Next Article in Journal
A Micromechanical Analysis to the Viscoplastic Behavior of Sintered Silver Joints under Shear Loading
Next Article in Special Issue
Current Trends and Promising Electrode Materials in Micro-Supercapacitor Printing
Previous Article in Journal
Coefficients of Thermal Expansion in La3Ga5SiO14 and Ca3TaGa3Si2O14 Crystals
Previous Article in Special Issue
Triboelectric Energy-Harvesting Floor Tile
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Review

Recent Advances in Molybdenum Disulfide and Its Nanocomposites for Energy Applications: Challenges and Development

by
Kamal Batcha Mohamed Ismail
1,2,
Manoharan Arun Kumar
1,*,
Shanmugam Mahalingam
3,
Junghwan Kim
3 and
Raji Atchudan
4,5,*
1
Department of Electrical, Electronics and Communication Engineering, School of Technology, Gandhi Institute of Technology and Management (GITAM), Bengaluru 561203, Karnataka, India
2
Department of Electronics and Communication Engineering, Agni College of Technology, Chennai 600130, Tamil Nadu, India
3
Department of Materials System Engineering, Pukyong National University, Busan 48513, Republic of Korea
4
School of Chemical Engineering, Yeungnam University, Gyeongsan 38541, Republic of Korea
5
Department of Chemistry, Saveetha School of Engineering, Saveetha Institute of Medical and Technical Sciences, Chennai 602105, Tamil Nadu, India
*
Authors to whom correspondence should be addressed.
Materials 2023, 16(12), 4471; https://doi.org/10.3390/ma16124471
Submission received: 1 June 2023 / Revised: 13 June 2023 / Accepted: 16 June 2023 / Published: 19 June 2023
(This article belongs to the Special Issue Smart Materials and Devices for Energy Harvesting, Volume II)

Abstract

:
Energy storage and conversion are critical components of modern energy systems, enabling the integration of renewable energy sources and the optimization of energy use. These technologies play a key role in reducing greenhouse gas emissions and promoting sustainable development. Supercapacitors play a vital role in the development of energy storage systems due to their high power density, long life cycles, high stability, low manufacturing cost, fast charging-discharging capability and eco-friendly. Molybdenum disulfide (MoS2) has emerged as a promising material for supercapacitor electrodes due to its high surface area, excellent electrical conductivity, and good stability. Its unique layered structure also allows for efficient ion transport and storage, making it a potential candidate for high-performance energy storage devices. Additionally, research efforts have focused on improving synthesis methods and developing novel device architectures to enhance the performance of MoS2-based devices. This review article on MoS2 and MoS2-based nanocomposites provides a comprehensive overview of the recent advancements in the synthesis, properties, and applications of MoS2 and its nanocomposites in the field of supercapacitors. This article also highlights the challenges and future directions in this rapidly growing field.

Graphical Abstract

1. Introduction

The global energy requirement is continuously on the rise because of the burgeoning population, expanding urban areas, and the growth of industries. This has led to a greater need for renewable energy sources and energy-efficient technologies to meet the demand while reducing carbon emissions. Non-renewable resources such as coal, oil, and natural gas are categorized as fossil fuels that took millions of years to form from the decomposed remains of dead animals and plants. These fuels are major sources of energy for electricity generation, transportation, and industrial processes, but their use contributes to climate change and environmental degradation. Fossil fuels still dominate the global energy mix and account for the majority of energy production in the world [1,2,3]. In addition to being finite resources that will eventually run out, fossil fuels also contribute to air pollution and climate change through the release of greenhouse gases during combustion. These negative impacts have spurred a global shift towards renewable energy sources. The sustainable and environmental advantages of renewable energy sources like solar, wind, and hydropower are causing them to gain more popularity [4,5].
Renewable energy sources provide several advantages, including decreasing the amount of greenhouse gas emissions, enhancing the quality of air, and generating employment opportunities in the clean energy industry. Additionally, renewable energy is often more cost-effective and sustainable in the long term compared to traditional fossil fuels [6]. With the increasing shift towards renewable sources of energy, energy storage is gaining more importance. The intermittent nature of wind and solar power underlines the amplified requirement for energy storage to balance out the supply and demand of energy and ensure the reliable and consistent availability of power [7]. Insufficient energy storage is a major challenge for renewable energy sources, as they are dependent on weather conditions. Developing cost-effective and efficient energy storage technologies is crucial to overcoming this challenge and making renewable energy more reliable and accessible [8]. Energy storage devices are designed to accumulate extra energy during periods of low consumption and restore it during periods of high demand. This process helps maintain a balanced grid and prevent power outages. This technology is becoming increasingly important as more renewable energy sources are added to the grid, which can be intermittent and unpredictable [9].
There are three types of energy storage devices: mechanical, electrical, and chemical. Flywheels and compressed air energy storage fall under the category of mechanical storage systems, while batteries and supercapacitors are classified as electrical storage systems [10]. Both batteries and capacitors are energy storage devices, but their energy densities and discharge rates differ. Batteries have a higher energy density and slower discharge rate, while capacitors have a lower energy density and faster discharge rate [11]. Batteries store the charges electrochemically. This means that they use chemical reactions to produce and store electrical energy, which can then be used to power various devices and equipment. Additionally, different types of batteries have varying capacities and lifetimes, making them suitable for different applications [12]. Capacitors store charges electrostatically and are commonly used in electronic circuits to smooth out voltage fluctuations and filter out unwanted signals [13]. They come in various sizes and types, including ceramic [14], electrolytic [15], and tantalum capacitors [16].
Supercapacitors are high-capacity electrochemical devices that store and release energy quickly. They have the ability to store and deliver much higher energy densities than conventional capacitors due to their unique electrode configurations. Supercapacitors typically have larger capacitance values compared to traditional capacitors, and their charge/discharge cycles are much faster. There are three types of supercapacitors, which are categorized as electrostatic double-layer capacitors, pseudo-capacitors, and hybrid capacitors. Electrostatic double-layer capacitors are the most common type of supercapacitor. They operate by separating positive and negative charges over two layers of electrically conducting material separated by a thin separator. This separation creates a high-capacity electrical field, which stores charge. Pseudo-capacitors, on the other hand, work by storing charge on the surface of a conducting material through a process called faradaic charge transfer. This type of supercapacitor has a higher energy density than electrostatic double-layer capacitors but typically has a lower power density. Hybrid capacitors, as the name suggests, combine the features of both electrostatic double-layer capacitors and pseudo-capacitors. By doing so, they are able to offer not only high energy density but also high power density. This makes them ideal for high-performance applications which require both high energy and power density [17]. The use of supercapacitors has been on the rise recently as they possess the capacity to quickly store and distribute energy, making them a suitable option for electric vehicles and sustainable energy setups. As the world shifts towards more sustainable forms of energy, the demand for supercapacitors is expected to continue to grow [18]. Supercapacitors have several advantages over traditional batteries, including faster charging times, longer lifetimes, and higher power densities. They are also more environmentally friendly, as they do not contain toxic chemicals or heavy metals [19]. In the energy storage industry, a Ragone plot is frequently utilized to assess the viability of various technologies by illustrating the compromise between power density and energy density. It compares the appropriateness of different energy storage systems for different applications. This plot (Figure 1) is also employed to gauge the potential of new materials and technologies in the field of energy storage [20].

Transition Metal Dichalcogenides (TMDs)

Transition metal dichalcogenides (TMDs) are a group of 2D materials that are made up of a transition metal atom like molybdenum or tungsten sandwiched between two layers of chalcogen atoms, such as sulfur or selenium. They display distinctive features in terms of their electrical, optical, and mechanical characteristics, which make them highly potential materials for applications in electronics [21], bio-applications [22], topological spintronics [23], optoelectronics [24], energy storage [25], and energy conversion devices [26]. Over the years, researchers have successfully synthesized stable TMDCs using a variety of methods like chemical vapor deposition (CVD), chemical exfoliation, and solvothermal synthesis. The utilization of these techniques permits the accurate manipulation of the size, morphology, and structure of the TMDs, ultimately influencing their characteristic traits [27]. TMDs like MoS2, WS2, MoSe2, and WSe2 have been extensively studied because of their extraordinary electronic, optical, and mechanical characteristics that are prominently displayed when their thickness is decreased to just a few layers [28]. TMDs have a layered crystal structure, with strong covalent bonds within the layers and weak van der Waals forces between the layers. This leads to a favorable relationship between surface area and volume, resulting in optimal mechanical flexibility. TMDs also have a direct bandgap, which makes them efficient light absorbers and emitters [29,30].
The edge locations exhibit a significant concentration of atoms that are unsaturated, thereby offering a greater number of active sites for chemical reactions. Additionally, the coordination of the edge atoms is different from that of the basal atoms, resulting in a different electronic environment. This causes the edge sites to have a different electrochemical potential, making them more active in redox reactions [31]. The fabrications of electrodes using TMDs are often optimized to incorporate the edge-exposed surface of these materials, as opposed to their basal planes. This strategy can enhance both their catalytic and electrochemical properties. The edge sites of TMDs possess higher reactivity and greater activity towards electrochemical reactions compared to the basal plane sites [32,33]. In recent years, there has been a noteworthy rise in the studies conducted on two-dimensional TMDs, particularly MoS2, with a focus on their electrochemical properties [34]. Molybdenum disulfide (MoS2) displays enormous potential in diverse electrochemical applications such as batteries [35], hydrogen evolution [36], supercapacitors [37], and sensors [38]. The unique atomic structure of MoS2, which consists of a layered structure of molybdenum and sulfur atoms, provides it with exceptional electro catalytic properties. MoS2-based electrochemical devices have shown remarkable performance in terms of rapid charge/discharge rates, high energy density, and extended life cycles. Researchers are also exploring the use of MoS2 in hybrid energy storage systems [39], ionic-liquid-based supercapacitors [40], and as a catalyst for water splitting [41] and carbon dioxide reduction [42].
This article provides a general overview of the various 2D TMDs, focusing on their significant structure of MoS2. The mechanical, electrical, and optical properties of MoS2 and their impact on various applications are discussed in detail. Additionally, the paper systematically outlines the latest advancements in the methods used for their preparation and highlights their primary advantages and disadvantages. The main focus of this article is to explore the applications of MoS2 and its nanocomposites in energy storage and conversion techniques. In this study, we extensively evaluate the electrochemistry and capabilities of wearable and flexible supercapacitors based on MoS2, which have not been previously discussed in other review articles. Finally, we discussed the real-time challenges and the research gaps to improve the performance of MoS2 and its nanocomposites for potential applications in industries. The schematic representation of the overview of this review article is shown in Figure 2.

2. Structures, Properties and Synthesis of MoS2

2.1. Structure of MoS2

MoS2 is a unique material that exhibits different properties and applications depending on its structure and dimensions. The structure is composed of layers that are arranged in a hexagonal lattice made up of molybdenum atoms, with two sulfur atoms in between each layer. MoS2 has three polymorphic crystalline structures, which are 1T-MoS2, 2H-MoS2 and 3R-MoS2. 1T-MoS2 is the most thermodynamically stable polymorph of MoS2 at high temperatures. The Mo atoms are arranged in trigonal prismatic coordination, with a distorted octahedron formed by the six closest sulfur atoms. Its crystal structure is characterized by the existence of one type of sulfur atom in the lattice [43]. 2H-MoS2 is the most common form of MoS2 in nature. It has a hexagonal crystal structure, and each Mo atom is surrounded by six sulfur atoms forming a trigonal prism arrangement. Its unit cell consists of two different sulfur sites in the lattice [44]. 3R-MoS2 polymorph has a rhombohedral crystal structure (Figure 3) and is found at low temperatures. It has a lattice parameter that lies between the 1T and 2H structure and three different sulfur sites in the lattice [45].
One of the most common and stable phases of MoS2 is known as the 2H structure. This structure has a hexagonal lattice, which has two layers per unit cell. The adjacent layers are stacked in an ABA pattern, in which the middle layer is shifted slightly in relation to the top and bottom layers. This arrangement allows for strong interlayer interactions between the sulfur atoms, resulting in a stable crystalline structure [46]. The sulfur atoms from different atomic planes occupy the same positions relative to each other. The Mo-S bond in MoS2 is predominantly covalent in nature, meaning that the electrons are shared between the two atoms. This results in strong bonding between the Mo and S atoms within each sheet, contributing to the strong mechanical properties and thermal stability of the material. On the other hand, the layers of S atoms are coupled by van der Waals interactions, which are weaker and result from the temporary dipole moments that arise when the electron cloud around the atoms is slightly displaced [47]. The layered structure of MoS2 turns it into a perfect material for various applications, and its morphology can be controlled by different synthesis methods. MoS2 can be synthesized in various shapes and morphologies, including planar [48,49,50], nanoflowers [51], nanowires [52], nanotubes [53], nanoplatelets [54,55] and vertically aligned nanosheets [56]. Overall, the different structures of MoS2 offer a wide range of possibilities for scientific research and technological innovation.

2.2. Properties of MoS2

The properties of MoS2 play a crucial role in determining its suitability for energy storage applications. MoS2 possesses exceptional attributes, including high electrochemical activity, fast ion diffusion, and outstanding electrical conductivity, which make it a highly favored choice as an electrode in batteries and supercapacitors. The characteristics of MoS2 have a considerable impact on the utilization of energy storage in various applications, mainly because of its vast surface area that allows for a substantial active area for electrochemical reactions. Thus, the electrodes made of MoS2 possess a high capacitance and can conveniently accumulate a significant amount of charge, a crucial aspect for the superior functioning of energy storage devices. Another important property of MoS2 is its high mechanical strength and stability, which enables it to withstand repeated cycles of charge and discharge with minimal degradation. Additionally, MoS2 has good thermal stability and is capable of operating at high temperatures without compromising its performance, making it suitable for use in harsh environments. In addition, MoS2 has an electronic band structure that gives it a high electron affinity. This property makes it possible to achieve high energy storage density and excellent charge retention, which are essential for the development of high-performance energy storage devices [57,58,59].

2.2.1. Electronic Properties

The properties of multilayer MoS2 have been widely examined because of its impressive electronic and optical characteristics. Its band structure has been a focus of interest due to its potential use in optoelectronic devices. Studies have shown that multilayer MoS2 has an indirect band gap of 1.2 eV, indicating that the transfer of electrons from the valence to conduction bands necessitates a shift in momentum. However, the band gap increases as the number of layers in MoS2 decreases. MoS2 in a single-layer configuration, also known as monolayer MoS2, demonstrates a direct band gap measuring 1.8 eV. Moreover, the thickness-dependent band gap of MoS2 makes it possible to engineer its optical and electronic properties by controlling the number of layers and even stacking different materials on top of each other [60,61]. However, compared to silicon, which has a direct bandgap of 1.12 eV, MoS2 still falls short in terms of its ability to efficiently absorb and emit light in the visible spectrum [62]. The electronic characteristics of MoS2 can be significantly impacted by mechanical strain, which refers to the deformation caused by an applied force. Specifically, it can cause a change in the material’s band gap. For MoS2, this strain can shift its band gap from a direct one to an indirect one, thereby affecting its electronic properties in a significant way. Specifically, it can turn the material from a semiconductor into a metal, where there is no longer a band gap, and electrons can move freely across the material. This change in properties could have significant implications for the use of MoS2 in electronic devices, making it possible to tune its conductivity and optoelectronic properties through the application of strain. In addition to mechanical strain, other factors, such as electric fields and chemical doping, can also influence the electronic characteristics of MoS2 [63].
Monolayer MoS2 has become a noteworthy semiconductor material in recent times owing to its distinct characteristics. When this material is doped with chromium, copper, or scandium, it undergoes a transition to become an n-type semiconductor. On the other hand, doping with nickel or zinc causes monolayer MoS2 to become a p-type semiconductor. The ability to control the electrical properties of monolayer MoS2 through the process of doping opens up many potential applications in electronic devices. For example, n-type MoS2 can be used as a component in transistors, while p-type MoS2 can be used to create diodes [64]. The doping of Titanium in MoS2 can significantly alter its electronic properties, and the type of doping (interstitial or substitutional), as well as the doping concentration, play a crucial role in the resulting semiconductor behavior. Low levels of Ti doping lead to p-type behavior, while high levels result in n-type and, eventually, a ferromagnetic half-metal with spin polarization equal to one. These results may pave the way for the creation of advanced electronic gadgets that offer better performance and functionality [65].

2.2.2. Optical Properties

MoS2 is a semiconducting material that exhibits interesting optical properties. One of its notable characteristics is its absorption coefficient—a measure of how much light is absorbed as it passes through the material. The absorption coefficient of MoS2 was influenced by various factors, such as the chemical composition of the material, its thickness, and the wavelength of light being used. In the case of MoS2, its absorption coefficient is relatively large for wavelengths ranging from 400 nm to 500 nm [66]. The bandgap of bulk MoS2 changes when it is reduced to a few layers. This bandgap change in MoS2 enables the tunability of its photoresponsivity, specific detectivity, and response time. The photoresponsivity of MoS2-based devices is enhanced by the reduction in thickness due to quantum confinement effects. This confinement effect increases the electronic density of states in the bandgap, leading to an increase in light absorption and an increase in photoresponsivity. In addition to photoresponsivity, the specific detectivity of MoS2-based devices is improved by the increased surface area when reduced to a few layers, which improves the signal-to-noise ratio. The response time of MoS2-based devices is improved due to the reduction in thickness, which allows for faster carrier transport and recombination. Furthermore, the high mobility of charge carriers in MoS2 also contributes to its fast response time. Overall, the potential for MoS2 to be used in optoelectronics is very high due to its ability to have a tunable bandgap. This material has promising applications in photodetectors, solar cells, light-emitting diodes, and even optical switches and modulators [67].
The electronic and structural properties of MoS2 can be effectively assessed using its photoluminescence (PL) spectra. Any alterations in the material’s band gap, doping, or crystal structure can greatly impact its PL activity, making it a valuable tool for characterization. In pure MoS2, the band gap is estimated to be around 1.8 eV, resulting in an emission of around 670 nm. However, MoS2 can be doped with various elements, such as nitrogen or sulfur, which can alter the band structure and shift the emission peak. For example, nitrogen-doped MoS2 exhibits a blue-shifted PL peak due to a reduced band gap [68]. Moreover, the PL activity of MoS2 can also be affected by its structure. MoS2 can exist in different crystal forms, such as 1T or 2H, which have different electronic properties and, therefore, different PL activities. According to reports, the PL intensity of 1T-MoS2 is stronger as compared to 2H-MoS2 [69]. The addition of an H2O2 solution has been found to be an effective approach for enhancing the photoluminescence properties of monolayer MoS2. This is because H2O2 acts as a strong oxidizer that oxidizes the MoS2 surface without altering its crystalline structure [70]. Amani et al. attained an important improvement in the quality of MoS2 by using a chemical treatment of an organic super-acid, resulting in a quantum yield (QY) of 95%. This means that almost all of the absorbed energy is emitted as light, indicating a highly efficient process. It was noticed that the lifespan of MoS2 carriers is nearly 10.8 nanoseconds, making it a suitable material for utilization in advanced solar cells and high-performance lasers [71]. MoS2 exhibits exceptional electrical and optical characteristics, which make it a highly desirable substance for optoelectronic applications. However, the presence of defects has been a major obstacle to the realization of its full potential.

2.2.3. Mechanical Properties

The exclusive structure of Monolayer MoS2 contributes to its remarkable mechanical strength, which is similar to that of graphene, a two-dimensional material renowned for its exceptional strength. The Young’s modulus of a single layer of MoS2, which measures its stiffness and resistance to deformation, has been found to be 0.33 ± 0.07 TPa (terapascals). This is a remarkable value, particularly given that the Young’s modulus of steel, a material commonly used in construction, is only around 200 GPa (gigapascals). The lattice structure of MoS2 enables the material to withstand large amounts of stress without breaking or deforming [57]. One notable property of MoS2 is that it undergoes a transition from a bulk material to a two-dimensional (2D) material when its thickness is reduced to a single layer. This change is significant as the mechanical properties of MoS2 are affected: single-layered structures are more flexible than bulk materials. This is predominantly because of the interlayer interactions that exist in the bulk form of MoS2, resulting in a stiffer structure, whereas in the form of a single layer, the feeble van der Waals forces between layers enable increased flexibility [72].
One of the ways to alter the electronic characteristics of MoS2 is through mechanical strain. If mechanical stress is applied to MoS2, its band gap transforms from direct to indirect. This change in the band gap can result in new electronic and optical properties. Furthermore, when MoS2 is subjected to high strain values, it can undergo a structural deformation that can transform it from a semiconductor to a metal. This is because the deformation alters the Mo-S bonds and changes the electronic states of the material. Furthermore, the mechanical strain can also change the lattice symmetry, which influences the electronic properties of the material [73]. One of the significant differences between MoS2 monolayers and graphene is their thermal conductivity. MoS2 monolayers have a thermal conductivity of around 35 Wm−1 K−1, which is approximately 100 times lower than the thermal conductivity of graphene. This difference in thermal conductivity is attributed to the distinct atomic structure and electron configuration of the two materials. The lattice structure of graphene allows for the free flow of phonons, whereas MoS2 monolayers have a more complex lattice structure and exhibit phonon scattering [74].

