5000 cycles at 10.0 A g−1. More recently, Arvind Singh et al. synthesized porous NiCo2O4@MnMoO4 heterostructures via a simple hydrothermal route (Fig. 7a and b).118 The as-obtained NiCo2O4@MnMoO4 electrode exhibits superior electrochemical performance, specifically a high specific capacitance of 1821 F g−1 at 5.0 A g−1, and an outstanding cycling stability of ∼94% retained after 5000 cycles at 70.0 A g−1 (Fig. 7c–e). Furthermore, the NiCo2O4@MnMoO4 electrode shows better specific capacitance compared to those of pure NiCo2O4 and pure MnMoO4 at various current densities (Fig. 7f). The choice of two-phase particles plays a decisive role in the construction of innovative 3D MnMoO4 multi-component heterostructures electrode materials.
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Fig. 7 (a and b) Field emission scanning electron microscopy (FE-SEM) images of the NiCo2O4@MnMoO4 heterostructures. (c) CV curves of the NiCo2O4@MnMoO4 electrode at various scan rates. (d) GCD curves of the NiCo2O4@MnMoO4 heterostructures at different current densities. (e) The stability profile of the NiCo2O4@MnMoO4 electrodes at 70.0 A g−1. (f) Specific capacitances of MnMoO4, NiCo2O4 and NiCo2O4@MnMoO4 electrodes at typical current densities.118 Copyright 2020, Elsevier.
3.2.4 Forming composites with other conductive materials. Apart from the transition-metal oxides, diverse conductive materials were applied to modify the microstructures of MnMoO4 to enhance the ion transparent properties, such as sulfides,115,119 graphene120–122 and conducting polymers.123,124 Wei et al. fabricated hierarchical NiCo2S4@MnMoO4 core–shell composites via a three-steps hydrothermal route.115 The MnMoO4 nanosheets with a thickness of 0.5 μm controllably attached to the NiCo2S4 nanotubes with a diameter of ∼100 nm. The specific capacitance of this NiCo2S4@MnMoO4 hybrid electrode is calculated to be 1186.44 F g−1 at 1.0 A g−1, and maintains 90.1% of the initial capacitance after 5000 cycles at 10.0 A g−1. Furthermore, Li et al. developed a novel core–shell CoS/MnMoO4/rGO/NF nanocomposite with a complicated network structure through hydrothermal treatment, followed by electrodeposition routes, as shown in Fig. 8a.119 When the loading amount of CoS is 0.4 mg cm−2, the corresponding CoS-0.4/MnMoO4/rGO/NF electrode with the thickness of 30 nm shows that CoS-0.4/MnMoO4 is tightly bound to rGO/NF. In particular, the CoS shell is evenly wrapped on the MnMoO4 core (Fig. 8b–d). As illustrated in Fig. 8e–h, the as-prepared CoS-0.4/MnMoO4/rGO/NF electrode displays a significant specific capacitance of 3074.5 F g−1 at 1.0 A g−1 and the capacitance retention of 87% over 5000 cycles at a constant current density of 10.0 A g−1. These nice electrochemical properties can be ascribed to the appropriate proportion of active substance, as well as the orderly unique microstructure.
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Fig. 8 The characterizations of the CoS-0.4/MnMoO4/rGO/NF nanocomposites: (a) The schematic illustration of the synthesis approach for the composite. (b and c) SEM images. (d) TEM images. (e) CV curves at different scan rates. (f) GCD curves. (g) The real capacitance and specific capacitance at various current densities. (h) Cycle performances of parallel samples at 10 A g−1.119 Copyright 2019, Elsevier.