2.3. Synthesis Methods of MoS2

MoS2 has emerged as a potential material for advanced portable electronic gadgets like sensors, transistors, and photovoltaic cells in the future. To achieve the desired material features and uses, there are several techniques for synthesizing MoS2 and related composites that are more significant. The synthesis of MoS2 and its nanocomposites involves top-down and bottom-up methods for fabrication are shown in Figure 4. Chemical vapor deposition (CVD), liquid-chemical exfoliation, hydrothermal synthesis, solvothermal synthesis, and mechanical exfoliation are among the popular methods used for synthesis. The synthesis methodologies for MoS2 and its related composites are varied and provide researchers with a range of options for producing high-quality materials for a wide range of applications [75,76,77,78].

2.3.1. Top-Down Approaches

In the top-down method, MoS2 bulk crystal is carefully processed to produce MoS2 nanomaterials, which are commercially available. This downsizing process involves physical manipulation of the crystal to produce smaller particles with dimensions at the nanometer scale. This method is widely used in nanotechnology and is preferred for its ability to produce uniform and well-defined nanomaterials [79,80,81]. MoS2 nanosheets can be readily produced through the exfoliation technique owing to their layered structure and van der Waals forces. There are several exfoliation methods available for synthesizing these nanosheets, such as mechanical, chemical, electrochemical, and liquid-phase exfoliation [82,83,84,85]. Even though the top-down methods are uncomplicated to utilize, they are not successful in producing irregularly shaped and very minute particles. The primary disadvantage of this approach is the challenge of acquiring the appropriate shape and size of particles.
(a)
Mechanical Exfoliation
The mechanical exfoliation technique involves the removal of appropriate MoS2 flakes from the bulk crystal of MoS2 through the use of adhesive tape and then transferring them onto a specific substrate [86,87]. As there is no chemical reaction involved in the mechanical exfoliation of MoS2 from its bulk crystal, there will be no alteration in its structure. The exfoliation process yields single- or few-layer MoS2 nanosheets with various shapes and sizes after removing the scotch tape, leaving some MoS2 residues on the substrate. These nanosheets possess excellent quality, making them ideal for investigating the original material’s properties and device performance. Nevertheless, the yield of production is not high in this process, and it is challenging to regulate the particle size of the resulting MoS2 nanosheet [86,88,89]. A study was conducted to investigate the interlayer interactions in heterostructures of transition metal dichalcogenides. The study was successful in creating MoS2/WS2 and MoSe2/WSe2 heterostructures using a mechanical transfer technique after exfoliating the relevant crystals [90]. The field of 2D materials has witnessed a major advancement with the creation of an automated approach for exfoliating transition metal dichalcogenides (TMDs) into single-layer or few-layer forms. The technique hinges on deploying controlled normal and shear forces to detach a thin sample from bulk MoS2 or MoTe2 with the help of a parallel plate rheometer. This detached sample is subsequently affixed to the rheometer’s movable upper fixture through the application of blue dicing tape. The process of creating atomically thin films of specific materials can be initiated through a step-and-repeat exfoliation process by utilizing preprogrammed contact force and liftoff speed. This method results in the consistent formation of such MoS2 films [91]. The mechanical exfoliation method is simple, inexpensive, and does not require any special equipment, making it a popular technique for synthesizing high-quality MoS2 nanosheets. It can be further optimized by controlling the pressure, speed, and direction of the peeling process to obtain larger and more uniform MoS2 nanosheets.
(b)
Ball Milling
Ball milling is a mechanical method that involves the use of high-energy ball mills to reduce the size of the precursor materials. The ball milling process has been shown to be a favorable technique for the large-scale production of MoS2 nanosheets, as it offers several advantages, such as homogeneity of the final product, low cost, and ease of operation. The procedure can be readily expanded for large-scale manufacturing as well. Additionally, ball milling can be used to produce MoS2 nanosheets with varying thicknesses by simply adjusting the milling time and speed [92,93,94]. Cantarella et al. investigated commercial MoS2 nanopowders subjected to ball-milling for 20 and 40 h has revealed that the process has significantly enhanced the adsorption properties of the nanopowders. The researchers found that MoS2 ball-milled for 40 h showed an exceptional capability to remove methylene blue dye from aqueous solutions. It was able to adsorb all the dye present in just 20 min. This indicates that the milling process led to a considerable increase in the adsorption capacity of the nanopowders [95]. Kumar et al. reported that the ball-milling process was used to treat bulk MoS2, resulting in an improvement in the capacitive properties of the material. Specifically, the treated BL-MoS2 showed an increase in specific capacitance and energy density, making it highly suitable for use as an active component in supercapacitors [96]. The ultrasonic ball milling technology was utilized for the synthesis of materials like h-BN, graphene, MoS2, WS2, and BCN. The iron balls used for milling in this study had diameters ranging from 1.0 to 1.5 mm. The outcome achieved was more than 20% in terms of yield. The resulting materials had sizes ranging from 1 to 20 µm and had a thickness of approximately 1–3 nm [97]. Overall, the ball milling process is an effective and efficient method for synthesizing MoS2, producing uniform and highly crystalline particles that have potential applications in various fields.
(c)
Liquid phase Exfoliation
A popular technique for generating nanosheets and colloidal dispersions involves the use of liquid phase exfoliation (LPE) on layered materials, such as MoS2. In this method, the bulk material is dispersed in a solvent to form a suspension and then subjected to high-intensity sonication to break down the layered structure and produce nanosheets. The new approach to producing 2H-MoS2 nanosheets, which involves synthesizing two to seven layers, presents several advantages. These advantages include simplicity, effectiveness, environmental friendliness, and absence of contamination. One of the unique aspects of this technique is that no surfactants are required, which can be a common drawback of other methods. Additionally, the use of acetone as a solvent is a notable improvement over NMP, which is commonly used but has low volatility. This technique utilizes solvents that have surface energies that match well with the solid interface, making the synthesis more efficient. By using extended sonication times and low concentrations of bulk powder, the layers are effectively peeled off, and the dispersions remain stable [98,99]. Chlorophyll extracts have been found to be a highly effective exfoliating agent for producing a thin layer of MoS2/WS2 heterostructure. This novel method of synthesis has opened the door to exciting possibilities in the field of renewable energy. The MoS2/WS2 heterostructure produced through this method has proven to be an effective catalyst for the production of hydrogen, which is a vital ingredient in a range of clean energy applications [100]. The study examined the electrocatalytic performance of 2H-MoS2 nanosheets produced through LPE in N-dimethyl formamide, 1-methyl-2-pyrrolidinone, and formamide by examining their surface and interface functionalization. The findings indicated that MoS2 nanosheets produced in formamide were comparatively smaller in size and thickness but showed significantly better electrocatalytic activity when compared to those produced in the other two solvents [101]. One of the biggest challenges in energy research is finding electrode materials for sodium-ion batteries that are inexpensive but can store a large amount of energy. Fortunately, a solution has been found in the form of MoS2 nanosheets that are exfoliated in the liquid phase and reinforced with 20 wt% single-wall carbon nanotubes (SWNTs). When shaped into sodium-ion battery electrodes, these materials have impressive gravimetric, volumetric, and areal capacities [102]. The implementation of a partial etching approach has been suggested to be a highly effective method for modifying the thickness and lateral dimensions of MoS2 nanosheets, resulting in an increased percentage of edges. This technique has been found to significantly improve the production rate of monolayer MoS2 (20%) and WS2 (12%) nanosheets through LPE [103].

2.3.2. Bottom-Up Approaches

The bottom-up approach is an effective method for synthesizing MoS2 and other 2D materials. The bottom-up approach involves the fabrication of a material from its constituent atoms or molecules. In the case of MoS2, it involves the synthesis of Mo and S atoms or molecules, followed by their assembly into the final material. The synthesis process is controlled at the atomic and molecular level, which allows for precise control over the particle size and structure of the resulting MoS2 nanocrystals. Bottom-up synthesis methods are highly scalable, making it possible to produce large amounts of MoS2 with fewer impurities and defects at a relatively low cost. It requires less energy and fewer processing steps than top-down methods, making them a more energy-efficient and environmentally friendly approach. There are various methods for producing MoS2, such as chemical vapor deposition (CVD) and wet chemical synthesis [104].
(a)
Chemical Vapor Deposition (CVD)
The preferred method for synthesizing MoS2 is chemical vapor deposition (CVD) because it can produce films with large surface areas that have high crystallinity and purity [105]. CVD involves the deposition of MoS2 from precursor molecules in the gas phase onto a substrate. It utilizes various methods, including the sulfurization of Mo-based films, thermolysis of S and Mo precursors, and vaporization and decomposition of precursors that contain Mo and S atoms to produce a high-quality film. The thickness of the film can be easily adjusted by varying the duration of the deposition process [106,107,108,109]. The sulfurization of Mo-based films involves the deposition of Mo films followed by the introduction of sulfur gas. The sulfur atoms react with the Mo atoms to form MoS2. According to Hong et al., the vapor deposition of sulfurization of MoO3 precursor involves three main steps: the adsorption of sulfur on the MoO3 surface, the formation of an intermediate sulfur compound, and the final conversion to an MoS2 monolayer. The availability of sulfur atoms plays a crucial role in determining the growth rate of the MoS2 layer, whereas the quantity of sulfur precursor utilized in the reaction can regulate the thickness of the resulting MoS2 layer [110,111]. The oxygen content in the resultant material, specifically MoOxSy, led to a significant decrease in sheet conductivity. It is important to carefully control the synthesis conditions to minimize the presence of oxygen and other impurities in the material to ensure optimal conductivity and performance [112,113,114].
Rovira et al. reported that the CVD process had successfully synthesized MoS2 nanoribbons, where MoO3 nanoribbons were used as a template. Two distinct morphologies of MoS2 ribbons were obtained by altering the positioning of the crucibles. The first morphology consisted of dense, compact MoS2 ribbons, whereas the second morphology comprised ribbons with “thorns” caused by incomplete sulfurization [115]. A new technique called single-step vapor-phase sulfurization has been developed to cultivate uninterrupted films of monolayer MoS2. In a study conducted by Chiawchan et al., the process was carried out using MoO2 as the source material. The outcome demonstrated a noticeable pattern on the substrate surface, suggesting changes in the concentration-gradient of the Mo-source material throughout the growth phase [116]. The growth of an ordered array of MoS2 nanodots with lateral sizes ranging from approximately 100–250 nm has been reported through a thermal chemical vapor deposition process. The process was conducted directly onto SiO2 substrates at a relatively low temperature range of 510–560 °C. The results indicate that this CVD method can facilitate the growth of high-quality MoS2 nanodot arrays [117]. The integration of the wet synthesis and chemical vapor deposition technique is beneficial for producing MoS2 films of superior quality. To create MoS2 using the liquid precursor, the process requires transforming a sample coated with a solution of L-cysteine and sodium molybdate while being exposed to an argon gas flow at a temperature of 680 °C. This process results in the direct conversion of the coating into an MoS2 film on the substrate [118]. Moreover, the transferring process of prepared films can be quite complicated and may require specialized equipment and expertise. Additionally, achieving uniformity and controllability in the film deposition process can also be a challenge, leading to variability in the quality and properties of the resulting films.
(b)
Physical Vapor Deposition
Molecular beam epitaxy (MBE) is a highly advanced technology that has the ability to produce thin films of single-crystal semiconductors. However, its application is limited to the manufacture of two-dimensional (2D) materials [119]. Conversely, physical vapor deposition is not commonly employed for 2D material synthesis. Ti and MoS2 materials were employed in the preparation of an MoS2/Ti composite using direct current magnetron sputtering. The PVD process is an effective method for growing MoS2 at significantly lower temperatures, as low as 350 °C, in this particular study [120]. MoS2 can be directly grown on thermally grown silicon oxide and (002) graphite. The technique is based on sputtering and can be easily implemented for growing other TMDs [121]. The electronic and optoelectronic properties of MoS2(1−x)Se2x monolayer alloys can be studied through their growth with different edge orientations, specifically the Mo-zigzag and S-Se-zigzag edge orientations. It is possible to obtain these edge orientations by controlling the deposition temperature. Moreover, the remarkably large domain size of MoS2(1−x)Se2x monolayer alloys (x = 0.41–1) can pave the way for the development of high-quality films on a large scale [122]. The study of the early stages of growth of very thin Pd, Au, and Ag films on a single layer of MoS2 has uncovered different patterns of growth that were identified via atomic force microscopy. In particular, Pd develops an even layer of contact, whereas Au clusters into small nanostructures, and Ag takes on a scattered formation of islands on the MoS2 surface [123].
(c)
Wet Chemical Synthesis
Wet chemical synthesis is a commonly employed and economical method for producing few-layered MoS2 and related nanocomposites. It involves mixing reagents in a specific order and under certain conditions to control the chemical reactions and the resulting product. The reaction can occur at different temperatures and pressures, and various factors such as pH, concentration, and stirring rate can also affect the final product [124,125]. The hydro/solvothermal method has gained popularity in the hybridization of MoS2 with other functional nanomaterials because of its simple procedure, convenient handling, and economical reaction method. Additionally, this method allows for the creation of unique morphologies in metal oxides, hydroxides, and sulfides [126,127]. The ammonium heptamolybdate, MoO3, sodium molybdate, etc., are used as precursors for molybdenum and thiourea, sulfur powder, thioacetamide, etc., are used as precursors for sulfur in the preparation of MoS2 powder. The hydrothermal/solvothermal methods were widely used for synthesizing a variety of MoS2 powder with different structures and properties [128,129,130,131]. The synthesis of MoS2 nanosheets and their subsequent aggregation into various morphologies, such as nanotubes, nanoflowers and microspheres etc., holds great potential for applications in diverse fields, including catalysis, energy storage, and bio-imaging [132,133,134].
Luo et al. demonstrated that the preparation conditions of wrapped nano-sheet greatly affect its adsorption capacity. Specifically, a wrapped nano-sheet with a 3:1 ratio of S and Mo, hydrothermally treated at 240 °C for 37 h, exhibited the highest adsorption capacity. The gradual evolution of morphology from coral-like aggregates to flower-like spheres to wrapped nano-sheet structures is significant as it enables the production of three distinct morphologies that can cater to varying demands in various fields [135]. The production of MoS2 nanosheets has been accomplished effectively through an uncomplicated and environmentally friendly hydrothermal technique that utilizes l-cysteine and ammonium molybdenum hydrate. During the synthesis process, l-cysteine can serve a dual purpose as a sulfur source and as a capping agent [136]. MoS2 nanosheets with different layer thicknesses (bilayer, trilayer, quadrilayer, and more) and a combination of MoS2 quantum dot-nanosheets were produced using a hydrothermal process by controlling the amount of MoS2 and NaOH. NaOH serves as an agent for intercalating, and the fragmentation of nanosheets results in the production of quantum dots [137]. The study conducted by Cordeiro et al. highlights the possibility of utilizing microwave-assisted hydrothermal synthesis to cultivate MoS2 nanostructures on cellulose paper substrates. This development presents potential applications in the fields of electronics and sensors. The researchers investigated the influence of synthesis parameters like temperature and time on the quantity of MoS2 grown on cellulose fibers. The evaluation identified the existence of both metallic and semiconductor phases of the nanostructures [138]. Xuan et al. investigated the effect of reaction temperature (160–220 °C) and reaction time (6–14 h) on the microstructure and morphology of MoS2. The outcomes showed that as the reaction heat increased from 160 to 220 °C, the morphology of MoS2 transformed gradually from aggregated particles to flower-like spheres to a nanosheet structure. In contrast, the reaction time affected the restacking and refinement of the MoS2 crystal structure but did not have a significant impact on the morphology [139]. Duraisamy et al. described a straight forward hydrothermal method for creating a 3D network of metallic MoS2/MoO3 nanosheets. The study found that the resulting nanosheets exhibit not only the desired metallic MoS2 phase but also a significant density of active sites and a tuned electrical conductivity that contribute strongly to their catalytic activity and hydrogen evolution reaction [140]. The comparison of advantages and disadvantages of various synthesis methods are listed in Table 1.

3. Energy Applications

MoS2 shows great potential for use in energy-related applications. However, further research and developments are necessary to address the scalability, stability, and cost-effectiveness challenges associated with its integration into the energy industry. We will categorize our conversation about energy applications into two primary domains, namely, the storage and conversion of energy. Ultimately, we will examine the challenges that MoS2 might encounter during its integration into the energy sector [141,142]. Various applications of MoS2 in energy storage and conversion fields are shown in Figure 5.

3.1. MoS2-Based Nanocomposites in Energy Applications

MoS2 composites have gained significant attention in recent years due to their unique properties that make them useful in energy applications. Here are some reasons why MoS2 composites are important in these applications:
  • Improved conductivity: MoS2 composites offer improved electrical conductivity compared to pure MoS2, making them ideal for use in batteries, fuel cells, and other energy storage and conversion devices;
  • Enhanced catalytic activity: MoS2 composites exhibit enhanced catalytic activity, which is useful in energy conversion processes like hydrogen evolution reaction (HER), oxygen reduction reaction (ORR), and carbon dioxide reduction reaction (CO2RR);
  • Increased stability: MoS2 composites are more stable than pure MoS2 and other transition metal dichalcogenides (TMDs) under extreme conditions, such as high temperatures and corrosive environments. This makes them suitable for use in harsh industrial and energy-related applications;
  • Reduced cost: MoS2 is a low-cost material, and its composites can be produced by simple, scalable processes, making them an economical option for energy applications.
In conclusion, MoS2 composites play a crucial role in energy production, storage, and conversion, making them highly useful in energy applications. With their exceptional properties, they have opened up new avenues for the development of highly efficient and sustainable energy technologies.

3.2. Energy Storage Applications

MoS2 is a potential material for energy storage applications due to its remarkable ability to store high amounts of energy and its extended lifespan. Its potential has been explored for its utilization in energy storage applications, specifically supercapacitors, sodium-ion batteries (SIBs) and lithium-ion batteries (LIBs). MoS2 nanosheets can also improve the overall performance of LIBs by improving their specific capacity and cycle life. MoS2 has displayed positive outcomes as a cathode material in SIBs concerning long cycle life and high energy density. Similarly, it has been observed that MoS2 carries a high surface area, excellent electrical conductivity, and exceptional electrochemical stability, making it an ideal electrode material for supercapacitors. Studies have revealed that MoS2-based supercapacitors exhibit better energy storage capacity than others, high power density, and long cycle life [143,144,145,146,147,148].

3.2.1. Li-Ion Batteries

MoS2 has become a popular material for lithium-ion batteries (LIBs) in recent times. This is because it possesses distinctive characteristics that can enhance the performance and durability of the batteries. MoS2 acts as an anode or cathode in Li-ion batteries. It has a high inherent capacity for storing lithium ions, the ability to prevent lithium-ion insertion/extraction during charge cycles, and stability over long-time cycling. It has been shown that by incorporating MoS2 as an electrode into Li-ion batteries, the battery life can be increased due to the superior charge/discharge properties and stability of the MoS2 material [149]. Liu et al. introduced a new MoS2/C hybrid electrode for use as a Li-ion battery anode. This electrode exhibits impressive low-temperature performance, maintaining a stable discharge capacity of up to 854.3 mAh g−1 at −20 °C, which is equivalent to 72.8% of its room-temperature performance. Despite operating at a current density of 3 A g−1, this electrode continues to exhibit a capacity of 140.9 mAh g−1. The increased spacing between MoS2 layers promotes rapid Li+ diffusion, ultimately enhancing the kinetics of lithiation/delithiation and improving the performance rate at low temperatures [150]. Baheri et al. developed an innovative method to produce 1T/2H-MoS2 nanocrystals within N-doped nanoporous carbon shown in Figure 6. This process involves using a pyrolysis method of sodium molybdate and potassium persulfate within an acrylonitrile-based polymer base. As a result, the C-MoS2 composite showed exceptional battery performance, with a specific capacitance of 556 mAh g−1 at a current density of 0.2 A g−1 and maintained excellent stability even after undergoing 100 cycles [151]. A recent study has shown that a 3D bulky MoS2@C/RGO composite may offer significant benefits for the cycling performance and rate capability of Li-ion batteries. The synthesized nanocomposite demonstrated a comparable cycling performance of 1189 mAh g−1 after undergoing 100 charge/discharge cycles at 200 mA g−1, which was better than the control samples and earlier reports [152]. The composite also showcased a good rate capability, with 1211 mAh g−1 at a current density of 50 mA g−1 and even 726 mAh g−1 at a current density of 2000 mA g−1. Moreover, when tested in an MoS2-PDA-GO30//LiCoO2 full-cell configuration, this composite material exhibited a superior cycling capability of 890 mAh g−1, which is equivalent to 1750 Wh kg−1. Despite the challenges, MoS2 remains a promising electrode material for LIBs, and research efforts are ongoing to address its cycle stability issues [153]. The widespread use of MoS2 electrodes in LIBs could potentially lead to the development of more efficient and longer-lasting batteries, with significant implications for various industries and applications. Bozheyev et al. investigated the use of MoS2 nanopowder as an anode material in LIBs. The nanopowder was produced through a solid-state synthesis method (SHS). The electrochemical performance of this nanopowder was evaluated through a coin-type CR2032 cell. According to the findings, MoS2-NP displayed an initial charging ability of 567 mAh g−1 when subjected to a current density of 50 mAh g−1. This indicates that MoS2-NP could be a promising contender for a proficient anode substance in LIBs [154]. The study on MoS2 phase transformation and the incorporation of CNT additives in batteries have showcased promising results in the application of metal sulfide electrodes in high-energy-density batteries [155].
The MoS2 composite electrodes were prepared by a method of uniaxial cold-pressing, which involved the pressing of the materials under a high pressure of 3 tons. The composite electrodes contained 60 wt% MoS2, 10 wt% carbon black, and 30 wt% β-Li3PS4 solid electrolyte. The solid electrolyte used in these electrodes was β-Li3PS4, which has high ionic conductivity and stability in air. Solid-state lithium-ion batteries were utilized to assess the efficiency of these electrodes, with a Li-In alloy serving as the counter electrode. During the discharge process at a rate of 67 mA g−1 (C-10) within the voltage range of 0.01–3.0 V, the electrodes displayed an initial specific capacity of approximately 439 mAh g−1. The specific capacity retention was also outstanding, with 312 mAh g−1 obtained after undergoing 500 cycles [156]. MoS2 and its composites have garnered increasing attention as potential electrode materials in the field of battery technology. One key advantage is their larger interlayer spacing, which enables fast metallic ion diffusion compared to other materials. This is particularly useful for ions like Na+, Zn2+, and Mg2+, which are commonly used beyond LIBs. Furthermore, the usual abundance of molybdenum and sulfur means that MoS2-based electrodes can be produced at a relatively low cost compared to other materials [157]. Cha et al. demonstrated that the incorporation of MoS2 in Li metal batteries can effectively mitigate the issues of dendrite formation and electrolyte decomposition, which are notorious for causing safety hazards and performance degradation. MoS2 can be used as a protective coating for Li metal anodes to improve their cyclic stability and avoid the formation of lithium dendrites. The use of MoS2 as a separator modification can also improve the battery’s performance by enhancing the wettability of the electrolyte and decreasing the impedance. Moreover, the solid electrolyte interphase formed between MoS2 and Li metal can serve as a stable interfacial layer, reducing the risk of side reactions between the electrolyte and Li metal [158].

3.2.2. Sodium-Ion Batteries

Molybdenum-based materials have shown remarkable electrochemical properties and stability, making them a favorable choice for anode materials in sodium-ion batteries (SIBs). These materials have been researched in several different forms, like nanoparticles, flakes, and membranes. They have demonstrated encouraging outcomes regarding their ability to maintain capacity and stability during cycles. One of the key advantages of molybdenum-based materials is their ability to interact with sodium ions through various mechanisms, including alloying, intercalation, and conversion reactions. The unique Na-insertion properties of molybdenum-based materials can be attributed to the open framework of their crystal structure, which can accommodate large sodium ions and allow for reversible and sustainable storage [159]. A combination of two distinct 1T and 2H phases has been utilized to produce a dual-phase MoS2 (DP-MoS2). This electrode has displayed exceptional cycling stability, with a reversible capacity of 300 mAh g−1 after undergoing 200 cycles, as well as excellent rate capability with a capacity of ~220 mAh g−1 at 2 A g−1. These findings indicate that DP-MoS2 has the capability to be utilized in commercial devices, offering a fresh strategy to create metal chalcogenides for applications in storing electrochemical energy [160]. A thorough analysis of MoS2 in comparison with MoO2 indicates that MoS2 has the ability to store sodium through the insertion reaction due to its larger interlayer distance compared to MoO2. Furthermore, the weaker bonds of MoS2, as compared to MoO2, make the conversion reaction of sodium with MoS2 more favorable [161]. The MoS2/grapheme/chitosan electrode has demonstrated superior performance as an anode material for SIBs. After undergoing 200 charge/discharge cycles at a current density of 100 mA g−1, the electrode exhibited a high capacity retention of 527.3 mAh g−1. It also displayed excellent rate capability and maintained a high capacity of 439.1 mAh g−1 at 1 A g−1. Importantly, the MoS2/G/C electrode exhibited exceptional stability over a long cycle life span, making it a favorable material for high-performance SIBs [162]. MoS2@CNTs composite material has been found to exhibit remarkable performance as an anode material for SIBs. This composite material demonstrates a high rate of performance and can deliver 508, 418, 359, 305, 258, and 183 mAh g−1 at current densities of 0.1, 0.2, 0.5, 1, 2, and 5 A g−1, respectively. The remarkable cycling stability of this composite material allows it to retain 360 mAh g−1 after undergoing 400 charge/discharge cycles at 0.5 A g−1. The outstanding ability of MoS2@CNTs is attributed to the strong combination of the MoS2 and CNT components, which makes it highly robust [163].
Ye et al. offer a different approach to enhancing the cycling performance of SIBs with respect to their reversible capacity. The remarkable performance of the Metal-semiconductor phase twinned hierarchical (MPTH) MoS2 electrode is ensured by expanding interlayers and preserving structural stability. It has been proven to deliver high reversible capacities of up to 200 mAh g−1 at a current density of 0.1 A g−1 for undergoing 200 cycles and an impressive 154 mAh g−1 at a current density of 1 A g−1 for undergoing 2450 cycles in the voltage range of 0.4–3.0 V. The electrode is capable of maintaining 6500 cycles when exposed to a current density of 2 A g−1, which results in 82.8% capacity retention from the second cycle. These findings exceed all previously recorded cycling performances of MoS2 by a significant margin [164]. A novel method for producing molecule-intercalated MoS2 with accurate interlayer spacing ranging from 0.62 to 1.24 nm has been suggested in a recent research study. This innovative technique allows for the fine-tuning of electrical conductivity, which ranges from 1.3 × 10−4 to 3.5 × 10−2 S cm−1, through incorporating guest molecules into MoS2. The synthesized MoS2 exhibits excellent sodium ion storage capacity, with the highest initial capacity of 465 mAh g−1 and retaining a capacity of 420 mAh g−1 after undergoing 600 charge/discharge cycles at a rate of 100 mA g−1. The better electronic conductivity and increased interlayer spacing collaborate to produce a synergistic impact that promotes the rapid movement of sodium ions and electrons. As a result, material usage is more efficient, and the outcomes are impressive [165]. Chothe et al. proposed a technique based on the solid-state method to generate ultrathin nanosheets of MoS2-graphene, which can be utilized in Na-ion batteries. During the galvanostatic study, the assembled Na-ion cell demonstrated a high specific capacity of 420 mAh g−1 at 50 mA g−1 and a capacity retention of 172 mAh g−1 at 200 mA g−1 after undergoing 200 cycles. This study highlights the potential of using hybrid materials in battery applications and demonstrates the importance of optimizing the electrode architecture for improved battery performance [166]. Halankar et al. developed an MoS2/C/CNT nanocomposite using a simple hydrothermal method shown in Figure 7. This composite material served as an electrode in SIB applications. The composite possesses excellent electronic conductivity and mechanical strength due to the presence of CNT, and at the same time, it effectively captures the polysulfide forms that occur during cycling. The full-cell SIB was developed using Na(Ni0.5Mn0.3Co0.2)O2 as a positive electrode and MoS2/C/CNT as a negative electrode. This battery demonstrated a specific capacitance of 96 mAh g−1 at a current density of 50 mA g−1 [167]. Researches on MoS2 in Na-ion batteries are still in its early stages, but there is potential for this material to show a significant role in the improvement of next-generation energy storage devices. Further investigation and optimization of the material’s properties and performance will be crucial for its successful integration into commercial Na-ion batteries.

3.2.3. Supercapacitors

MoS2 has a two-dimensional layered structure with remarkable electrochemical activity. This characteristic makes it an excellent option to serve as an electrode substance in supercapacitors, which require materials with high surface area and low resistance to store and release electrical energy quickly. Additionally, MoS2 has a high capacitance, which makes it an attractive option for supercapacitors, as increased capacitance typically leads to higher energy storage capacity.
(a)
1T and 2H MoS2 Electrodes for Supercapacitors
The surface functionalization of 1T MoS2 nanosheets with NH2Ph ring, through the chemical reaction with iodobenzene, leads to the formation of Fc-1T MoS2, which exhibits improved electrocatalytic performance as compared to 1TMoS2. By adding NH2Ph ring functionality and 1T MoS2 phase, the charge density and electronic properties are improved, resulting in faster charge transport and greater charge storage capacity. Fc-1T MoS2 displays a significant specific capacitance of 501 F g−1 at 1 A g−1 while maintaining 76.32% capacitance retention even after 2000 cycles. This is 2.6 times greater than the bare 1T MoS2 nanosheets [168]. The latest combination of ammonium ion intercalation molybdenum disulfide (A-MoS2) with a considerable 1T proportion exhibits great potential in augmenting the functioning of energy storage devices, such as supercapacitors and batteries. Its substantial specific capacitance of 228 F g−1 at 5 mV s−1 indicates that A-MoS2 possesses a remarkable charge-storing capacity. Additionally, A-MoS2’s retention capability is also noteworthy, retaining 127 F g−1 at 80 mV s−1, which is vital for real-world usage [169]. Zarach et al. demonstrate the potential of Pt@1T/2H-MoS2 electrode material for energy storage applications, as it shows significantly improved specific capacitance and consistent coulombic efficiency during multiple charging and discharging cycles. The surface modification with Pt shows a crucial role in enhancing the material’s electrochemical properties by promoting the exfoliation process [170]. Shrivastav et al. synthesized 2H-MoS2 using a hydrothermal method [171]. At a scanning rate of 10 mv s−1, 2H MoS2 demonstrated a specific capacitance of 115.42 F g−1, and at a current density of 0.5 A g−1, it showed a specific capacitance of 57.69 F g−1. The 2H MoS2 also exhibited an electrochemical double-layer capacitive behavior with partial pseudo-capacitance. The retention of 71.5% of specific capacitance after 5000 CV cycles indicates good cyclic stability of the samples.
(b)
MoS2 with Graphene and Carbon-Based Nanocomposites
MoS2 with graphene-based nanocomposites have been researched as electrode materials for supercapacitors owing to their exceptional electrical conductivity and high surface area [172]. Moreover, the addition of carbon-based materials like carbon nanotubes or carbon black can enhance the electrochemical activities of the composite, improving the overall performance of the supercapacitor [173,174]. Ramakrishnan et al. developed an MoS2@rGO nanocomposite through a hydrothermal synthesis followed by an ultra-sonication method. This composite has been shown to be a profound candidate for sodium ion symmetric hybrid SCs. The electrode material was examined in a half-cell formation using metallic sodium and exhibited a high specific capacity of 226 F g−1 at a current density of 0.03 A g−1. In a full-cell configuration, the electrode exhibited a high capacitance of 55 F g−1 at a current density of 0.03 A g−1 [175]. Zhan et al. developed high-performance hybrid supercapacitors (HSCs) based on an interlayer-expanded MoS2/rGO nanocomposite. The sodium hybrid supercapacitor (Na-HSC) outperforms the lithium hybrid supercapacitor (Li-HSC) when combined with N-doped hierarchically porous 3D graphene (N-3DG). It displays remarkable performance, achieving an energy density of 140 Wh kg−1 at a power density of 630 W kg−1 and an energy density of 43 Wh kg−1 at an extremely high power density of 103 kW kg−1 (with a charge completed within 1.5 s). Furthermore, even after over 10,000 cycles, there is no apparent reduction in capacity [176]. Ji et al. synthesized an MoS2-reduced graphene oxide (rGO) in a sandwich structure through a solvent-free and one-step ball-milling process. The resulting MoS2-rGO nanocomposite sample exhibited exceptional electrochemical performance when used as an electrode material for supercapacitors. The composite demonstrated a high specific capacitance of 306 F g−1 at a current density of 0.5 A g−1, which was higher than that of pure MoS2. Additionally, the composite exhibited minimal discharge capacity decay after 100 cycles in li-ion batteries (0.2 A g−1) and 5000 cycles in supercapacitors (4 A g−1), demonstrating its excellent potential for long-term energy storage devices [177]. Quan et al. discovered a novel nanostructure composed of hollow carbon–MoS2–carbon, which has been synthesized using an l-cysteine-assisted hydrothermal method. The hollow nanoplate morphology of the material provided a high specific surface area of 543 m2 g−1 and a total pore volume of 0.677 cm3 g−1, with fairly small mesopores at approximately 5.3 nm. These properties make the hollow carbon–MoS2–carbon nanoplates ideal for use in supercapacitors. When tested in a symmetric supercapacitor, the material exhibited a specific capacitance of 248 F g−1 (0.12 F cm−2) at a constant current density of 0.1 A g−1 [178]. The MoS2/CNT composite is a highly effective material for producing high-performance supercapacitors. At a current density of 1 A g−1, the MoS2/CNT composite has a specific capacitance of 402 F g−1. This is an impressive result that indicates high energy storage capacity. Moreover, the composite maintains 81.9% capacitance retention after 10,000 continuous charge/discharge cycles at the same high current density, indicating excellent cycling stability [179].
Mahajan et al. successfully developed a high-performance supercapacitor using biocarbon-based MoS2 nanoparticles synthesized from date fruits. By converting agricultural biowaste into an easily affordable energy resource via the pyrolysis technique, the team has developed a carbon-based nanocomposite that exhibits a high specific capacitance of 945 F g−1 at a current density of 0.5 A g−1. This biocompatible Bio-C/MoS2 nanocomposite displayed an impressive reproducing stability of 92% even after 10,000 charge/discharge cycles. Furthermore, the Bio-C/MoS2 nanosphere demonstrated an exceptionally high power density of 3800–8000 W kg−1 and an energy density of 74.9–157 Wh kg−1, making it a promising material for high-performance energy devices [180]. Zhang et al. reported the successful development of a new hierarchically porous MoS2/C composite aerogel using a simple one-pot mass preparation method. The composite aerogel displays a high specific capacitance of 712.6 F g−1 at 1 A g−1 and a capacity retention rate of 97.3% after 13,000 cycles at 6 A g−1 when tested as a supercapacitor electrode [181].
(c)
MoS2 with Metal Oxide/Sulfide-Based Nanocomposites
The electrochemical performance of MoS2 is restricted by its low surface area and porosity. To enhance its performance, nanocomposites can be produced using metal oxides or sulfides, which have high surface areas and better ionic conductivity. The use of nanocomposites combining MoS2 with metal oxides or sulfides shows significant promise for improving the performance of supercapacitors. The study conducted on CoNi2S4 and an MoS2 nanocomposite fixed on porous graphene oxide yielded promising results in their potential as a high-performance substrate. The spongy nanocomposite showed a remarkable specific capacitance of 3268 F g−1 in a 3 M KOH solution at 1 A g−1. Furthermore, the CoNi2S4@MoS2@rGO electrode displayed an impressive 93.6% stability of its initial capacity after 3000 consecutive charge/discharge cycles at a current density of 10 A g−1. Moreover, the energy density of 41 Wh kg−1 and power density of 700 W kg−1 demonstrate the potential for this electrode to operate effectively under high power needs, indicating its wide-ranging applicability in supercapacitor applications [182]. The Bi2S3/MoS2 nanohybrid, which has a flower-like structure and contains high-quality heterostructures and 3D aisles, boasts exceptional electrochemical capabilities. This includes a high specific capacitance of 1258 F g−1 at 30 A g−1 and outstanding cycle stability of 92.65% after 5000 cycles at 10 A g−1 [183]. The prepared SnS2/MoS2 layered heterojunction has shown remarkable promise in terms of supercapacitor properties when compared with the sole SnS2. The specific capacitance achieved was a noteworthy 466.6 F g−1 at a current density of 1 A g−1, indicating a significant improvement. Furthermore, the experiment demonstrated impressive cycling stability, with 88.2% capacitance retention at a current density of 4 A g−1. The as-fabricated symmetric supercapacitor displayed an energy density of 115 Wh kg−1 at a power density of 2230 Wh kg−1, which demonstrates its high energy storage capacity in high power demand situations [184]. Govindan et al. highlighted the exceptional properties of CeO2/C/MoS2 hybrid for charge storage applications. The hybrid exhibited an outstanding specific capacitance of 1325.67 F g−1. This value is significantly higher than that of CeO2/C (727.49 F g−1) or MoS2 (300.33 F g−1) alone. Furthermore, the cyclic stability of the hybrid was excellent, as it showed a capacitance retention of 92.8% after 1000 charging/discharging cycles. The asymmetric supercapacitor (ASC) showed a remarkable electrochemical performance with a high specific capacitance of 110.55 F g−1, excellent cyclic stability (even after 1000 cycles) and a high energy density of 34.55 Wh kg−1 at a power density of 666.7 W kg−1 [185].
The preparation of an MoS2/Fe2O3/G composite heterostructure material through the hydrothermal method has enabled the development of a highly efficient electrode material for supercapacitor devices. The unique combination of MoS2, Fe2O3, and graphene has resulted in a significant increase in capacitance, with a value of 98.2 mAh g−1 at 1 A g−1. Importantly, the ASC device incorporating the MoS2/Fe2O3/G composite electrode has shown remarkable energy and power density of 46.8 Wh kg−1 and 750 W kg−1, respectively. Moreover, the impressive performance of the device is retained over a prolonged duration of usage with excellent capacity retention of up to 77% even after 10,000 cycles [77]. MnS/MoS2/Ni-Inverse opal structure nanocomposites were synthesized using the electrochemical deposition (ECD) technique. These specimens demonstrated exceptional specific capacitance values of 1880 F g−1 at a charge current density of 5 A g−1. Furthermore, the samples were subjected to 2000 cycles of cycle life testing, and even after this rigorous testing, they retained a respectable capacitance value of 76.6% of their initial value [186]. Tue et al. proposed a novel method to produce NiCo2S4/MoS2 composite with different morphologies (like sheet and rod shape) using a simple solvothermal method shown in Figure 8. The composite electrode in sheet-like morphology (NCMS-L) demonstrated remarkable performance, including outstanding coulombic efficiency, elevated specific capacitance, exceptional energy density, and good cyclic stability. Specifically, the electrode presented a capacity of 2594 F g−1 at a current density of 0.8 A g−1 after undergoing 45,000 charge and discharge cycles. Additionally, the hybrid supercapacitor device comprising NCMS-L and activated carbon achieved an energy density of 31.9 Wh kg−1 [187].
(d)
MoS2 with Conducting polymer-based nanocomposites
In recent years, conducting polymers have gained increasing attention as electrode materials because of their numerous benefits. One of the most significant benefits of using conducting polymers is their low cost compared to traditional electrode materials such as metals. Additionally, conducting polymers possess high electrical conductivity, providing efficient transport of charge between the electrode/electrolyte interfaces. Chen et al. synthesized a hybrid electrode material, MoS2@PANI, by using a one-pot hydrothermal synthesis method. The resultant material had 25 wt% MoS2 and exhibited a high capacitance of 645 F g−1 at a current rate of 0.5 A g−1, which indicates maximum energy storage capacity. Additionally, this hybrid electrode material showed good cycling stability with a retention rate of 89% of its capacitance value after 2000 cycles at a current density of 10 A g−1 [188]. The CeO2/MoS2/PANI nanocomposite has demonstrated impressive electrochemical functionality, as evidenced by its specific capacitance values of 177 F g−1 at a scan rate of 5 mV s−1 and 62 F g−1 at a current density of 0.5 A g−1. This indicates its ability to store electrical charge efficiently. Additionally, the composite has exhibited excellent cyclic stability, with a capacitance retention rate of 98% after 2000 cycles at a current density of 5 A g−1, indicating its durability and long lifespan [189]. Ren et al. successfully developed MoS2/PANI nanocomposites with varying PANI loadings, using MoS2 nanosheets as the substrate. The composites with a 53 wt% PANI loading displayed the highest electro-capacitive property, resulting in exceptional electrochemical performance with a symmetric supercapacitor having an energy density of 35 Wh kg−1 and a power density of 335 W kg−1. Furthermore, the material demonstrated excellent cycling stability, showing 81% retention after 8000 cycles [190]. The preparation of a highly efficient MoS2/PANI/functionalized carbon cloth (MoS2/PANI/FCC) has been accomplished through a drop-casting method. This method allows for facile construction of the MoS2/PANI/FCC-based symmetric supercapacitor, which demonstrates a specific capacity of 72.8 F g−1 at 0.2 A g−1, based on the total mass of the two electrodes with a retention rate of 85% after 1000 cycles [191].
(e)
MoS2 based Flexible and wearable Supercapacitors
The emergence of wearable and flexible energy storage systems has revolutionized the field of wearable technology. These energy storage systems are designed to provide a reliable and sustainable source of power to wearable devices, including medical monitors, fitness trackers, and smartwatches. They are ultra-thin and flexible, which allows them to be integrated into the fabric of clothing or the band of a watch, making them easy to wear and practically invisible. The capability to deliver consistent and dependable power is a crucial factor for any wearable energy storage gadget. These devices must be able to store enough energy to last for an extended period, and they must also be capable of delivering a high current rate to meet the demands of different wearable devices. To achieve this level of performance, a variety of energy storage technologies are being researched, including batteries, supercapacitors, and hybrid systems that combine the best of both worlds [192,193,194]. Over the past few years, the wearable electronics industry has shown a remarkable interest in two-dimensional nanomaterials such as graphene, transition metal dichalcogenides (TMDs), and black phosphorus. This is because they possess distinctive features and benefits when compared to conventional materials [195,196,197,198,199,200,201]. One of the main benefits of these materials is their layer thickness, which is typically only a few atoms thick, making them ultra-thin and lightweight. In addition, the weak van der Waals force between layers enables simple exfoliation of these materials into thin layers, which enables the development of thin layers exhibiting distinct properties [202]. Due to its remarkable electrical conductivity, high surface area, and chemical stability, MoS2 has become a prominent contender as a material for flexible supercapacitor electrodes. When employed as an electrode material in flexible supercapacitors, MoS2 can improve their energy storage capacity, as well as their overall stability. The utilization of MoS2 in these capacitors shows great potential for next-generation energy storage devices that are lightweight, adaptable, and highly effective. Continued research into the fabrication and optimization of MoS2-based supercapacitors will be critical for realizing these capabilities and advancing the field of energy storage [203].
Manuraj et al. developed a symmetric supercapacitor utilizing MoS2 as an active material with an impressively large mass loading. The process of growing MoS2 nanowires was conducted over Ni foam through a basic hydrothermal technique. The MoS2 nanowire electrode prepared at 36 h with a bulk loading of 30 mg cm−2 showed a specific capacity of 244 F g−1 and displayed an energy density of 12.2 Wh kg−1 at 1 A g−1 in the symmetric configuration. Even after undergoing 9000 charge/discharge cycles at 5 A g−1, the capacitor managed to maintain almost 92% of its maximum capacitance [204]. A recent study reports the effective fabrication of an MoS2/Gr heterostructure using a cost-effective and simple strategy. The versatile and asymmetrical supercapacitor gadget demonstrated remarkable electrochemical performance, with a specific capacity of 208 F g−1 at 0.5 A g−1. It also has an impressive specific energy of 65 Wh kg−1 and a power density of 0.33 kW kg−1. Moreover, the device maintained 86.5% of its electrochemical capacitance in spite of undergoing 10,000 cycles, demonstrating its exceptional long-term durability [205]. The article describes the preparation and characterization of a high-performance flexible and self-sustaining aerogel film electrode made of MoS2/SWCNT/CNF that is highly efficient. The electrode was employed in the creation of an all-solid-state supercapacitor that is both flexible and symmetric. The specific capacity and specific energy of the supercapacitor electrode were observed to increase as the amount of MoS2–SWCNT was raised. It was observed that the substance containing the highest amount of MoS2-SWCNT in MoSCF3 was capable of achieving a specific capacity of 605.32 mF cm−2 at a speed of 2 mV s−1 and exhibited a capacitance of 30.34 F g−1 when the speed was reduced to 0.01 A g−1. At an area-specific power of 0.03 mW cm−2, MoSCF3 had a recorded area-specific energy of 35.61 mWh cm−2. After undergoing 10,000 cycles of both charging and discharging, the capacity retention rate for MoSCF3 was observed to be at 91.01% [206]. The creation of ultrathin electrodes using MoS2 nanosheets through inkjet printing marks a significant advancement in the production of in-plane microsupercapacitors that are flexible and solid-state (Figure 9). These capacitors possess a high capacitance, with a maximum energy density of 0.215 mWh cm−3 and a high-power energy density of 0.079 W cm−3, making them suitable for various applications. In addition, they display strong cycle stability, retaining 85.6% of their capacitance even after undergoing 10,000 charge/discharge cycles. Another crucial advantage of these MSCs is that they are easy to scale up. This scalability makes it possible to fabricate large-scale, integrated circuits that can be used in a range of applications [207].
Chen et al. utilized a laser etching technology to directly etch the self-supporting MXene-MoS2 film for micro-supercapacitor (MSC) production. The micro-supercapacitor exhibited a maximum specific capacitance of 173.6 F cm−3 at a rate of 1 mV s−1. Moreover, it demonstrated a high energy density of 15.5 mWh cm−3 and a high power density of 0.97 W cm−3. After undergoing 6000 cycles of charge/discharge and being bent up to 150 °C, the specific capacitances of the MSC remained at approximately 98% of its initial value, highlighting the robustness and longevity of the MSC device [208]. The flexible conducting film with mesh-like silver networks was coated using a spin coating process with a dispersion of MoS2 that had been exfoliated electrochemically. Consequently, the composite electrode showed a significant areal capacity of 89.44 mF cm−2 at a current density of 6 mA cm−2. The electrode has an impressive energy density of 12.42 µWh cm−2 and power density of 6043 µW cm−2 at a current density of 6 mA cm−2 while used in a symmetric supercapacitor cell layout [209]. The future scope of MoS2 and its composites for flexible supercapacitors holds great potential in enhancing the performance, stability, and integration of energy storage devices. Continued research in this area will enable the development of more efficient and reliable energy storage systems. The electrochemical performances of several other MoS2 nanocomposite electrodes for FSC applications are listed in Table 2.