3.3 Reaction mechanisms for MnMoO4 in the supercapacitor

The charge storage mechanisms of the MnMoO4 electrodes in different electrolytes have a vital influence on the pseudo-capacitive properties.125–127 The Faradaic redox reactions and electron transference numbers of MnMoO4 in aqueous electrolytes, including alkaline, neutral, and acidic solutions, are described in Table 1. In alkaline electrolytes, a plausible mechanism is the fully reversible redox reactions on the surface of the MnMoO4 electrodes corresponding to the pseudocapacitive capability and the adsorption/desorption of OH in the electrochemical double layer.98,128 At the beginning, Mn2+ undergoes an oxidation process (losing one electron) to form Mn3+ (Mn2O3), which matches eqn (1).92,119,129 Later, Mn2O3 further reacts with OH to generate MnO2 with increasing electrode potentials, manifesting the occurrence of the electron transfer of Mn3+/Mn4+ (eqn (2)).113,115 Meanwhile, the presence of Mo can raise the electronic conductivity of the MnMoO4 electrodes (MnMoO4: 4.27 × 10−3 S cm−1vs. MnO2: 10−5–10−6 S cm−1),110,130,131 and then furnish the fundamental of decreasing the internal resistances to enhance the rate capability and cycling stability of MnMoO4. During the charge and discharge, the molybdate species exist as MoO42− in alkaline solution,132,133 in which every Mo atom in the tetrahedral MoO42− is surrounded by four O atoms. Each Mo–O bond processes a high binding energy of 540 kJ mol−1;134,135 thus, the Mo element does not take part directly in the redox reaction. For instance, the electrochemical processes of the MnMoO4@MWCNT electrode, reported by Jai Bhagwan et al., equal the following eqn (1) and (2) having the charge transfer kinetics of Mn2+/Mn3+ and Mn3+/Mn4+, achieving a specific capacitance of 1017 F g−1 at 1.0 A g−1 and an energy density of 18.1 W h kg−1 at a power density of 362.4 W kg−1 using 1 M KOH electrolyte.128
Table 1 The reaction mechanisms of MnMoO4 electrodes in three typical aqueous electrolytes
Type of electrolytes Faradaic redox reactions Ref.
Alkalinity 2[Mn(OH)3] ↔ Mn2O3 + 3H2O + 2e (1) 98, 113, 115 and 128
Mn2O3 + 2OH ↔ 2MnO2 + H2O + 2e (2)
Neutrality MnMoO4 + M+ + e ↔ MMnMoO4 (3) 122
Acidity Mechanism 1: 136–139
Mo(VI)O42− + 2H+ ↔ H2Mo(VI)O4 (4)
H2Mo(VI)O4 + 2e + 2H+ ↔ H2Mo(IV)O3 + H2O (5)
H2Mo(VI)O4 + e + H+ ↔ HMo(V)O3 + H2O (6)
Mechanism 2: 44
MnxMo1−xO4 + yH+ + ye ↔ HyMnxMo1−xO4 (7)


For the neutral electrolyte (e.g., Na2SO4, KCl, etc.), the redox process of the Faradaic reaction at the MnMoO4 electrodes is changed from MnMoO4 to MMnMoO4 (eqn (3)), which is accompanied by the embedding and disembedding of the electrolyte cationic M+ (e.g., Na+, K+, etc.). Debasis Ghosh and his colleagues reported that the Faradaic reactions at the hexahedron-shaped α-MnMoO4 electrodes in 1 M Na2SO4 electrolyte can be expressed as an equation: MnMoO4+ Na+ + e ↔ NaMnMoO4, which made a high pseudocapacitance contribution (267 F g−1 at 5 mV s−1) since the Na+ was involved in the redox processes.122