3.3. Energy Conversion Applications

MoS2 has been widely studied for its potential applications in energy conversion reactions, including photovoltaic cells, hydrogen production, and catalytic reactions. Studies have shown that MoS2 can be used as a highly efficient and stable photo-absorber in solar cells. MoS2 has shown excellent activity, stability, and durability as a catalyst in hydrogen evolution reactions. Apart from that, MoS2 has also been found to be effective in many other catalytic reactions, such as CO2 reduction, water splitting, and oxygen reduction reactions [219,220].

3.3.1. Carbon Dioxide (CO2) Reduction

MoS2 is a promising material for CO2 reduction reactions, and ongoing research is focused on improving its conductivity and catalytic activity to make it comparable to other noble metal-based catalysts. With further advancements in this field, MoS2 could become an attractive alternative for sustainable CO2 conversion technologies [221]. Asadi et al. investigated that the edges of MoS2, specifically the inclined or sharp edges, are particularly effective at adsorbing CO2 and reducing it to CO. The study found that the inclined edges of MoS2 have a higher density of active sites for CO2 adsorption and reduction compared to the flat surfaces [222]. Recent research has shown that the concentration of sulfur vacancies in MoS2 materials can have a significant impact on their electrocatalytic performance for the reduction of CO2. Specifically, the presence of these vacancies can lead to lower overpotentials during the CO2 reduction reaction (CO2RR) and potentially offer a more efficient means of converting CO2 into valuable fuels and other chemicals. To better guide the design of these materials, researchers have used S K-edge x-ray absorption spectroscopy to identify the unique spectral signature associated with sulfur vacancies in MoS2. These findings offer promising avenues for the development of more efficient CO2RR electrocatalysts by leveraging the unique properties of sulfur-deficient MoS2 materials [223]. Linghu et al. investigated the catalytic potential of single-atom catalysts with low dimensionality for reducing CO2 to CH4. The research primarily examines how transition metal-modified 1T′-MoS2 monolayers promote stability and decrease CO2 through their catalytic mechanisms. The findings indicate that introducing transition metals in 1T′-MoS2 can expand the range of CO2RR products. Upon evaluating different catalysts, it was noted that Ru@1T′-MoS2 and Pt@1T′-MoS2 display the ability to stimulate the conversion of CO2 into CH4 and CH3OH, with relatively low limiting potentials of −0.56 and −0.73 V, respectively [224]. MoS2 has exposed edges that have a tendency to attract CO2 molecules and facilitate the catalytic conversion of CO2 to CO. This is achieved through the activation of the CO2 molecule by two Mo atoms located next to each other, causing the C–O double bond to undergo reconstruction during the adsorption process. The initial reaction between protons and electrons (H+ + e) occurring at the edges of MoS2 follows a distinct pathway compared to that of a transition metal catalyst. It was further proved that the release of CO from the edges of MoS2 happens due to a distinct diffusion process for the CO atoms that have been adsorbed [225].
Recent research investigations have demonstrated that aqueous electrolytes containing single-crystal MoS2 or thin-film MoS2 electrodes can effectively reduce carbon dioxide, yielding 1-propanol as the primary CO2 reduction product. Furthermore, the predominant reduction process occurring at these electrodes is the reduction of water into hydrogen gas [226]. Khan et al. demonstrated that the addition of MoS2 layers onto NiTiO3 nanofibers could enhance the CO2 conversion yield significantly. In the study, the optimized combination yielded CO and CH4 at a rate of 130 and 55 μmol g−1 h−1, respectively, which is remarkably higher than those achieved from pure NiTiO3 nanofibers. Specifically, the yields were 3.8 times more for CO and 3.6 times more for CH4 compared to the pure nanofibers. This finding suggests that the tailored integration of the MoS2 layer on NiTiO3 nanofibers can potentially lead to the design of more efficient and effective CO2 conversion catalysts [227].

3.3.2. Solar Cells

MoS2 has distinct chemical and structural properties that make it a highly desirable material for utilization in solar cells. Its outstanding carrier mobility facilitates the easy transfer of electrons and holes, leading to improved power conversion ability when employed in solar cells [228]. Tsai et al. successfully created a high-efficiency photovoltaic device by forming a type-II heterojunction with p-Si and MoS2 monolayers. The remarkable power conversion efficiency of 5.23% was achieved in a heterojunction photovoltaic device by utilizing a built-in electric field introduced near the interface, which aided in the separation of photogenerated carriers. This achievement represents a significant breakthrough in the use of monolayer TMDs for solar cell applications [229]. The integration of MoS2 into the ITO/p-Si/Ag solar cell structure has resulted in significant improvements in key performance factors, such as short-circuit current density, open-circuit voltage, and fill factor. These improvements have resulted in a remarkable increase in the conversion rate of the solar cell, from 1.1% to an impressive 4.6% [230]. The device with a structure of glass/FTO/MoS2/perovskite-po-spiro-OMeTAD/Au was utilized to produce perovskite solar cells (PSCs). These cells (Figure 10) demonstrated a power conversion rate of 13.1%, which is quite similar to the PSCs based on solid TiO2 and SnO2 electron transport layers [231]. Iqbal et al. described the effective activation of surface plasmon polaritons (SPPs) by fine-tuning the geometrical properties of MoS2-Au. The main objective is to improve the efficiency of photovoltaic cells that rely on plasmonics. This can be achieved by adjusting the slit widths (range encompasses wavelengths between 270 nm and 480 nm) and material thickness (ranging from 40 nm to 50 nm) while maintaining a constant periodicity of 720 nm for the unit cell [232].
Sattari et al. investigated the impact of a monolayer MoS2 film on the absorbance of CH3NH3PbI3, a favorable material for perovskite solar cells. The results show that the existence of the MoS2 film induces a rise in the absorbance of longer wavelengths [233]. Aymukhanov et al. described the findings from an investigation into how the presence of MoS2 nanoparticles affects electron transportation in the zinc oxide transport layer of a polymer solar cell. The researchers used impedance spectra measurements to analyze an organic solar cell and discovered that at a specific concentration, MoS2 nanoparticles enhance the lifetime of charge carriers and the diffusion coefficient in the composite film of zinc oxide [234]. The use of MoS2-assisted substrates for preparing perovskite films leads to improved crystallinity, which can be witnessed by enhanced photoluminescence and a prolonged emission lifetime. MoS2 quantum dots have a wider bandgap of 2.68 eV, which not only helps in hole collection but also prevents photogenerated electrons from moving to the hole transport layer [235]. The use of MoS2 nanoflakes as a hole transport interlayer can significantly enhance the stability and efficiency of Cs2AgBiBr6-based perovskite solar cells [236]. The hydrothermal technique was employed to deposit a blend of 1T and 2H phases of MoS2 onto an FTO substrate, resulting in the formation of thin films. The bandgap of MoS2 increased from 1.82 eV to 1.97 eV due to the change in shape, resulting in the superiority of mixed-phase MoS2 nanobelts. This makes them potential candidates for counter electrodes in platinum-free dye-sensitized solar cells at a lower cost [237].

3.3.3. Hydrogen Evolution Reactions (HER)

MoS2 is a highly feasible substitute for valuable platinum in the catalysis of the hydrogen evolution reaction (HER). This is because it is abundant in nature, inexpensive, and has tunable electronic properties, as well as exceptional chemical stability. The potential to control the electronic properties of MoS2 during the catalysis process of HER could lead to fresh possibilities in the catalytic use of other transitional metal dichalcogenide materials and more [238]. The inclusion of heteroatoms is a useful approach for improving the catalytic behaviors of MoS2 through the impacts of interfaces and anions. This method can raise the number of active sites that facilitate speedy electron transfer. These advancements include the engineering of interfaces and anions, specifically for MoS2-Mo2C, MoS2-MoO2, MoS2-MoSe2, MoS2-MoP, and MoS2-MoNx. Enhanced conductivity and catalytic activity can be achieved through the introduction of heteroatom doping and the formation of heterostructures, leading to a substantial improvement in the performance of hydrogen evolution reaction [239]. An inkjet printing technique was used to create a Cu-supported 3D patterned catalyst consisting of MoS2/VP/RGO with partial 1 T-MoS2 and spatial configuration. This catalyst demonstrated remarkable catalytic performance, boasting an extremely minimal overpotential (51 mV at 10 mA cm−2, 126 mV at 100 mA cm−2), a very low Tafel slope (32 mV dec−1), and an exceptionally high cathodic current density [240]. The use of Er-MOF/MoS2 composite materials has proved to be a significant breakthrough in the field of electrocatalysis. These materials possess a porous structure, exposing more active sites and enhancing conductivity. This unique feature has resulted in exceptional hydrogen evolution reaction activity in acidic media, achieving a current density of 10 mA cm−2 with only 234 mV overpotential. Moreover, the Tafel slope of 54.3 mV dec−1 highlights the superior proficiency of these materials towards HER [241]. It has been found that reducing the growth time and temperature to sufficiently low levels enhances the performance of the HER catalysts. This promising observation offers a potential pathway for designing high-performance HER catalysts using MoS2-based compounds. This finding has significant effects on the progress of renewable energy technologies that rely on efficient HER [242]. The unique structure of the dendrite edge nanostructures in the monolayer MoS2 offers notable advantages over traditionally synthesized thermodynamic equilibrium MoS2. Due to the higher catalytic site densities, the dendrite MoS2 monolayer provides a highly efficient reaction surface area for HER. The Tafel slope of the dendrite MoS2 monolayer was significantly lower (59 mV dec−1) compared to the triangular MoS2 sample (97 mV dec−1), indicating that the dendrite MoS2 monolayer is more effective in facilitating HER [243].
The CoCH nanosheets were utilized to create a three-dimensional self-supported cross-linked Co-MoS2 nanostructured HER catalyst. This catalyst has numerous active centers and the ability to transfer electrons quickly. Furthermore, the Co component is effective in activating the basal-plane sulfur atom in MoS2, making it the reactive center for HER [244]. The remarkable durability of the MoS2@Gr catalyst has been proven through extended experimentation in both acidic and alkaline electrolytes [245]. The research on morphology and spectroscopy suggests the production of excellent MoS2 nanosheets with metal ions that have been randomly doped. It is noteworthy to point out that Ni-MoS2 exhibited a superior HER performance in comparison to Co-MoS2 and Fe-MoS2 when considering other transition metals doping on MoS2. To achieve a current density of 10 mA cm−2, an overpotential of only −0.302 V vs. reversible hydrogen electrode (RHE) was needed for Ni-MoS2 [246]. The enhanced efficiency of HER observed in the MoS2 electrocatalyst doped with dual atoms is a result of alterations made to the electronic structure of the material. The dual atoms act as electron donors, and they effectively regulate charge on the S site, increasing the adsorption of H+. The almost negligible binding energy of H adsorption was discovered in the TM-Co co-doped layer of MoS2. It is highly noteworthy because it suggests that this substance could serve as a proficient electrocatalyst for HER and potentially replace platinum [247]. The Co, P-codoped MoS2, which is an optimized form of molybdenum disulfide, has shown remarkable catalytic activity. It exhibits a lower overpotential of 230 mV at a current density of 10 mA cm−2. The Tafel slope is smaller than 53 mV dec−1, which implies that the rate of HER is much faster compared to the pristine MoS2. Furthermore, the Co, P-MoS2 has also demonstrated excellent stability in acidic media, which is a crucial factor for the long-term use of catalysts in practical uses [248]. The 1T MoS2/NiS heterostructure exhibits higher efficiency in HER activity in comparison to 1T MoS2, particularly in 1.0 M KOH. At a current density of 10 mA cm−2, it attains a 0.12 V overpotential and a Tafel slope of 69 mV dec−1. This improvement is credited to interface engineering, which regulates the electronic states of the S sites in 1T MoS2, thus contributing to the boosted HER activity of the 1T MoS2/NiS heterostructure [249]. Wei et al. utilized interface engineering to create a heterostructure of 1T-MoS2/NiS, as shown in Figure 11. The resulting heterostructure demonstrated greater activity in terms of HER compared to that of 1T-MoS2, specifically in a 1.0 M KOH solution. At a current density of 10 mA cm−2, it achieved an overpotential of 0.12 V and had a Tafel slope of 69 mV dec−1. According to calculations based on density functional theory (DFT), the heterostructure of 1T-MoS2/NiS induced by interface engineering shows regulated electronic states of S sites in 1T-MoS2, which leads to an improved HER activity. This study suggests that adjusting the electronic structure through interface engineering could be an effective approach for enhancing the intrinsic activity of electrocatalysts [249].