Distinct from the alkaline and neutral electrolyte, the effects of the acidic electrolyte for the performances of MnMoO4 have been discussed in a few literature, which entails more systematic research. It was reported that MnMoO4 abides by two possible reaction mechanisms in the acid solutions: (1) The molybdate species (MoO42−) tend to form polymeric ions of H2MoO4 (eqn (4)). H2MoO4 can be further transformed to H2Mo(IV)O3 and HMo(V)O3 through the redox reaction between the redox pairs Mo(VI)/Mo(V) and Mo(VI)/Mo(IV), which is shown in eqn (5) and (6).136–139 (2) The Faradaic reaction gets and releases electrons among MnxMo1−xO4 and HyMnxMo1−xO4, and is directly correlated to the insertion/extraction of H+ ions (eqn (7)). For example, Purushothaman et al. proposed that the possible redox reaction of α-MnMoO4 nanorods in 0.06 M H2SO4, HCl or para toluene sulfonic acid (p-TSA) can be expressed in eqn (7): MnxMo1−xO4 + yH+ + ye ↔ HyMnxMo1−xO4. They also found that the specific capacitance of α-MnMoO4 nanorods in 0.06 M H2SO4 electrolyte was 998 F g−1 at 5 mV s−1, which displayed a superior capacitive behavior compared to that of p-TSA (784 F g−1) and HCl (530 F g−1) acid solutions.44 In conclusion, the reaction mechanisms of the MnMoO4 electrodes can be strongly determined by the pH of the electrolytes, and the electrochemical properties in these as-mentioned systems are summarized in the following sequence: alkalinity > acidity > neutrality.

According to the above reports on the reaction mechanisms of the MnMoO4 electrodes for a supercapacitor, a deeper understanding of the complex electrochemical behaviors under different acidic and alkaline electrolytes and dynamics attributed by MnMoO4-based materials is the key to a major breakthrough.140–142 Therefore, the introduction of in situ analysis techniques, such as in situ X-ray diffraction (XRD), in situ Raman, in situ X-ray absorption spectroscopy (XAS) and in situ X-ray photoelectron spectroscopy (XPS) can track the redox process in real-time during cycling, and directly reveal the intermediate phase structures and the valence changes of Mn and Mo, resulting in an enhanced specific capacitance.143–145 The combination of in situ TEM and in situ SEM roundly demonstrates the morphological changes of the MnMoO4-based electrodes during the operation of supercapacitors, including volume expansion and crack formation, which suggests that regulating the growth parameters of MnMoO4-based electrodes will be beneficial to improve its cycling stability.146,147 These advanced in situ characterization approaches have an important effect on monitoring the microstructural evolution of the MnMoO4-based materials during the charge and discharge process, providing guidance for the reasonable design of electrode materials and electrolyte, which can accelerate the large-scale practical application of supercapacitors.

For a recent comprehensive comparison, the synthetic routes and corresponding electrochemical performances of MnMoO4-based electrodes are summarized in Table 2. A rationally designed microstructure with specific features is the premise of its superior electrochemical behaviors.148–157 The great specific surface area and the regular morphology of the MnMoO4 micro/nano particles can effectively accelerate the diffusion rate of the ion/electron, and promote the reaction kinetics, thereby improving its electronic conductivity and specific capacitance. Besides, both conductive materials and MnMoO4 materials show enhanced specific capacitance among the conductive material/MnMoO4 composites. MnMoO4 composites are promising electrode materials for supercapacitors.

Table 2 Summary on the electrochemical properties of manganese molybdate and its composites in supercapacitors
Type of electrolyte Material Synthesis method Electrolyte Specific capacitance Rate capability Cyclic stability Energy density Power density Ref.
Alkalinity MnMoO4@MWCNT Hydrothermal reaction 1 M KOH 1017 F g−1 at 1.0 A g−1 18.1 W h kg−1 362.4 W kg−1 128
MnMoO4·0.9H2O nanorods Precipitation 1 M KOH 215 F g−1 at 1 mA cm−2 76
MnMoO4 nanorods Microwave-assisted method 1 M KOH 836 F g−1 at 5 mV s−1 100 F g−1 at 15 A g−1 84% after 3000 cycles (100 mV s−1) 63
Tube-like MnMoO4 Single-spinneret electrospinning technique 2 M KOH 620 F g−1 at 1.0 A g−1 460 F g−1 at 60 A g−1 91% after 10[thin space (1/6-em)]000 cycles (1.0 A g−1) 31.7 W h kg−1 797 W kg−1 26
α-MnMoO4 nanorods Microwave-assisted method 2 M KOH 446.7 F g−1 at 1 mA cm−2 125.4 F g−1 at 10 mA cm−2 81.12% after 3000 cycles (8 mA cm−2) 67
α-MnMoO4 3D fan-like nanostructures Precipitation 2 M KOH 562 F g−1 at 1.0 A g−1 218 F g−1 at 10.0 A g−1 99.8% after 1000 cycles (1.0 A g−1) 112
MnMoO4 nanorods Solvothermal method 2 M KOH 697.4 F g−1 at 0.5 A g−1 237.4 F g−1 at 10.0 A g−1 84% after 500 cycles (5.0 A g−1) 81
CoS-0.4/MnMoO4/rGO/NF Hydrothermal and electrodeposition methods 2 M KOH 3074.5 F g−1 at 1.0 A g−1 2236.5 F g−1 at 10.0 A g−1 87% after 5000 cycles (10.0 A g−1) 50.3 W h kg−1 415.8 W kg−1 119
Ni3S2@MnMoO4 Hydrothermal reaction 2 M KOH 979.3 C g−1 at 2 mA cm−2 690.0 C g−1 at 30 mA cm−2 88.3% after 7000 cycles (10 mA cm−2) 31.4 W h kg−1 399.9 W kg−1 148
MnMoO4·H2O@MnO2 Hydrothermal reaction 2 M KOH 3560.2 F g−1 at 1.0 A g−1 84.1% after 10[thin space (1/6-em)]000 cycles (5.0 A g−1) 45.6 W h kg−1 507.3 W kg−1 149
NiCo2O4@MnMoO4 Hydrothermal reaction 2 M KOH 1705.3 F g−1 at 5 mA cm−2 1252.6 F g−1 at 20 mA cm−2 92.6% after 5000 cycles (5 mA cm−2) 150
MnMoO4/NiWO4 Hydrothermal reaction 2 M KOH 598 F g−1 at 1.0 A g−1 422 F g−1 at 20 A g−1 82% after 5000 cycles (1.0 A g−1) 103
Rod-like MnMoO4 Precipitation 2 M KOH 112.8 C g−1 at 0.5 A g−1 58.8 C g−1 at 8.0 A g−1 109 C g−1 after 2000 cycles (1.0 A g−1) 100
NiCo2O4@MnMoO4 Hydrothermal reaction 3 M KOH 1169 F g−1 at 2.5 mA cm−2 92.58% after 5000 cycles (30 mA cm−2) 15 W h kg−1 6734 W kg−1 116
Co3O4@MnMoO4 Hydrothermal reaction 3 M KOH 663.75 F g−1 at 2.5 mA cm−2 399 F g−1 at 15 mA cm−2 95.32% after 3000 cycles (3.0 A g−1) 12.03 W h kg−1 300 W kg−1 39
NiCo2S4@MnMoO4 Hydrothermal reaction 3 M KOH 1186.44 F g−1 at 1.0 A g−1 820 F g−1 at 15 A g−1 90.1% after 5000 cycles (10.0 A g−1) 47.8 W h kg−1 699.9 W kg−1 115
NF@MnMoO4 Hydrothermal reaction 3 M KOH 4609 F g−1 at 1.0 A g−1 2800 F g−1 at 20 A g−1 92.4% after 20[thin space (1/6-em)]000 cycles (100 mV s−1) 107.38 W h kg−1 801.34 W kg−1 113
NiCo2O4@MnMoO4 Hydrothermal reaction 3 M KOH 1118 F g−1 at 1.0 A g−1 746 F g−1 at 10.0 A g−1 87.85% after 5000 cycles (1.0 A g−1) 236.44 W h kg−1 699.99 W kg−1 104