3.3.4. Oxygen Evolution Reactions (OER)

The oxygen evolution reaction (OER) is the electrochemical process of generating oxygen gas from water in the presence of an electric potential. It is an important reaction in various applications, including in the production of hydrogen fuel from water and in renewable energy generation systems such as electrolyzers and fuel cells. German, E. et al. reported that the poor performance of monolayer MoS2 in the oxygen evolution reaction could be attributed to the fact that the reaction intermediates HO* and HOO* bind less strongly compared to the intermediate O*, resulting in a higher overpotential of 1.13 eV. The overpotential on the Mo-edge is nearly the same as that on the pure MoS2 monolayer, while on the S-edge, the overpotential is significantly higher. This means the S-edge configuration is even less desirable for the OER [250]. Bao et al. created a heterostructure catalyst for OER on a Ti mesh substrate by merging MoS2 nanosheets with NiCo2O4 hollow spheres. The electrocatalyst has demonstrated outstanding OER performance in an alkaline setting, producing overpotentials of 313 and 380 mV and reaching 10 and 100 mA cm−2 [251]. The remarkable electrochemical characteristics of the hybrid nanomaterial, comprising 1T MoS2/Co3S4/Ni3S2, demonstrate its potential as a favorable option for energy conversion uses. The nanoarray is able to achieve low overpotentials of only 50 and 240 mV at a current density of 10 mA cm−2 for HER and OER, respectively. Furthermore, the nanoarray displays remarkable stability, making it a reliable and long-lasting option for applications in various electrochemical devices [252]. The SnO2@MoS2 heterostructures and the synergistic effects of MoS2 and SnO2 contributed to the improved catalytic activity in both HER and OER. The bi-functional electrode, which possessed these distinct characteristics, demonstrated remarkable performance in alkaline water electrolysis. It accomplished 10 mA cm−2 at a cell voltage of 1.57 V and retained 98.3% of its initial current after 300 h of continuous testing, exhibiting exceptional long-term electrochemical stability [253]. The unique 3D structure of MoS2 nanosheets anchored on Ni9S8 nanorods has shown promising results in the field of water splitting. As a result, the MoS2/Ni9S8 composite exhibits a low overpotential at 50 mA cm−2 for OER and 10 mA cm−2 for HER during the water-splitting process [254]. The electrocatalytic activity of cobalt-aluminum-layered double hydroxide can experience substantial improvement through the dual doping of MoS2 and Ce. As a result, CoAl LDH@MoS2 with 5% Ce exhibits a potential of 1.508 V at a current density of 10 mA cm−2, which is notably lower than the 1.733 V observed in CoAl LDH [255]. A novel Ni(OH)2/MoS2/NF electrocatalyst was synthesized using two-step hydrothermal and solvothermal methods shown in Figure 12. Exceptional OER performance in 1.0 M KOH electrolyte was observed, with a lower overpotential of 296 mV at 50 mA cm−2, along with remarkable durability. A thorough examination demonstrates that the improved catalytic activity results from the cooperative influence of Ni(OH)2 and MoS2, which provides more active sites for the catalyst. This also offers a dependable approach to implementing heterogeneous interface engineering for energy catalysis [256].
The single-atom catalytic mechanism utilized in TMO6@MoS2 (TM = Fe, Mn and Co) species creates active sites and orbitals that are responsive to adsorption. This allows for increased adsorption of oxidative intermediates and ultimately improves the catalytic activity of the OER. When compared to benchmark IrO2, TMO6@MoS2 species demonstrate superior electrocatalytic activity for the OER [257]. The combination of CoFeOx(OH)y and MoS2 results in greater efficiency in converting water into oxygen through the process of oxidation. This occurs because the electronic interaction between the two materials increases the amount of energy available to convert water into oxygen, leading to improved activity and stability of the electrode. The resultant CFOMS-CP electrode offers a promising solution for efficient and reliable electrochemical OER applications [258]. The formation of heterojunctions has been demonstrated to be an effective method for enhancing the electrocatalytic activity of materials, particularly in the context of OER. In the case of MoS2, the incorporation of a graphene-like material, g-C3N4, has demonstrated significant improvements in OER performance due to the modification of the electronic structure. The high catalytic activity of the MoS2/g-C3N4 heterojunction can be attributed to the heteroepitaxial growth of the two materials, creating an interface between them. This electronic coupling enables efficient electron transfer between the materials, which promotes the OER process [259]. Elrahim et al. explored the fabrication of Co3O4–MoS2/Ni foam electrodes utilizing a vacuum kinetic spray method with microparticles of MoS2 and Co3O4. The research findings suggest that the addition of MoS2 in a gradual manner increases the OER activity, which is attributed to improved charge transfer kinetics [260]. The use of AlCo3-MoS2 substrate in electrocatalytic OER applications has shown to be highly effective due to the production of M−O (M=Al, Co and Mo) species with oxygen vacancies. These species play a crucial role in initiating the surface self-reconstruction of pre-catalysts, resulting in the formation of new and highly active facets. The oxygen vacancies created on the substrate also assist in improving the electronic conductivity of the catalyst, further enhancing its electrocatalytic performance [261].
Mixed oxide-based lithium electrode batteries are widely favored for their stability and capacity retention after numerous cycles. In contrast, MoS2-based LIBs have impressive specific capacities but require further improvement in cycling stability and cost-effectiveness to become more competitive. The rising cost and high demand for Li-ion batteries have sparked interest in exploring Na-ion-based batteries as a viable alternative. In order to meet commercial needs, it is important to conduct more thorough research on electrode materials, electrolytes and current collectors for SIBs. This can accelerate the path toward commercialization by enhancing our understanding of storage capacity and the preparation of electrode materials. MoS2 has become increasingly popular as a material for supercapacitors due to its decent charge storage capacity. However, it still falls behind state-of-the-art materials like graphene or mixed oxide, which possess considerably higher specific surface areas for charge storage. Research is being conducted on composite materials that contain MoS2 to enhance their storage capacity. However, the manufacturing cost of these composites is high, and there is a loss in electrochemical performance that needs to be resolved. There are still challenges to be addressed when it comes to integrating MoS2 into solar cells, such as ensuring its stability and scalability, but the potential benefits are great. With continued research and development, MoS2-based solar cells could become a major player in the renewable energy market. The ongoing research on HER catalysts is primarily centered on substituting costly noble metal catalysts with more economical and easily accessible materials. The ultimate objective for HER catalysts materials is to reduce the Tafel slope and enhance the current density. Recently, there has been a shift towards utilizing MoS2-based electrocatalysts as a means to enhance catalytic performance and eliminate the use of noble metals. These catalysts have demonstrated comparable long-term stability in HER acidic solutions as platinum-based electrocatalysts. However, the existing MoS2-based catalysts have limited ability to produce high current densities, leading to impractical Tafel slopes. On the contrary, electrodes based on MoS2 are not yet as efficient and stable over repeated cycles compared to the current leading technology. Despite its high electrical conductivity, 1T-MoS2 is challenging to prepare as it involves the use of hazardous and air-sensitive materials. Advanced equipment like glove boxes and autoclaves are necessary, which makes its manufacturing expensive and difficult to scale. Therefore, finding a safer method to prepare conductive MoS2 would be highly advantageous in overcoming the limitations of electrical conductivity.

4. Challenges and Future Directions

Despite the promising properties of MoS2, there are certain challenges that limit its commercial applications. Synthesizing MoS2 on a large scale in a cost-effective way is still a major challenge. The conductivity of 2H MoS2 and the stability of 1T MoS2 has to be addressed in the future. The outstanding properties of 1T MoS2 were more suitable for commercial energy storage applications in hybrid supercapacitors. More research has been focused on increasing the production of 1T MoS2 using several synthesis techniques and stability [38,109]. The properties of MoS2 also depend on its quality and size, which can be influenced by the synthesis method, additives, and processing conditions. To achieve high-quality MoS2, its synthesis method needs careful consideration, as even minor variations can impact its properties. The preferred method for producing an MoS2 layer that is uniform, of high quality, and covers a large surface area is chemical vapor deposition (CVD). However, the CVD process has certain limitations, such as high-temperature requirements and limited control over thickness and size. Besides the synthesis method, additional processing steps are also required to optimize MoS2’s properties. These additional steps include surface modification, doping, and dispersion in various solvents. Surface modification can improve MoS2’s properties by increasing its stability, biocompatibility, and electrical conductivity. Doping of MoS2 with other elements can enhance its electronic and optical properties, as well as improve its catalytic activities. Dispersion of MoS2 in solvents can increase its uniformity, stability, and availability for further processing. Apart from the crystal quality and size, controlling the particle size of MoS2 is also crucial for numerous applications, including energy storage and catalysis. The particle size of MoS2 affects its surface area and hence its reaction kinetics, as well as its interaction with other materials. Therefore, several techniques have been developed to control MoS2 particle size, including hydrothermal synthesis, microwave-assisted synthesis, and electrode deposition. In conclusion, the particle size, crystalline structure, and purity of MoS2 are critical factors that need careful consideration to harness its full potential in various applications. A better understanding of the synthesis and processing methods can maximize MoS2’s properties, ultimately leading to its widespread usage in various fields ranging from energy to biomedicine [262].
To overcome the stability issue, researchers are making enormous efforts to enhance the metallic phase of MoS2. There have been significant advancements in this area, including the usage of transition metal doping and chemical treatment methods to improve the cyclic stability of MoS2 in the metallic phase. Despite these advancements, there is still a need for further research to improve the stability of MoS2 in its metallic phase. The study of MoS2’s stability has both scientific and practical applications, and addressing these issues will open up new avenues for its use in various fields, including electronics, energy storage and catalysis [263]. MoS2 has good electrochemical properties in energy applications, but it seems to be low as compared to Nobel metals [264]. The study of pristine MoS2 was almost completed, but the study of its nanocomposites with noble metals, carbon and metal oxides/sulfides with outstanding characteristics in energy storage/conversion applications needs further research [39,265]. The restacking of the layers in MoS2 reduces its effectiveness in certain applications. Additionally, MoS2 undergoes significant volume expansion during electrochemical intercalation, which can lead to structural instability or even failure. Another issue is its poor intrinsic electronic conductivity, which hinders its ability to efficiently conduct electrical charges. While researchers are actively exploring ways to mitigate these challenges, further developments are needed to fully unlock the potential of MoS2 for practical and commercial use [266,267].
The several research gaps in the understanding and development of MoS2 and its composites are summarized.
  • Synthesis methods: there is a need for developing simple, cost-effective synthesis methods for large-scale production of MoS2 and its composites, especially those with controlled morphology and structure;
  • Stability and durability: it is crucial to investigate the stability and durability of MoS2 and its composites under various environmental and mechanical conditions, which would provide insights into the potential applications of these materials;
  • Composites design: developing novel and effective composite designs by incorporating MoS2 with other materials can lead to enhanced properties, such as mechanical strength, electrical conductivity, and wear resistance. However, there is still a need to identify the optimum composition and processing conditions for achieving the desired properties;
  • Characterization: there are still gaps in the understanding of the structural and compositional properties of MoS2 and its composites, particularly for those with multiple layers and complex architectures;
  • Applications: the full potential of MoS2 and its composites in various applications, including energy storage, catalysis, electronics, and biomedicine, is yet to be explored. It is necessary to investigate the performance and reliability of these materials in real-world applications.
Overall, bridging these research gaps can significantly advance our understanding and utilization of MoS2 and its composites in various fields.

5. Conclusions

Our review highlights MoS2 as an emerging material for future energy applications. MoS2 stands out due to its economic cost, copious availability, and uncomplicated synthesis process. Moreover, its distinctive photocatalytic and electrocatalytic characteristics and structure have created opportunities for its utilization in energy generation reactions and energy storage devices. In addition, the characteristics of its structure, photocatalysis, and electrocatalysis have made it suitable for utilization in energy storage devices and energy generation applications. The chemical exfoliation approach is a convenient choice for industrial manufacturing procedures because it can be expanded effortlessly to produce MoS2 nanosheets on a large scale. The 1T MoS2 metallic phase has several desirable properties that make it suitable for use in various applications. As a result of its excellent conductivity and relatively weak van der Waal forces between layers, it is a suitable material for use as a Li-ion battery anode because Li-ions can easily intercalate between the layers. It also has a large area and superconductivity, making it perfect for use in supercapacitors. Its ability to restack easily is an added advantage. The high electrocatalytic and photocatalytic activity of MoS2 makes it useful in solar cells and hydrogen/oxygen evolution reactions. It has the potential to minimize CO2 and generate energy, making it a promising solution for environmentally-friendly energy production and mitigation of CO2 levels in our surroundings. The use of MoS2 in various technological applications is still being explored and researched, and it holds immense potential for the development of novel and advanced technologies. As the demand for sustainable and environmentally friendly solutions grows, the versatility and unique properties of MoS2 make it a valuable material in the advancement of various technological fields. It is evident that the potential of MoS2 is limitless and future research in this area is necessary to explore its full potential and benefit society as a whole.

Author Contributions

Investigation and writing-original draft, K.B.M.I.; Conceptualization, visualization, writing—original draft, and supervision M.A.K.; Investigation and visualization, S.M. and J.K.; Visualization and writing—review & editing, R.A. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Gao, P.; Xiao, Y.; Li, L.; Li, W.; Tao, W. Biomedical applications of 2D monoelemental materials formed by group VA and VIA: Aconcise review. J. Nanobiotechnol. 2021, 19, 96. [Google Scholar] [CrossRef] [PubMed]
  2. Piggot, G.; Erickson, P.; Boudet, H.; Hazboun, S. Fossil fuel export as a climate policy problem. In Public Responses to Fossil Fuel Export; Elsevier: Amsterdam, The Netherlands, 2022; pp. 45–54. [Google Scholar]
  3. Olanipekun, I.O.; Ozkan, O.; Olasehinde-Williams, G. Is renewable energy use lowering resource-related uncertainties? Energy 2023, 271, 126949. [Google Scholar] [CrossRef]
  4. Algarni, S.; Tirth, V.; Alqahtani, T.; Alshehery, S.; Kshirsagar, P. Contribution of renewable energy sources to the environmental impacts and economic benefits for sustainable development. Sustain. Energy Technol. Assess. 2023, 56, 103098. [Google Scholar] [CrossRef]
  5. Zhang, D.; Zheng, M.; Feng, G.; Chang, C. Does an environmental policy bring to green innovation in renewable energy? Renew. Energy 2022, 195, 1113–1124. [Google Scholar] [CrossRef]
  6. Sayed, E.T.; Olabi, A.G.; Alami, A.H.; Radwan, A.; Mdallal, A.; Rezk, A.; Abdelkareem, M.A. Renewable Energy and Energy Storage Systems. Energies 2023, 16, 1415. [Google Scholar] [CrossRef]
  7. Guerra, O.J.; Zhang, J.; Eichman, J.; Denholm, P.; Kurtz, J.; Hodge, B.M. The value of seasonal energy storage technologies for the integration of wind and solar power. Energy Environ. Sci. 2020, 13, 1909–1922. [Google Scholar] [CrossRef]
  8. Behabtu, H.A.; Messagie, M.; Coosemans, T.; Berecibar, M.; Anlay Fante, K.; Kebede, A.A.; Mierlo, J.V. A Review of Energy Storage Technologies’ Application Potentials in Renewable Energy Sources Grid Integration. Sustainability 2020, 12, 10511. [Google Scholar] [CrossRef]
  9. Kalair, A.; Abas, N.; Saleem, M.S.; Kalair, A.R.; Khan, N. Role of energy storage systems in energy transition from fossil fuels to renewables. Energy Storage 2021, 3, e135. [Google Scholar] [CrossRef] [Green Version]
  10. Chen, H.; Ling, M.; Hencz, L.; Ling, H.Y.; Li, G.; Lin, Z.; Liu, G.; Zhang, S. Exploring Chemical, Mechanical, and Electrical Functionalities of Binders for Advanced Energy-Storage Devices. Chem. Rev. 2018, 118, 8936–8982. [Google Scholar] [CrossRef]
  11. Riaz, A.; Sarker, M.R.; Saad, M.H.M.; Mohamed, R. Review on Comparison of Different Energy Storage Technologies Used in Micro-Energy Harvesting, WSNs, Low-Cost Microelectronic Devices: Challenges and Recommendations. Sensors 2021, 21, 5041. [Google Scholar] [CrossRef]
  12. Li, C.; Wang, Z.; He, Z. An advance review of solid-state battery: Challenges, progress and prospects. Sustain. Mater. Technol. 2021, 29, e00297. [Google Scholar] [CrossRef]
  13. Simon, P.; Gogotsi, Y. Perspectives for electrochemical capacitors and related devices. Nat. Mater. 2020, 19, 1151–1163. [Google Scholar] [CrossRef] [PubMed]
  14. Covaci, C.; Gontean, A. “Singing” Multilayer Ceramic Capacitors and Mitigation Methods—A Review. Sensors 2022, 22, 3869. [Google Scholar] [CrossRef]
  15. Musetti, A.; Sadegh Lafmejani, H.; Soldati, A. Control and Design of a Boost-Based Electrolytic Capacitor-Less Single-Phase-Input Drive. Energies 2022, 15, 5929. [Google Scholar] [CrossRef]
  16. Agrawal, M.; Singh, R.; Ranitović, M.; Kamberovic, Z.; Ekberg, C.; Singh, K.K. Global market trends of tantalum and recycling methods from Waste Tantalum Capacitors: A review. Sustain. Mater. Technol. 2021, 29, e00323. [Google Scholar] [CrossRef]
  17. Raghavendra, K.V.G.; Vinoth, R.; Zeb, K.; Muralee Gopi, C.V.V.; Sambasivam, S.; Kummara, M.R.; Obaidat, I.M.; Kim, H.J. An intuitive review of supercapacitors with recent progress and novel device applications. J. Energy Storage 2020, 31, 101652. [Google Scholar] [CrossRef]
  18. Sharma, K.; Arora, A.; Tripathi, S.K. Review of supercapacitors: Materials and devices. J. Energy Storage 2019, 21, 801–825. [Google Scholar]
  19. Patel, K.; Singhal, T.; Pandey, V.; Sumangala, T.P.; Sreekanth, M.S. Evolution and recent developments of high performance electrode material for supercapacitors: A review. J. Energy Storage 2021, 44, 103366. [Google Scholar] [CrossRef]
  20. Bokhari, S.W.; Siddique, A.H.; Sherrell, P.C.; Yue, X.; Karumbaiah, K.M.; Wei, S.; Ellis, A.V.; Gao, W. Advances in graphene-based supercapacitor electrodes. Energy Rep. 2020, 6, 2768–2784. [Google Scholar] [CrossRef]
  21. Özuğur Uysal, B.; Nayır, Ş.; Açba, M.; Çıtır, B.; Durmaz, S.; Koçoğlu, Ş.; Yıldız, E.; Pekcan, Ö. 2D Materials (WS2, MoS2, MoSe2) Enhanced Polyacrylamide Gels for Multifunctional Applications. Gels 2022, 8, 465. [Google Scholar] [CrossRef]
  22. Derakhshi, M.; Daemi, S.; Shahini, P.; Habibzadeh, A.; Mostafavi, E.; Ashkarran, A.A. Two-Dimensional Nanomaterials beyond Graphene for Biomedical Applications. J. Funct. Biomater. 2022, 13, 27. [Google Scholar] [CrossRef] [PubMed]
  23. Chen, H.; Zhang, J.; Kan, D.; He, J.; Song, M.; Pang, J.; Wei, S.; Chen, K. The Recent Progress of Two-Dimensional Transition Metal Dichalcogenides and Their Phase Transition. Crystals 2022, 12, 1381. [Google Scholar] [CrossRef]
  24. Wang, H.; Li, C.; Fang, P.; Zhang, Z.; Zhang, J.Z. Synthesis, Properties, and Optoelectronic Applications of Two-Dimensional MoS2 and MoS2-Based Heterostructures. Chem. Soc. Rev. 2018, 47, 6101–6127. [Google Scholar] [CrossRef]
  25. Lin, L.; Lei, W.; Zhang, S.; Liu, Y.; Wallace, G.G.; Chen, J. Two-dimensional transition metal dichalcogenides in supercapacitors and secondary batteries. Energy Storage Mater. 2019, 19, 408–423. [Google Scholar] [CrossRef]
  26. Prabhu, P.; Jose, V.; Lee, J. Design Strategies for Development of TMD-Based Heterostructures in Electrochemical Energy Systems. Matter 2020, 2, 526–553. [Google Scholar] [CrossRef] [Green Version]
  27. Li, T.; Li, H.; Yuan, J.; Xia, Y.; Liu, Y.; Sun, A. Recent Advance and Modification Strategies of Transition Metal Dichalcogenides (TMDs) in Aqueous Zinc Ion Batteries. Materials 2022, 15, 2654. [Google Scholar] [CrossRef] [PubMed]
  28. Ji, J.; Choi, J.H. Recent progress in 2D hybrid heterostructures from transition metal dichalcogenides and organic layers: Properties and applications in energy and optoelectronics fields. Nanoscale 2022, 14, 10648–10689. [Google Scholar] [CrossRef]
  29. Mia, A.K.; Meyyappan, M.; Giri, P.K. Two-Dimensional Transition Metal Dichalcogenide Based Biosensors: From Fundamentals to Healthcare Applications. Biosensors 2023, 13, 169. [Google Scholar] [CrossRef]
  30. Liu, Y.; NO, W.; Duan, X.; Cheng, H.-C.; Huang, Y.; Duan, X. Van der Waals Heterostructures and Devices. Nat. Rev. Mater. 2016, 1, 16042. [Google Scholar] [CrossRef]
  31. Chia, X.; Eng, A.Y.S.; Ambrosi, A.; Tan, S.M.; Pumera, M. Electrochemistry of nanostructured layered transition-metal dichalcogenides. Chem. Rev. 2015, 115, 11941–11966. [Google Scholar] [CrossRef] [Green Version]
  32. Kong, D.; Wang, H.; Cha, J.J.; Pasta, M.; Koski, K.J.; Yao, J.; Cui, Y. Synthesis of MoS2 and MoSe2 films with vertically aligned layers. Nano Lett. 2013, 13, 1341. [Google Scholar] [CrossRef] [PubMed]
  33. Chung, D.Y.; Park, S.K.; Chung, Y.H.; Yu, S.H.; Lim, D.H.; Jung, N.; Ham, H.C.; Park, H.Y.; Piao, Y.; Yoo, S.J.; et al. Edge-exposed MoS2nano-assembled structures as efficient electrocatalysts for hydrogen evolution reaction. Nanoscale 2014, 6, 2131–2136. [Google Scholar] [CrossRef] [PubMed]
  34. Zhang, X.; Lai, Z.; Tan, C.; Zhang, H. Solution-Processed Two-Dimensional MoS2 Nanosheets: Preparation, Hybridization, and Applications. Angew. Chem. Int. Ed. 2016, 55, 8816. [Google Scholar] [CrossRef] [PubMed]
  35. Cao, Y.; Lin, Y.; Wu, J.; Huang, X.; Pei, Z.; Zhou, J.; Wang, G. Two-Dimensional MoS2 for Li−S Batteries: Structural Design and Electronic Modulation. ChemSusChem 2020, 13, 1392–1408. [Google Scholar] [CrossRef] [PubMed]
  36. Yu, Y.; Huang, S.; Li, Y.; Steinmann, S.N.; Yang, W.; Cao, L. Layer-Dependent Electrocatalysis of MoS2 for Hydrogen Evolution. Nano Lett. 2014, 14, 553–558. [Google Scholar] [CrossRef] [Green Version]
  37. Isacfranklin, M.; Princy, L.E.; Rathinam, Y.; Kungumadevi, L.; Ravi, G.; Al-Sehemi, A.G.; Velauthapillai, D. Rare Earth-Doped MoS2 for Supercapacitor Application. Energy Fuels 2022, 36, 6476–6482. [Google Scholar] [CrossRef]
  38. Samy, O.; Zeng, S.; Birowosuto, M.D.; El Moutaouakil, A. A Review on MoS2 Properties, Synthesis, Sensing Applications and Challenges. Crystals 2021, 11, 355. [Google Scholar] [CrossRef]
  39. Wang, T.; Chen, S.; Pang, H.; Xue, H.; Yu, Y. MoS2-Based Nanocomposites for Electrochemical Energy Storage. Adv. Sci. 2017, 4, 1600289. [Google Scholar] [CrossRef]
  40. Liang, Z.; Zhao, C.; Zhao, W.; Zhang, Y.; Srimuk, P.; Presser, V.; Feng, G. Molecular Understanding of Charge Storage in MoS2 Supercapacitors with Ionic Liquids. Energy Environ. Mater. 2021, 4, 631–637. [Google Scholar] [CrossRef]
  41. Gupta, U.; Rao, C.N.R. Hydrogen generation by water splitting using MoS2 and other transition metal dichalcogenides. Nano Energy 2017, 41, 49–65. [Google Scholar] [CrossRef]
  42. Kim, R.; Kim, J.; Do, J.Y.; Seo, M.W.; Kang, M. Carbon Dioxide Photoreduction on the Bi2S3/MoS2 Catalyst. Catalysts 2019, 9, 998. [Google Scholar] [CrossRef] [Green Version]
  43. Xu, H.; Yi, J.; She, X.; Liu, Q.; Song, L.; Chen, S.; Yang, Y.; Song, Y.; Vajtai, R.; Lou, J.; et al. 2D heterostructure comprised of metallic 1T-MoS2/Monolayer O-g-C3N4 towards efficient photocatalytic hydrogen evolution. Appl. Catal. B Environ. 2018, 220, 379–385. [Google Scholar] [CrossRef]
  44. Backes, C.; Berner, N.C.; Chen, X.; Lafargue, P.; LaPlace, P.; Freeley, M.; Duesberg, G.S.; Coleman, J.N.; McDonald, A.R. Functionalization of liquid-exfoliated two-dimensional 2H-MoS2. Angew. Chem. Int. Ed. 2015, 54, 2638–2642. [Google Scholar] [CrossRef] [PubMed]
  45. Tan, D.; Willatzen, M.; Wang, Z.L. Prediction of strong piezoelectricity in 3R-MoS2 multilayer structures. Nano Energy 2019, 56, 512–515. [Google Scholar] [CrossRef]
  46. Li, S.; Sun, J.; Guan, J. Strategies to improve electrocatalytic and photocatalytic performance of two-dimensional materials for hydrogen evolution reaction. Chin. J. Catal. 2021, 42, 511–556. [Google Scholar] [CrossRef]
  47. Ma, Y.; Lu, S.; Dong, X.; Han, G.; Chen, Z.; Liu, Y. Optical parameters of graphene/MoS2 van der Waals heterostructure investigated by spectroscopic ellipsometry. Appl. Surf. Sci. 2022, 599, 153987. [Google Scholar] [CrossRef]
  48. Singh, A.; Moun, M.; Sharma, M.; Barman, A.; Kapoor, A.K.; Singh, R. NaCl-assisted substrate dependent 2D planar nucleated growth of MoS2. Appl. Surf. Sci. 2021, 538, 148201. [Google Scholar] [CrossRef]
  49. Yu, H.; Liao, M.; Zhao, W.; Liu, G.; Zhou, X.J.; Wei, Z.; Xu, X.; Liu, K.; Hu, Z.; Deng, K.; et al. Wafer-Scale Growth and Transfer of Highly-Oriented Monolayer MoS2 Continuous Films. ACS Nano 2017, 11, 12001–12007. [Google Scholar] [CrossRef]
  50. Yang, P.; Zhang, S.; Pan, S.; Tang, B.; Liang, Y.; Zhao, X.; Zhang, Z.; Shi, J.; Huan, Y.; Shi, Y.; et al. Epitaxial Growth of Centimeter-Scale Single-Crystal MoS2 Monolayer on Au(111). ACS Nano 2020, 14, 5036–5045. [Google Scholar] [CrossRef]
  51. Hu, Z.; Wang, L.; Zhang, K.; Wang, J.; Cheng, F.; Tao, Z.; Chen, J. MoS2Nanoflowers with Expanded Interlayers as High-Performance Anodes for Sodium-Ion Batteries. Angew. Chem. Int. Ed. 2014, 53, 12794–12798. [Google Scholar] [CrossRef]
  52. Li, W.J.; Shi, E.W.; Ko, J.M.; Chen, Z.Z.; Ogino, H.; Fukuda, T. Hydrothermal synthesis of MoS2 nanowires. J. Cryst. Growth 2003, 250, 418–422. [Google Scholar] [CrossRef]
  53. Chen, J.; Kuriyama, N.; Yuan, H.; Takeshita, H.T.; Sakai, T. Electrochemical hydrogen storage in MoS2 nanotubes. J. Am. Chem. Soc. 2001, 123, 11813–11814. [Google Scholar] [CrossRef] [PubMed]
  54. Hwang, H.; Kim, H.; Cho, J. MoS2 nanoplates consisting of disordered graphene-like layers for high rate lithium battery anode materials. Nano Lett. 2011, 11, 4826–4830. [Google Scholar] [CrossRef] [PubMed]
  55. Deokar, G.; Vancsó, P.; Arenal, R.; Ravaux, F.; Casanova-Cháfer, J.; Llobet, E.; Makarova, A.; Vyalikh, D.; Struzzi, C.; Lambin, P.; et al. MoS2–Carbon Nanotube Hybrid Material Growth and Gas Sensing. Adv. Mater. Interfaces 2017, 4, 1700801. [Google Scholar] [CrossRef]
  56. Chen, X.P.; Xing, G.J.; Xu, L.F.; Lian, H.Q.; Wang, Y. Vertically aligned MoS2 films prepared by RF-magnetron sputtering method as electrocatalysts for hydrogen evolution reactions. Compos. Interfaces 2020, 28, 707–716. [Google Scholar] [CrossRef]
  57. Li, X.; Zhu, H. Two-dimensional MoS2: Properties, preparation, and applications. J. Mater. 2015, 1, 33–44. [Google Scholar] [CrossRef] [Green Version]
  58. Ataca, C.; Şahin, H.; Aktürk, E.; Ciraci, S. Mechanical and Electronic Properties of MoS2 Nanoribbons and Their Defects. J. Phys. Chem. C 2011, 115, 3934–3941. [Google Scholar] [CrossRef] [Green Version]
  59. Kumar, A.; Ahluwalia, P.K. A first principle Comparative study of electronic and optical properties of 1H–MoS2 and 2H–MoS2. Mater. Chem. Phys. 2012, 135, 755–761. [Google Scholar] [CrossRef]
  60. Johari, P.; Shenoy, V.B. Tuning the Electronic Properties of Semiconducting Transition Metal Dichalcogenides by Applying Mechanical Strains. ACS Nano. 2012, 6, 5449–5456. [Google Scholar] [CrossRef]
  61. Habib, M.R.; Wang, W.; Khan, A.; Khan, Y.; Obaidulla, S.M.; Pi, X.; Xu, M. Theoretical Study of Interfacial and Electronic Properties of Transition Metal Dichalcogenides and Organic Molecules Based van der Waals Heterostructures. Adv. Theory Simul. 2020, 3, 2000045. [Google Scholar] [CrossRef]
  62. Venkata Subbaiah, Y.P.; Saji, K.J.; Tiwari, A. Atomically Thin MoS2: A Versatile Nongraphene 2D Material. Adv. Funct. Mater. 2016, 26, 2046–2069. [Google Scholar] [CrossRef]
  63. Kadantsev, E.S.; Hawrylak, P. Electronic Structure of a Single MoS2 Monolayer. Solid State Commun. 2012, 152, 909–913. [Google Scholar] [CrossRef]
  64. Tsai, Y.-C.; Li, Y. Impact of Doping Concentration on Electronic Properties of Transition Metal-Doped Monolayer Molybdenum Disulfide. IEEE Trans. Electron. Devices 2018, 65, 733–738. [Google Scholar] [CrossRef]
  65. Williamson, I.; Li, S.; Hernandez, A.C.; Lawson, M.; Chen, Y.; Li, L. Structural, electrical, phonon, and optical properties of Ti- and V-doped two-dimensional MoS2. Chem. Phys. Lett. 2017, 674, 157–163. [Google Scholar] [CrossRef]
  66. Halim, S.N.M.; Zuikafly, S.N.F.; Taib, M.F.M.; Ahmad, F. First Principles Study on Electronic and Optical Properties of Graphene/MoS2 for Optoelectronic Application. In Proceedings of the 2020 IEEE International Conference on Semiconductor Electronics (ICSE), Kuala Lumpur, Malaysia, 28–29 July 2020; pp. 29–32. [Google Scholar]
  67. Nalwa, H.S. A Review of Molybdenum Disulfide (MoS2) Based Photodetectors: From Ultra-Broadband, Self-Powered to Flexible Devices. RSC Adv. 2020, 10, 30529–30602. [Google Scholar] [CrossRef] [PubMed]
  68. Aryeetey, F.; Pourianejad, S.; Ayanbajo, O.; Nowlin, K.; Ignatova, T.; Aravamudhan, S. Bandgap recovery of monolayer MoS2 using defect engineering and chemical doping. RSC Adv. 2021, 11, 20893–20898. [Google Scholar] [CrossRef]
  69. Xia, Z.; Tao, Y.; Pan, Z.; Shen, X. Enhanced photo catalytic performance and stability of 1T MoS2 transformed from 2H MoS2 via Li intercalation. Results Phys. 2019, 12, 2218–2224. [Google Scholar] [CrossRef]
  70. Cheng, Y.; Wang, J.-Z.; Wei, X.-X.; Guo, D.; Wu, B.; Yu, L.-W.; Wang, X.-R.; Shi, Y. Tuning Photoluminescence Performance of Monolayer MoS2 via H2O2 Aqueous Solution. Chin. Phys. Lett. 2015, 32, 117801. [Google Scholar] [CrossRef]
  71. Amani, M.; Lien, D.-H.; Kiriya, D.; Xiao, J.; Azcatl, A.; Noh, J.; Madhvapathy, S.R.; Addou, R.; Kc, S.; Dubey, M.; et al. Near-Unity Photoluminescence Quantum Yield in MoS2. Science 2015, 350, 1065–1068. [Google Scholar] [CrossRef] [Green Version]
  72. Thomas, N.; Mathew, S.; Nair, K.M.; O’Dowd, K.; Forouzandeh, P.; Goswami, A.; McGranaghan, G.; Pillai, S.C. 2D MoS2: Structure, mechanisms, and photocatalytic applications. Mater. Today Sustain. 2021, 13, 100073. [Google Scholar] [CrossRef]
  73. Ghorbani-Asl, M.; Zibouche, N.; Wahiduzzaman, M.; Oliveira, A.F.; Kuc, A.; Heine, T. Electromechanics in MoS2 and WS2: Nanotubes vs. Monolayers. Sci. Rep. 2013, 3, 2961. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  74. Yan, R.; Simpson, J.R.; Bertolazzi, S.; Brivio, J.; Watson, M.; Wu, X.; Kis, A.; Luo, T.; Hight Walker, A.R.; Xing, H.G. Conductivity of Monolayer Molybdenum Disulfide Obtained from Temperature-Dependent Raman Spectroscopy. ACS Nano 2014, 8, 986–993. [Google Scholar] [CrossRef] [PubMed]
  75. Krishnan, U.; Kaur, M.; Singh, K.; Kumar, M.; Kumar, A. A synoptic review of MoS2: Synthesis to applications. Superlattices Microstruct. 2019, 128, 274–297. [Google Scholar] [CrossRef]
  76. Singh, A.; Late, D.J.; Kumar, A.; Patel, S.; Singh, J. 2D layered transition metal dichalcogenides (MoS2): Synthesis, applications and theoretical aspects. Appl. Mater. Today 2018, 13, 242–270. [Google Scholar] [CrossRef]