NiCo2O4@MnMoO4 Hydrothermal reaction 6 M KOH 1821 F g−1 at 5.0 A g−1 1265 F g−1 at 60 A g−1 94% after 5000 cycles (70 A g−1) 91.87 W h kg−1 374.15 W kg−1 118
MnCo2O4@MnMoO4 Hydrothermal reaction 6 M KOH 885 C g−1 at 3.0 A g−1 629 C g−1 at 30 A g−1 95% after 5000 cycles (10.0 A g−1) 49.4 W h kg−1 815 W kg−1 117
CuCo2O4@MnMoO4 Hydrothermal reaction 6 M KOH 1327.5 F g−1 at 1.0 A g−1 1055.3 F g−1 at 20 A g−1 92.8% after 6000 cycles (5 A g−1) 58.9 W h kg−1 670 W kg−1 151
NiCo2O4@MnMoO4 Hydrothermal reaction 6 M KOH 2603.9 F g−1 at 5 mA cm−2 92.1% after 3000 cycles (5 mA cm−2) 44.16 W h kg−1 800 W kg−1 152
MnMoO4·nH2O Hydrothermal reaction 1 M NaOH 1271 F g−1 at 5 mV s−1 619 F g−1 at 100 mV s−1 84.5% after 2000 cycles (10 A g−1) 31.6 W h kg−1 935 W kg−1 101
MnMoO4·4H2O Hydrothermal reaction 1 M NaOH 2300 F g−1 at 4 mA cm−2 1260 F g−1 at 24 mA cm−2 92% after 3000 cycles (5 mV s−1) 105
α-MnMoO4 nanorods Microwave hydrothermal method 2 M NaOH 551 F g−1 at 1.0 A g−1 253 F g−1 at 5.0 A g−1 89% after 1000 cycles (5.0 A g−1) 69
MnMoO4/MnCO3 Hydrothermal reaction 2 M NaOH 1311.1 F g−1 at 1.0 A g−1 400 F g−1 at 10.0 A g−1 79% after 5000 cycles (10.0 A g−1) 26.5 W h kg−1 657 W kg−1 153
MnMoO4 nanorods Solid-state chemistry reaction 2 M NaOH 210.2 F g−1 at 1.0 A g−1 112.6% after 10[thin space (1/6-em)]000 cycles (5.0 A g−1) 23.5 W h kg−1 187.4 W kg−1 154
MnMoO4/CoMoO4 Simple refluxing method 2 M NaOH 187.1 F g−1 at 1.0 A g−1 134.7 F g−1 at 3.0 A g−1 98% after 1000 cycles (3.0 A g−1) 98
CNT/rGO/MnMoO4 Hydrothermal reaction 2 M NaOH 2374.9 F g−1 at 2 mV s−1 703.9 F g−1 at 100 mV s−1 97.1% after 3000 cycles (2 mV s−1) 59.4 W h kg−1 1367.9 W kg−1 121
Rhombohedron-like α-MnMoO4 Precipitation 2 M NaOH 200 F g−1 at 1.6 A g−1 84 F g−1 at 6.4 A g−1 91% after 1000 cycles (1 mA cm−2) 11 W h kg−1 100 W kg−1 92
α-MnMoO4 nanorods Sonochemical method 2 M NaOH 168.32 F g−1 at 0.5 mA cm−2 96% after 2000 cycles (100 mV s−1) 9.87 W h kg−1 95.58 W kg−1 155
Neutrality MnMoO4/G Hydrothermal reaction 1 M Na2SO4 142.08 F g−1 at 0.7 A g−1 129.1 F g−1 at 1.0 A g−1 93.7% after 1000 cycles (0.7 A g−1) 41.9 W h kg−1 208 W kg−1 120
α-MnMoO4/PANI Sonochemical method 1 M Na2SO4 396 F g−1 at 5 mV s−1 321 F g−1 after 500 cycles (5 mV s−1) 124
MnMoO4/graphene Hydrothermal reaction 1 M Na2SO4 364 F g−1 at 2.0 A g−1 287 at 8.0 A g−1 88% after 1000 cycles (8.0 A g−1) 202.2 W h kg−1 2000 W kg−1 122
PEG-MnMoO4 Precipitation 1 M Na2SO4 424 F g−1 at 1.0 A g−1 138 F g−1 at 5.0 A g−1 93
PPy@MnMoO4 In situ oxidative polymerization 2 M KCl 374.8 F g−1 at 0.2 A g−1 208.5 F g−1 at 5.0 A g−1 80.6% after 1000 cycles (5.0 A g−1) 34.4 W h kg−1 500 W kg−1 123
Acidity PPy@MnMoO4/CFs Double in situ deposition method 0.6 M H2SO4 440.1 F g−1 at 0.2 A g−1 143.4 F g−1 at 4.0 A g−1 83% after 1000 cycles (2.0 A g−1) 156
α-MnMoO4 nanorods Sol–gel spin coating method 0.06 M H2SO4 998 F g−1 at 5 mV s−1 449 F g−1 at 15 mV s−1 44
0.06 M para toluene sulfonic acid 784 at 5 mV s−1 527 F g−1 at 15 mV s−1
0.06 M HCl 530 at 5 mV s−1 294 F g−1 at 15 mV s−1