  77. Palanisamy, R.; Karuppiah, D.; Venkatesan, S.; Mani, S.; Kuppusamy, M.; Marimuthu, S.; Karuppanan, A.; Govindaraju, R.; Marimuthu, S.; Rengapillai, S.; et al. Performance asymmetric supercapacitor fabricated with a novel MoS2/Fe2O3/Graphene composite electrode. Colloids Interface Sci. Commun. 2022, 46, 100573. [Google Scholar] [CrossRef]
  78. Anbalagan, A.k.; Hu, F.C.; Chan, W.K.; Gandhi, A.C.; Gupta, S.; Chaudhary, M.; Chuang, K.W.; Ramesh, A.K.; Billo, T.; Sabbah, A.; et al. Gamma-Ray Irradiation Induced Ultrahigh Room-Temperature Ferromagnetism in MoS2 Sputtered Few-Layered Thin Films. ACS Nano 2023, 17, 6555–6564. [Google Scholar] [CrossRef]
  79. Li, H.; Wu, J.; Yin, Z.; Zhang, H. Preparation and applications of mechanically exfoliated single-layer and multilayer MoS2 and WSe2 nanosheets. Acc. Chem. Res. 2014, 47, 1067–1075. [Google Scholar] [CrossRef]
  80. Jeon, J.; Lee, J.; Yoo, G.; Park, J.H.; Yeom, G.Y.; Jang, Y.H.; Lee, S. Size-tunable synthesis of monolayer MoS2 nanoparticles and their applications in non-volatile memory devices. Nanoscale 2016, 8, 16995–17003. [Google Scholar] [CrossRef]
  81. Zhang, S.; Liu, X.; Liu, C.; Luo, S.; Wang, L.; Cai, T.; Zeng, Y.; Yuan, J.; Dong, W.; Pei, Y.; et al. MoS2 quantum dots growth induced by S vacancy in ZnIn2S4 monolayer: Atomic-level heterostructure for photocatalytic hydrogen production. ACS Nano 2018, 12, 751–758. [Google Scholar] [CrossRef]
  82. Ottaviano, L.; Palleschi, S.; Perrozzi, F.; D’Olimpio, G.; Priante, F.; Donarelli, M.; Benassi, P.; Nardone, M.; Gonchigsuren, M.; Gombosuren, M.; et al. Mechanical exfoliation and layer number identification of MoS2 revisited. 2D Mater. 2017, 4, 5013. [Google Scholar] [CrossRef]
  83. Lin, H.; Wang, J.; Luo, Q.; Peng, H.; Luo, C.; Qi, R.; Huang, R.; Travas-Sejdic, J.; Duan, C.G. Rapid and highly efficient chemical exfoliation of layered MoS2 and WS2. J. Alloys Compd. 2017, 699, 222–229. [Google Scholar] [CrossRef]
  84. Liu, N.; Kim, P.; Kim, J.H.; Ye, J.H.; Kim, S.; Lee, C.J. Large-Area Atomically Thin MoS2 Nanosheets Prepared Using Electrochemical Exfoliation. ACS Nano 2014, 8, 6902–6910. [Google Scholar] [CrossRef] [PubMed]
  85. Gupta, A.; Arunachalam, V.; Vasudevan, S. Liquid-Phase Exfoliation of MoS2 Nanosheets: The Critical Role of Trace Water. J. Phys. Chem. Lett. 2016, 7, 4884–4890. [Google Scholar] [CrossRef] [PubMed]
  86. Liu, H.; Li, Y.; Xiang, M.; Zeng, H.; Shao, X. Single-layered MoS2 directly grown on rutile TiO2 (110) for enhanced interfacial charge transfer. ACS Nano 2019, 13, 6083–6089. [Google Scholar] [CrossRef]
  87. Wang, Q.H.; Kalantar-Zadeh, K.; Kis, A.; Coleman, J.N.; Strano, M.S. Electronics and optoelectronics of two-dimensional transition metal dichalcogenides. Nat. Nanotechnol. 2012, 7, 699–712. [Google Scholar] [CrossRef]
  88. Li, H.; Wu, J.; Huang, X.; Lu, G.; Yang, J.; Lu, X.; Xiong, Q.H.; Zhang, H. Rapid and reliable thickness identification of twodimensional nanosheets using optical microscopy. ACS Nano 2013, 7, 10344–10353. [Google Scholar] [CrossRef] [Green Version]
  89. Gao, E.; Lin, S.Z.; Qin, Z.; Buehler, M.J.; Feng, X.Q.; Xu, Z. Mechanical exfoliation of two-dimensional materials. J. Mech. Phys. Solids 2018, 115, 248–262. [Google Scholar] [CrossRef]
  90. Rigos, A.F.; Hill, H.M.; Li, Y.L.; Chernikov, A.; Heinz, T.F. Probing Interlayer Interactions in Transition Metal Dichalcogenide Heterostructures by Optical Spectroscopy: MoS2/WS2 and MoSe2/WSe2. Nano Lett. 2015, 15, 5033–5038. [Google Scholar] [CrossRef]
  91. DiCamillo, K.; Krylyuk, S.; Shi, W.; Davydov, A.; Paranjape, M. Automated Mechanical Exfoliation of MoS2 and MoTe2 Layers for 2D Materials Applications. IEEE Trans. Nanotechnol. 2019, 18. [Google Scholar] [CrossRef]
  92. Li, H.; Yu, K.; Li, C.; Guo, B.; Lei, X.; Fu, H.; Zhu, Z. Novel dual-petal nanostructured WS2@MoS2 with enhanced photocatalytic performance and a comprehensive first-principles investigation. J. Mater. Chem. A 2015, 3, 20225. [Google Scholar] [CrossRef]
  93. Krishnamoorthy, K.; Pazhamalai, P.; Veerasubramani, G.K.; Kim, S.J. Mechanically delaminated few layered MoS2 nanosheets based high performance wire type solid-state symmetric supercapacitors. J. Power Sources 2016, 321, 112–119. [Google Scholar] [CrossRef]
  94. Delogu, F.; Gorrasi, G.; Sorrentino, A. Fabrication of polymer nanocomposites via ball milling: Present status and future perspectives. Prog. Mater. Sci. 2017, 86, 75–126. [Google Scholar] [CrossRef]
  95. Cantarella, M.; Gorrasi, G.; Mauro, A.D.; Scuderi, M.; Nicotra, G.; Fiorenza, R.; Scirè, S.; Scalisi, M.E.; Brundo, M.V.; Privitera, V.; et al. Mechanical milling: A sustainable route to induce structural transformations in MoS2 for applications in the treatment of contaminated water. Sci. Rep. 2019, 9, 974. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  96. Kumar, S.; Kumar, V.; Devi, R.; Sisodia, A.K.; Jatrana, A.; Singh, R.B.; Dahiya, R.; Mishra, A.K. Sustainable and Scalable Approach for Enhancing the Electrochemical Performance of Molybdenum Disulfide (MoS2). Adv. Mater. Sci. Eng. 2022, 2022, 1288623. [Google Scholar] [CrossRef]
  97. Shi, D.; Yang, M.; Chang, B.; Ai, Z.; Zhang, K.; Shao, Y.; Wang, S.; Wu, Y.; Hao, X. Ultrasonic-Ball Milling: A Novel Strategy to Prepare Large-Size Ultrathin 2D Materials. Small 2020, 16, 1906734. [Google Scholar] [CrossRef]
  98. Sahoo, D.; Kumar, B.; Sinha, J.; Ghosh, S.; Roy, S.S.; Kaviraj, B. Cost effective liquid phase exfoliation of MoS2 nanosheets and photocatalytic activity for wastewater treatment enforced by visible light. Sci. Rep. 2020, 10, 10759. [Google Scholar] [CrossRef]
  99. Kumar, R.R.; Habib, M.R.; Khan, A.; Chen, P.C.; Murugesan, T.; Gupta, S.; Anbalagan, A.K.; Tai, N.H.; Lee, C.H.; Lin, H.N. Sulfur Monovacancies in Liquid-Exfoliated MoS2 Nanosheets for NO2 Gas Sensing. ACS Appl. Nano Mater. 2021, 4, 9459–9470. [Google Scholar] [CrossRef]
  100. Chen, I.-W.P.; Lai, Y.-M.; Liao, W.-S. One-Pot Synthesis of Chlorophyll-Assisted Exfoliated MoS2/WS2 Heterostructures via Liquid-Phase Exfoliation Method for Photocatalytic Hydrogen Production. Nanomaterials 2021, 11, 2436. [Google Scholar] [CrossRef]
  101. Gan, X.; Zhao, H.; Lei, D.; Wang, P. Improving electrocatalytic activity of 2H-MoS2 nanosheets obtained by liquid phase exfoliation: Covalent surface modification versus interlayer interaction. J. Catal. 2020, 391, 424–434. [Google Scholar] [CrossRef]
  102. Liu, Y.; He, X.; Hanlon, D.; Harvey, A.; Coleman, J.N.; Li, Y. Liquid Phase Exfoliated MoS2 Nanosheets Percolated with Carbon Nanotubes for High Volumetric/Areal Capacity Sodium-Ion Batteries. ACS Nano 2016, 10, 8821–8828. [Google Scholar] [CrossRef]
  103. Liu, J.; Liu, H.; Peng, W.; Li, Y.; Zhang, F.; Fan, X. High-yield exfoliation of MoS2 (WS2) monolayers towards efficient photocatalytic hydrogen evolution. Chem. Eng. J. 2022, 431, 133286. [Google Scholar] [CrossRef]
  104. Sun, J.; Li, X.; Guo, W.; Zhao, M.; Fan, X.; Dong, Y.; Xu, C.; Deng, J.; Fu, Y. Synthesis Methods of Two-Dimensional MoS2: A Brief Review. Crystals 2017, 7, 198. [Google Scholar] [CrossRef] [Green Version]
  105. Zhang, H. Ultrathin two-dimensional nanomaterials. ACS Nano 2015, 9, 9451–9469. [Google Scholar] [CrossRef] [PubMed]
  106. Zhan, Y.; Liu, Z.; Najmaei, S.; Ajayan, P.M.; Lou, J. Large-areavapor-phase growth and characterization of MoS2 atomic layers on aSiO2 substrate. Small 2012, 8, 966–971. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  107. Ambrosi, A.; Sofer, Z.; Pumera, M. 2H→1T phase transition and hydrogen evolution activity of MoS2, MoSe2, WS2 and WSe2 strongly depends on the MX2 composition. Chem Comm. 2015, 51, 8450–8453. [Google Scholar] [CrossRef]
  108. Voiry, D.; Goswami, A.; Kappera, R.; Silva, C.d.C.C.e.; Kaplan, D.; Fujita, T.; Chen, M.; Asefa, T.; Chhowalla, M. Covalentfunctionalization of monolayered transition metal dichalcogenides by phase engineering. Nat. Chem. 2015, 7, 45–49. [Google Scholar] [CrossRef]
  109. Shi, S.; Sun, Z.; Hu, Y.H. Synthesis, stabilization and applications of 2-dimensional 1T metallic MoS2. J. Mater. Chem. A 2018, 6, 23932–23977. [Google Scholar] [CrossRef]
  110. Hong, S.; Krishnamoorthy, A.; Rajak, P.; Tiwari, S.; Misawa, M.; Shimojo, F.; Kalia, R.K.; Nakano, A.; Vashishta, P. Computational synthesis of MoS2 layers by reactive molecular dynamics simulations: Initial sulfidation of MoO3 surfaces. Nano Lett. 2017, 17, 4866–4872. [Google Scholar] [CrossRef]
  111. Hong, S.; Sheng, C.; Krishnamoorthy, A.; Rajak, P.; Tiwari, S.; Nomura, K.I.; Misawa, M.; Shimojo, F.; Kalia, R.K.; Nakano, A.; et al. Chemical vapor deposition synthesis of MoS2 layers from the direct sulfidation of MoO3 surfaces using reactive molecular dynamics simulations. J. Phys. Chem. C 2018, 122, 7494–7503. [Google Scholar] [CrossRef]
  112. Park, W.; Park, J.; Jang, J.; Lee, H.; Jeong, H.; Cho, K.; Hong, S.; Lee, T. Oxygen environmental and passivation effects on molybdenum disulfide field effect transistors. Nanotechnology 2013, 24, 095202. [Google Scholar] [CrossRef]
  113. Qiu, H.; Pan, L.; Yao, Z.; Li, J.; Shi, Y.; Wang, X. Electrical characterization of back-gated bi-layer MoS2field-effect transistors and the effect of ambient on their performances. Appl. Phys. Lett. 2012, 100, 123104. [Google Scholar] [CrossRef]
  114. Choudhary, N.; Park, J.; Hwang, J.Y.; Choi, W. Growth of large-scale and thickness-modulated MoS2nanosheets. ACS Appl. Mater. Interfaces 2014, 6, 21215–21222. [Google Scholar] [CrossRef] [PubMed]
  115. Rovira, M.A.D.; Samaniego-Benitez, J.E.; Ramírez-Aparicio, J.; León-Sarabia, E.; Moreno-Bárcenas, A.; Garcia-Garcia, A. Synthesis of MoS2 ribbons with “thorns” by CVD process. Mater. Lett. 2022, 320, 132355. [Google Scholar] [CrossRef]
  116. Chiawchan, T.; Ramamoorthy, H.; Buapan, K.; Somphonsane, R. CVD Synthesis of Intermediate State-Free, Large-Area and Continuous MoS2 via Single-Step Vapor-Phase Sulfurization of MoO2 Precursor. Nanomaterials 2021, 11, 2642. [Google Scholar] [CrossRef]
  117. Mawlong, L.P.; Biroju, R.K.; Giri, P.K. Low-Temperature Chemical Vapor Deposition Growth of MoS2Nanodots and Their Raman and Photoluminescence Profiles. Front. Nanotech. 2021, 3, 775732. [Google Scholar] [CrossRef]
  118. Almohaimeed, Z.M.; Karamat, S.; Akram, R.; Sarwar, S.; Javaid, A.; Oral, A. An Effective Route for the Growth of Multilayer MoS2 by Combining Chemical Vapor Deposition and Wet Chemistry. Adv. Condens. Matter Phys. 2022, 2022, 1687–8108. [Google Scholar] [CrossRef]
  119. Vishwanath, S.; Liu, X.; Rouvimov, S.; Mende, P.; Azcatl, A.; McDonnell, S.; Wallace, R.; Feenstra, R.; Furdyna, J.; Jena, D.; et al. Comprehensive structural and optical characterization of MBE grown MoSe2 on graphite, CaF2 and graphene. 2D Mater. 2015, 2, 024007. [Google Scholar] [CrossRef]
  120. Qin, X.; Ke, P.; Wang, A.; Kim, K. Microstructure, mechanical and tribological behaviors of MoS2-Ti composite coatings deposited by a hybrid HIPIMS method. Surf. Coat. Technol. 2013, 228, 275–281. [Google Scholar] [CrossRef]
  121. Muratore, C.; Hu, J.J.; Wang, B.; Haque, M.A.; Bultman, J.E.; Jespersen, M.L.; Shamberger, P.J.; McConney, M.E.; Naguy, R.D.; Voevodin, A.A. Continuous ultra-thin MoS2 films grown by low-temperature physical vapor deposition. Appl. Phys. Lett. 2014, 104, 261604. [Google Scholar] [CrossRef] [Green Version]
  122. Feng, Q.; Mao, N.; Wu, J.; Xu, H.; Wang, C.; Zhang, J.; Xie, L. Growth of MoS2(1–x)Se2x (x = 0.41 − 1) Monolayer Alloys with Controlled Morphology by Physical Vapor Deposition. ACS Nano 2015, 9, 7450–7455. [Google Scholar] [CrossRef]
  123. Gong, C.; Huang, C.; Miller, J.; Cheng, L.; Hao, Y.; Cobden, D.; Kim, J.; Ruoff, R.S.; Wallace, R.M.; Cho, K.; et al. Metal Contacts on Physical Vapor Deposited Monolayer MoS2. ACS Nano 2013, 7, 11350–11357. [Google Scholar] [CrossRef] [PubMed]
  124. Jamkhande, P.G.; Ghule, N.W.; Bamer, A.H.; Kalaskar, M.G. Metal nanoparticles synthesis: An overview on methods of preparation, advantages and disadvantages, and applications. J. Drug Deliv. Sci. Technol. 2019, 53, 101174. [Google Scholar] [CrossRef]
  125. Asim, N.; Ahmadi, S.; Alghoul, M.A.; Hammadi, F.Y.; Saeedfar, K.; Sopian, K. Research and development aspects on chemical preparation techniques of photo anodes for dye sensitized solar cells. Int. J. Photoenergy 2014, 2014, 518156. [Google Scholar] [CrossRef] [Green Version]
  126. Lei, X.; Yu, K.; Qi, R.; Zhu, Z. Fabrication and theoretical investigation of MoS2-Co3S4 hybrid hollow structure as electrode material for lithium-ion batteries and supercapacitors. Chem. Eng. J. 2018, 347, 607–617. [Google Scholar] [CrossRef]
  127. Wen, S.; Liu, Y.; Zhu, F.; Shao, R.; Xu, W. Hierarchical MoS2 nanowires/NiCo2O4 nanosheets supported on Ni foam for highperformance asymmetric supercapacitors. Appl. Surf. Sci. 2018, 428, 616–622. [Google Scholar] [CrossRef]
  128. Wang, M.; Li, G.; Xu, H.; Qian, Y.; Yang, J. Enhanced lithium storage performances of hierarchical hollow MoS2 nanoparticles assembled from nanosheets. ACS Appl. Mater. Interfaces 2013, 5, 1003–1008. [Google Scholar] [CrossRef]
  129. Wang, P.P.; Sun, H.; Ji, Y.; Li, W.; Wang, X. Three dimensional assembly of single layered MoS2. Adv. Mater. 2014, 26, 964–969. [Google Scholar] [CrossRef]
  130. Ramakrishna Matte, H.; Gomathi, A.; Manna, A.K.; Late, D.J.; Datta, R.; Pati, S.K.; Rao, C. MoS2 and WS2 analogues of graphene. Angew. Chem. Int. Ed. 2010, 122, 4153–4156. [Google Scholar] [CrossRef]
  131. Muralikrishna, S.; Manjunath, K.; Samrat, D.; Reddy, V.; Ramakrishnappa, T.; Nagaraju, D.H. Hydrothermal synthesis of 2D MoS2 nanosheets for electrocatalytic hydrogen evolution reaction. RSC Adv. 2015, 5, 89389–89396. [Google Scholar] [CrossRef]
  132. Fan, L.Q.; Liu, G.J.; Zhang, C.Y.; Wu, J.H.; Wei, Y.L. Facile one-step hydrothermal preparation of molybdenum disulfide/carbon composite for use in supercapacitor. Int. J. Hydrogen Energy 2015, 40, 10150–10157. [Google Scholar] [CrossRef]
  133. Ma, L.; Chen, W.X.; Li, H.; Zheng, Y.F.; Xu, Z.D. Ionic liquid-assisted hydrothermal synthesis of MoS2 microspheres. Mater. Lett. 2008, 62, 797–799. [Google Scholar] [CrossRef]
  134. Nagaraju, G.; Tharamani, C.N.; Chandrappa, G.T.; Livage, J. Hydrothermal synthesis of amorphous MoS2 nanofiber bundles via acidification of ammonium heptamolybdate tetrahydrate. Nanoscale Res. Lett. 2007, 2, 461–468. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  135. Luo, L.; Shi, M.; Zhao, S.; Tan, W.; Lin, X.; Wang, H.; Jiang, F. Hydrothermal synthesis of MoS2 with controllable morphologies and its adsorption properties for bisphenol A. J. Saudi Chem. Soc. 2019, 23, 762–773. [Google Scholar] [CrossRef]
  136. Mulu, M.; Devi, D.R.; Belachew, N.; Basavaiah, K. Hydrothermal green synthesis of MoS2 nanosheets for pollution abatement and antifungal applications. RSC Adv. 2021, 11, 24536–24542. [Google Scholar] [CrossRef] [PubMed]
  137. Mani, N.P.; Cyriac, J. Green approach to synthesize various MoS2 nanoparticles via hydrothermal process. Bull. Mater. Sci. 2022, 45, 184. [Google Scholar] [CrossRef]
  138. Cordeiro, N.J.A.; Gaspar, C.; Oliveira, M.J.D.; Nunes, D.; Barquinha, P.; Pereira, L.; Fortunato, E.; Martins, R.; Laureto, E.; Lourenço, S.A. Fast and Low-Cost Synthesis of MoS2 Nanostructures on Paper Substrates for Near-Infrared Photodetectors. Appl. Sci. 2021, 11, 1234. [Google Scholar] [CrossRef]
  139. Xuan, T.T.; Long, L.N.; Khai, T.V. Effect of reaction temperature and reaction time on the structure and properties of MoS2 synthesized by hydrothermal method. Vietnam. J. Chem. 2020, 58, 92–100. [Google Scholar] [CrossRef] [Green Version]
  140. Duraisamy, S.; Ganguly, A.; Sharma, P.K.; Benson, J.; Davis, J.; Papakonstantinou, P. One-Step Hydrothermal Synthesis of Phase-Engineered MoS2/MoO3 Electrocatalysts for Hydrogen Evolution Reaction. ACS Appl. Nano Mater. 2021, 4, 2642–2656. [Google Scholar] [CrossRef]
  141. Theerthagiri, J.; Senthil, R.A.; Senthilkumar, B.; Polu, A.R.; Madhavan, J.; Ashokkumar, M. Recent advances in MoS2 nanostructured materials for energy and environmental applications—A review. J. Solid State Chem. 2017, 252, 43–71. [Google Scholar] [CrossRef]
  142. Ahmaruzzaman, M.d.; Gadore, V. MoS2 based nanocomposites: An excellent material for energy and environmental applications. J. Environ. Chem. Eng. 2021, 9, 105836. [Google Scholar] [CrossRef]
  143. Saha, D.; Kruse, P.J. Editors’ Choice—Review—Conductive Forms of MoS2 and Their Applications in Energy Storage and Conversion. J. Electrochem. Soc. 2020, 167, 126517. [Google Scholar] [CrossRef]
  144. Li, X.; Li, T.; Huang, S.; Zhang, J.; Pam, M.E.; Yang, H.Y. Controllable Synthesis of Two-Dimensional Molybdenum Disulfide (MoS2) for Energy-Storage Applications. ChemSusChem 2020, 13, 1379–1391. [Google Scholar] [CrossRef] [PubMed]
  145. Wen, X.; Luo, J.; Xiang, K.; Zhou, W.; Zhang, C.; Chen, H. High-performance monoclinic WO3 nanospheres with the novel NH4+ diffusion behaviors for aqueous ammonium-ion batteries. Chem. Eng. J. 2023, 458, 141381. [Google Scholar] [CrossRef]
  146. Li, D.; Guo, H.; Jiang, S.; Zeng, G.; Zhou, W.; Li, Z. Microstructures and electrochemical performances of TiO2-coated Mg–Zr co-doped NCM as a cathode material for lithium-ion batteries with high power and long circular life. New J. Chem. 2021, 45, 19446–19455. [Google Scholar] [CrossRef]
  147. Zhou, W.; Zeng, G.; Jin, H.; Jiang, S.; Huang, M.; Zhang, C.; Chen, H. Bio-Template Synthesis of V2O3@Carbonized Dictyophora Composites for Advanced Aqueous Zinc-Ion Batteries. Molecules 2023, 28, 2147. [Google Scholar] [CrossRef]