Conclusions

In summary, MnMoO4 and its composite materials have been widely studied as promising electrodes for advanced supercapacitors. The crystal structure, preparation methods, advantages and energy storage mechanisms of MnMoO4 have been discussed in detail, especially its current progress. Although the development of MnMoO4 electrodes has accessed some progress, several substantive issues about practical applications still pose a great challenge for us, which should be resolved toward its commercialization.

(1) All strategies for synthesizing micro/nanoscale MnMoO4 electrode materials revolve around the improvement of specific capacitance, rate performance and cycling durability, as well as synthetic controllability. Therefore, the key points to be studied are how to integrate the existing methods and obtain an architecture that is well-ordered, porous, ultra-tiny and more stable in high-rate charging/discharging.

(2) The microscopic morphology adjustment of MnMoO4, such as fabricating the 3D core–shell structure, in situ growth on conductive metal substrates, and composite formation with sulfides, graphene and polymers, can enhance the electrochemical properties of MnMoO4. Designing and fabricating novel Mn-based molybdates with high surface area, rich porosity, excellent specific capacitance and outstanding structural stability deserves considerable effort.

(3) During the electrochemical activities, the evolution and deformation of MnMoO4-based electrodes are not clear. Thus, there is a need for an in-depth analysis and profound revelation for the phase transformation and morphological changes of MnMoO4 composites via more accurate theoretical calculations and more detailed experimental data, which favors affording the basis for other related experimental characterization, such as in situ XRD, in situ XAS, in situ XPS, in situ SEM, and in situ TEM. The combination of theoretical calculations and experiments may open some new avenues to boost the characterizations of the MnMoO4 electrode.

(4) The current research studies on MnMoO4 electrodes for supercapacitors are mainly limited to the laboratory. However, the ultimate objective is to achieve the business application of MnMoO4 materials. Thus, more attention should be paid to the development of controllable routes for the large-scale synthesis of MnMoO4 with an optimum performance. It is expected that the MnMoO4-based electrodes will occupy an important position in the field of supercapacitors in the near future.

Author contributions

Zhu Zhu, Yan Sun, and Shulei Chou designed and wrote the review. Jiahao Zhu and Chunsheng Li revised the paper. Chen Yang and Miaomiao Wang drew the figures. Lin Li edited the mini-review. Didi Wang and Yuanliang Li discussed the structure of the paper.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

The authors gratefully acknowledge financial support from the National Natural Science Foundation of China (No. 51971182, 21203051, 21643005, and 21203135), the “Xingliao Talent Innovation Program” in Science and Technology of Liaoning Province, the Science and Technology Projects of Suzhou City (SYG201938 and SYG202025), and the Science and Technology Projects of Shanxi Province (S2022-JC-YB-0440). The work is also supported by the Australian Research Council through a Linkage Project (LP120200432).

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Footnote

Z. Zhu and C. Yang contributed equally to this work.

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