  148. Yan, Q.; Yu, L.; Jingyi, L.; Cuihua, T.; Han, X.; Yiqiang, W. Research progress of wood-derived energy storage materials. J. For. Eng. 2021, 6, 1–13. [Google Scholar]
  149. Jiao, Y.; Hafez, A.M.; Cao, D.; Mukhopadhyay, A.; Ma, Y.; Zhu, H. Metallic MoS2 for High Performance Energy Storage and Energy Conversion. Small 2018, 14, 1800640. [Google Scholar] [CrossRef]
  150. Liu, X.; Wang, Y.; Yang, Y.; Lv, W.; Lian, G.; Golberg, D.; Wang, X.; Zhao, X.; Ding, Y. A MoS2/Carbon hybrid anode for high-performance Li-ion batteries at low temperature. Nano Energy 2020, 70, 104550. [Google Scholar] [CrossRef]
  151. Baheri, Y.T.; Maleki, M.; Karimian, H.; Javadpoor, J.; Masoudpanah, S.M. Well-distributed 1T/2H MoS2 nanocrystals in the N-doped nanoporous carbon framework by direct pyrolysis. Sci. Rep. 2023, 13, 7492. [Google Scholar] [CrossRef]
  152. Li, S.; Liu, P.; Huang, X.; Tang, Y.; Wang, H. Reviving the bulky MoS2 as advanced anode for lithium-ion batteries. J. Mater. Chem. A 2019, 7, 10988–10997. [Google Scholar] [CrossRef]
  153. Deng, C.; Wanga, H.; Wang, S. Clarifying the lithium storage behavior of MoS2 with in situ electrochemical impedance spectroscopy. J. Mater. Chem. A 2021, 9, 15734–15743. [Google Scholar] [CrossRef]
  154. Bozheyev, F.; Zhexembekova, A.; Zhumagali, S.; Molkenova, A.; Bakenov, Z. MoS2 nanopowder as anode material for lithium-ion batteries produced by self-propagating high-temperature synthesis. Mater. Today: Proc. 2017, 4, 4567–4571. [Google Scholar]
  155. George, C.; Morris, A.J.; Modarres, M.H.; De Volder, M. Structural Evolution of Electrochemically Lithiated MoS2 Nanosheets and the Role of Carbon Additive in Li-Ion Batteries. Chem. Mater. 2016, 28, 7304–7310. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  156. Santhosha, A.L.; Nayak, P.K.; Pollok, K.; Langenhorst, F.; Adelhelm, P. Exfoliated MoS2 as Electrode for All-Solid-State Rechargeable Lithium-Ion Batteries. J. Phys. Chem. C 2019, 123, 12126–12134. [Google Scholar] [CrossRef]
  157. Yang, F.; Feng, X.; Glans, P.A.; Guo, J. MoS2 for beyond lithium-ion batteries. APL Mater. 2021, 9, 050903. [Google Scholar] [CrossRef]
  158. Cha1, E.; Kim, D.K.; Choi, W. Advances of 2D MoS2 for High-Energy Lithium Metal Batteries. Front. Energy Res. 2021, 9, 645403. [Google Scholar] [CrossRef]
  159. Jiang, Y.; Wang, Y.; Ni, J.; Li, L. Molybdenum-based materials for sodium-ion batteries. InfoMat 2021, 3, 339–352. [Google Scholar] [CrossRef]
  160. Wu, J.; Liu, J.; Cui, J.; Yao, S.; Ihsan-Ul-Haq, M.; Mubarak, N.; Quattrocchi, E.; Ciucci, F.; Kim, J. Dual-Phase MoS2 as a High-Performance Sodium-Ion Battery Anode. J. Mater. Chem. A 2020, 8, 2114–2122. [Google Scholar] [CrossRef]
  161. Jang, J.; Jung, H.; Oh, S.M.; Heon, J. A comparative study of reaction mechanism of MoS2 negative electrode materials for sodium-ion batteries. J. Alloys Compd. 2021, 876, 160182. [Google Scholar] [CrossRef]
  162. Song, P.; Di, J.; Kang, L.; Xu, M.; Tang, B.; Xiong, J.; Cui, J.; Zeng, Q.; Zhou, J.; He, Y.; et al. Enhancing the cycling stability of Na-ion batteries by bonding MoS2 on assembled carbon-based materials. Nano Mater. Sci. 2019, 1, 310–317. [Google Scholar] [CrossRef]
  163. Li, W.; Bashir, T.; Wang, J.; Zhou, S.; Yang, S.; Zhao, J.; Gao, L. Enhanced Sodium-Ion Storage Performance of a 2D MoS2 Anode Material Coated on Carbon Nanotubes. ChemElectroChem 2021, 8, 903–910. [Google Scholar] [CrossRef]
  164. Ye, W.; Wu, F.; Shi, N.; Zhou, H.; Chi, Q.; Chen, W.; Du, S.; Gao, P.; Li, H.; Xiong, S. Metal–Semiconductor Phase Twinned Hierarchical MoS2 Nanowires with Expanded Interlayers for Sodium-Ion Batteries with Ultralong Cycle Life. Small 2019, 15, 1805405–1805410. [Google Scholar]
  165. Dai, H.; Tang, M.; Huang, J.; Wang, Z. A Series of Molecule-Intercalated MoS2 as Anode Materials for Sodium Ion Batteries. ACS Appl. Mater. Interfaces 2021, 13, 10870–10877. [Google Scholar] [CrossRef] [PubMed]
  166. Chothe, U.; Ugale, C.; Kulkarni, M.; Kale, B. Solid-State Synthesis of Layered MoS2 Nanosheets with Graphene for Sodium-Ion Batteries. Crystals 2021, 11, 660. [Google Scholar] [CrossRef]
  167. Halankar, K.K.; Mandal, B.P.; Tyagi, A.K. Superior electrochemical performance of MoS2 decorated on functionalized carbon nanotubes as anode material for sodium ion battery. Carbon Trends 2021, 5, 100103. [Google Scholar] [CrossRef]
  168. Naz, R.; Abbas, W.; Liu, Q.; Shafi, S.; Gull, S.; Khan, S.; Rasheed, T.; Song, G.; Gu, J. Covalent functionalization of electrochemically exfoliated 1T-MoS2 nanosheets for high-performance supercapacitor electrode. J. Alloys Compd. 2023, 951, 169944. [Google Scholar] [CrossRef]
  169. Sun, X.; Pang, Y.; Li, S.; Yu, Y.; Ding, X.; Wang, L.; Zhang, Q. High performance asymmetric supercapacitor based on 3D microsphere-like 1T-MoS2 with high 1T phase content. Ceram. Int. 2022, 48, 21317–21326. [Google Scholar] [CrossRef]
  170. Zarach, Z.; Szkoda, M.; Trzciński, K.; Łapiński, M.; Trykowski, G.; Nowak, A. The phenomenon of increasing capacitance induced by 1T/2H-MoS2 surface modification with Pt particles—Influence on composition and energy storage mechanism. Electrochim. Acta 2022, 435, 141389. [Google Scholar] [CrossRef]
  171. Shrivastav, M.; Singh Kushwaha, H.; Dhiman, R. 2H-MoS2 as an electrode material for oxygen reduction reaction and supercapacitor applications. Mater. Today Proc. 2022, in press. [Google Scholar] [CrossRef]
  172. Arun Kumar, M.; Shanmugavel, C.; Hanagata, N.; Jayavel, R. Simplified detection of the hybridized DNA using a graphene field effect transistor. Sci. Tech. Adv. Mater. 2017, 18, 43–50. [Google Scholar]
  173. Arun Kumar, M.; Jayavel, R.; Shanmugam, M.; Sengottaiyan, C.; Chinnathambi, S.; Mohankumar, N. A compact sensory platform-based pH sensor using graphene field effect transistor. J. Nanosci. Nanotechnol. 2021, 21, 3299–3305. [Google Scholar] [CrossRef] [PubMed]
  174. Kumar, M.A.; Jayavel, R.; Arivanandhan, M.; Raj, B.; Mohankumar, N. Performance Enhancement and Comparison of Graphene Field Effect Transistor Devices Coated with HMDS Layer. Silicon 2022, 14, 10467–10474. [Google Scholar] [CrossRef]
  175. Ramakrishnan, K.; Nithya, C.; Karvembu, R. Heterostructure of two different 2D materials based on MoS2 nanoflowers@rGO: An electrode material for sodium-ion capacitors. Nanoscale Adv. 2019, 1, 334–341. [Google Scholar] [CrossRef] [Green Version]
  176. Zhan, C.; Liu, W.; Hu, M.; Liang, Q.; Yu, X.; Shen, Y.; Lv, R.; Kang, F.; Huang, Z.H. High-performance sodium-ion hybridcapacitors based on an interlayer-expanded MoS2/rGO composite: Surpassing the performance of lithium-ion capacitors in a uniform system. NPG Asia Mater. 2018, 10, 775. [Google Scholar] [CrossRef]
  177. Ji, H.; Hu, S.; Jiang, Z.; Shi, S.; Hou, W.; Yang, G. Directly scalable preparation of sandwiched MoS2/graphene nanocomposites via ball-milling with excellent electrochemical energy storage performance. Electrochim. Acta 2019, 299, 143–151. [Google Scholar] [CrossRef]
  178. Quan, T.; Goubard-Bretesche, N.; Hark, E.; Kochovski, Z.; Mei, S.; Pinna, N.; Ballauff, M.; Lu, Y. Highly Dispersible Hexagonal Carbon−MoS2−Carbon Nanoplates with Hollow Sandwich Structures for Supercapacitors. Chem. Eur. J. 2019, 25, 4757–4766. [Google Scholar] [CrossRef]
  179. Chen, X.; Ding, J.; Jiang, J.; Zhuang, G.; Zhang, Z.; Yang, P. Preparation of a MoS2/carbon nanotube composite as an electrode material for high-performance supercapacitors. RSC Adv. 2018, 8, 29488–29494. [Google Scholar] [CrossRef] [Green Version]
  180. Mahajan, H.; Mohanan, K.; Cho, S. Facile Synthesis of Biocarbon-Based MoS2 Composite for High-Performance Supercapacitor Application. Nano Lett. 2022, 22, 8161–8167. [Google Scholar] [CrossRef]
  181. Zhang, Y.; He, T.; Liu, G.; Zu, L.; Yang, J. One-pot mass preparation of MoS2/C aerogels for high-performance supercapacitors and lithium-ion batteries. Nanoscale 2017, 9, 10059–10066. [Google Scholar] [CrossRef]
  182. Farshadnia, M.; Ensafi, A.; Zarean, M.; Rezaei, B. Design and synthesis of three-dimensional CoNi2S4@MoS2@rGO nanocomposites and its application in electrochemical supercapacitors. J. Alloys Compd. 2022, 906, 164278. [Google Scholar] [CrossRef]
  183. Fang, L.; Qiu, Y.; Zhai, T.; Wang, F.; Lan, M.; Huang, K.; Jing, Q. Flower-like nanoarchitecture assembled from Bi2S3 nanorod/MoS2 nanosheet heterostructures for high-performance supercapacitor electrodes. Colloids Surf. 2017, 535, 41–48. [Google Scholar] [CrossRef]
  184. Wang, B.; Hu, R.; Zhang, J.; Huang, Z.; Qiao, H.; Gong, L.; Qi, X. 2D/2D SnS2/MoS2 layered heterojunction for enhanced supercapacitor performance. J. Am. Ceram. 2020, 103, 1088–1096. [Google Scholar] [CrossRef]
  185. Govindan, R.; Hong, X.; Sathishkumar, P.; Cai, Y.; Gu, F. Construction of metal-organic framework-derived CeO2/C integrated MoS2 hybrid for high-performance asymmetric supercapacitor. Electrochim. Acta 2020, 353, 136502. [Google Scholar] [CrossRef]
  186. Chiu, S.-K.; Chen, P.-Y.; Louh, R.-F. Electrochemically Deposited MoS2 and MnS Multilayers on Nickel Substrates in Inverse Opal Structure as Supercapacitor Microelectrodes. Micromachines 2023, 14, 361. [Google Scholar] [CrossRef]
  187. Tue, L.N.M.; Sahoo, S.; Dhakal, G.; Nguyen, V.H.; Lee, J.; Lee, Y.R.; Shim, J.-J. NiCo2S4/MoS2 Nanocomposites for Long-Life High-Performance Hybrid Supercapacitors. Nanomaterials 2023, 13, 689. [Google Scholar] [CrossRef]
  188. Chen, Q.; Xie, F.; Wang, G.; Ge, K.; Ren, H.; Yan, M.; Wang, Q.; Bi, H. Hybrid MoS2@PANI materials for high-performance supercapacitor electrode. Ionics 2021, 27, 4083–4096. [Google Scholar] [CrossRef]
  189. Suresh, S.; Sindhu, V. CeO2/PANI/MoS2 composite electrode for symmetric supercapacitor application. J. Indian Chem. Soc. 2022, 99, 100727. [Google Scholar] [CrossRef]
  190. Ren, L.; Zhang, G.; Lei, J.; Hu, D.; Dou, S.; Gu, H.; Li, H.; Zhang, X. Growth of PANI thin layer on MoS2 nanosheet with high electro-capacitive property for symmetric supercapacitor. J. Alloys Compd. 2019, 798, 227–234. [Google Scholar] [CrossRef]
  191. Ganesha, H.; Veeresh, S.; Nagaraju, Y.S.; Vandana, M.; Ashokkumar, S.P.; Vijeth, H.; Devendrappa, H. Growth of 3-Dimentional MoS2-PANI nanofiber for high electrochemical performance. Mater. Res. Express 2020, 8, 084001. [Google Scholar] [CrossRef]
  192. Hu, L.; Wu, H.; La Mantia, F.; Yang, Y.; Cui, Y. Thin, flexible secondary Li-ion paper batteries. ACS Nano 2010, 4, 5843–5848. [Google Scholar] [CrossRef]
  193. Liu, B.; Zhang, J.; Wang, X.; Chen, G.; Chen, D.; Zhou, C.; Shen, G. Hierarchical three-dimensional ZnCo2O4 nanowire arrays/carbon cloth anodes for a novel class of high-performance flexible lithium-ion batteries. Nano Lett. 2012, 12, 3005–3011. [Google Scholar] [CrossRef]
  194. Peng, X.; Peng, L.; Wu, C.; Xie, Y. Two dimensional nanomaterials for flexible supercapacitors. Chem. Soc. Rev. 2014, 43, 3303–3323. [Google Scholar] [CrossRef]
  195. Chee, W.K.; Lim, H.N.; Zainal, Z.; Huang, N.M.; Harrison, I.; Andou, Y. Flexible Graphene-Based Supercapacitors: A Review. J. Phys. Chem. C 2016, 120, 4153–4172. [Google Scholar] [CrossRef]
  196. Cherusseri, J.; Choudhary, N.; Kumar, K.S.; Jung, Y.; Thomas, J. Recent trends in transition metal dichalcogenide based supercapacitor electrodes. Nanoscale Horiz. 2019, 4, 840–858. [Google Scholar] [CrossRef]
  197. Wu, X.; Xu, Y.; Hu, Y.; Wu, G.; Cheng, H.; Yu, Q.; Zhang, K.; Chen, W.; Chen, S. Microfluidic-spinning construction of black-phosphorus-hybrid microfibres for non-woven fabrics toward a high energy density flexible supercapacitor. Nat. Commun. 2018, 9, 4573. [Google Scholar] [CrossRef] [Green Version]
  198. Yang, Y.; Huang, Q.; Niu, L.; Wang, D.; Yan, C.; She, Y.; Zheng, Z. Waterproof, Ultrahigh Areal-Capacitance, Wearable Supercapacitor Fabrics. Adv. Mater. 2017, 29, 1606679. [Google Scholar] [CrossRef] [PubMed]
  199. Lyu, S.; Chang, H.; Fu, F.; Hu, L.; Huang, J.; Wang, S. Cellulose-coupled graphene/polypyrrole composite electrodes containing conducting networks built by carbon fibers as wearable supercapacitors with excellent foldability and tailorability. J. Power Sources 2016, 327, 438–446. [Google Scholar] [CrossRef]
  200. Wu, Q.; Xu, Y.; Yao, Z.; Liu, A.; Shi, G. Supercapacitors based on flexible graphene/polyanilinenanofiber composite films. ACS Nano 2010, 4, 1963–1970. [Google Scholar] [CrossRef]
  201. Kou, L.; Huang, T.; Zheng, B.; Han, Y.; Zhao, X.; Gopalsamy, K.; Sun, H.; Gao, C. Coaxial wet-spun yarn supercapacitors for highenergy density and safe wearable electronics. Nat. Commun. 2014, 5, 3754. [Google Scholar] [CrossRef] [Green Version]
  202. Gopalakrishnan, A.; Badhulika, S. Flexible supercapacitors based on 2D materials. Fundam. Supercapacitor Appl. 2d Mater. 2021, 10, 253–310. [Google Scholar]
  203. Mohan, M.; Shetti, N.P.; Aminabhavi, T.M. Recent developments in MoS2-based flexible supercapacitors. Mater. Today Chem. 2023, 27, 101333. [Google Scholar] [CrossRef]
  204. Manuraj, M.; Nair, K.K.; Unni, K.N.; Rakhi, R.B. High performance supercapacitors based on MoS2 nanostructures with near commercial mass loading. J. Alloys Compd. 2020, 819, 152963. [Google Scholar] [CrossRef]
  205. Qian, Y.; Lyu, Z.; Zhang, Q.; Lee, T.H.; Kang, T.K.; Sohn, M.; Shen, L.; Kim, D.H.; Kang, D.J. High-Performance Flexible Energy Storage Devices Based on Graphene Decorated with Flower-Shaped MoS2 Heterostructures. Micromachines 2023, 14, 297. [Google Scholar] [CrossRef]
  206. Chang, H.; Zhang, L.; Lyu, S.; Wang, S. Flexible and Freestanding MoS2 Nanosheet/Carbon Nanotube/Cellulose Nanofibril Hybrid Aerogel Film for High-Performance All-Solid-State Supercapacitors. ACS Omega 2022, 7, 14390–14399. [Google Scholar] [CrossRef] [PubMed]
  207. Li, B.; Liang, X.; Li, G.; Shao, F.; Xia, T.; Xu, S.; Hu, N.; Su, Y.; Yang, Z.; Zhang, Y. Inkjet printed ultrathin MoS2-based electrodes for flexible in-plane microsupercapacitors. ACS Appl. Mater. Interfaces 2020, 12, 39444–39454. [Google Scholar] [CrossRef]
  208. Chen, X.; Wang, S.; Shi, J.; Du, X.; Cheng, Q.; Xue, R.; Wang, Q.; Wang, M.; Ruan, L.; Zeng, W. Direct laser etching free-standing MXene-MoS2 film for highly flexible micro-supercapacitor. Adv. Mater. Interfaces 2019, 6, 1901160. [Google Scholar] [CrossRef]
  209. Raman, V.; Rhee, D.; Selvaraj, A.R.; Kim, J.; Prabakar, K.; Kang, J.; Kim, H.K. High performance flexible transparent micro-supercapacitors from nanocomposite electrodes encapsulated with solution processed MoS2 nanosheets. Sci. Technol. Adv. Mater. 2021, 22, 875–884. [Google Scholar] [CrossRef]
  210. Wu, H.; Guo, Z.; Li, M.; Hu, G.; Tang, T.; Wen, J.; Li, X.; Huang, H. Enhanced pseudocapacitive performance of MoS2 by introduction of both N-GQDs and HCNT for flexible supercapacitors. Electrochim. Acta 2021, 370, 137758. [Google Scholar] [CrossRef]
  211. Jiang, Z.; Zhai, S.; Huang, M.; Songsiriritthigul, P.; Aung, S.H.; Oo, T.Z.; Luo, M.; Chen, F. 3D carbon nanocones/metallic MoS2 nanosheet electrodes towards flexible supercapacitors for wearable electronics. Energy 2021, 227, 120419. [Google Scholar] [CrossRef]
  212. Pi, X.; Sun, X.; Wang, R.; Chen, C.; Wu, S.; Zhan, F.; Zhong, J.; Wang, Q.; Ostrikov, K.K. MoS2 nanosheets on plasma-nitrogen-doped carbon cloth for high-performance flexible supercapacitors. J. Colloid Interface Sci. 2023, 629, 227–237. [Google Scholar] [CrossRef]
  213. Zhang, G.; Zhu, R.; Zhang, R.; Zhang, D.; Sun, C.; Long, Z.; Li, Y. 3D hetero-nanostructured electrode constructed on carbon fiber paper with 2D 1T-MoS2/1D Cu(OH)2 for flexible asymmetric solid-state supercapacitors. J. Power Sources 2022, 523, 231031. [Google Scholar] [CrossRef]
  214. Sharma, G.K.; Ranjan, B.; Kaur, D. Electrochemical kinetics of 2D-MoS2 sputtered over stainless-steel mesh: Insights into the Na+ ions storage for flexible supercapacitors. Ceram. Int. 2022, 48, 23404–23414. [Google Scholar] [CrossRef]
  215. Sharma, G.K.; Ranjan, B.; Kaur, D. Estimating Li-ion storage in semiconducting nanocomposite of 2D-MoS2 decorated aluminum nitride nanoflowers for flexible electrodes of supercapacitors. Appl. Phys. Lett. 2022, 121, 013901. [Google Scholar] [CrossRef]
  216. Li, Y.; Wang, H.; Shu, T.; Yuan, J.; Lu, G.; Lin, B.; Gao, Z.; Wei, F.; Ma, C.; Qi, J.; et al. Two-dimensional hierarchical MoS2 lamella inserted in CoS2 flake as an advanced supercapacitor electrode. J. Energy Storage 2022, 51, 104299. [Google Scholar] [CrossRef]
  217. Sharma, G.K.; Ranjan, B.; Kaur, D. Two-dimensional MoS2 reinforced with Cu3N nanoflakes prepared via binder less sputtering route for flexible supercapacitor electrodes. Appl. Phys. Lett. 2021, 118, 203901. [Google Scholar] [CrossRef]
  218. Chen, I.; Chou, Y.; Wang, P. Integration of Ultrathin MoS2/PANI/CNT Composite Paper in Producing All-Solid-State Flexible Supercapacitors with Exceptional Volumetric Energy Density. J. Phys. Chem. C 2019, 123, 17864–17872. [Google Scholar] [CrossRef]
  219. Wu, W.; Wang, L.; Li, Y.; Zhang, F.; Lin, L.; Niu, S.; Chenet, D.; Zhang, X.; Hao, Y.; Heinz, T.F.; et al. Piezoelectricity of single-atomic-layer MoS2 for energy conversion and piezotronics. Nature 2014, 514, 470–474. [Google Scholar] [CrossRef] [PubMed]
  220. Kumar, S.; Kaur, N.; Bhullar, V.; Mahajan, A. MoS2 nanorods anchored reduced graphene oxide nanohybrids for electrochemical energy conversion applications. Physica E Low Dimens. Syst. Nanostruct. 2021, 128, 114589. [Google Scholar] [CrossRef]
  221. Hiragond, C.B.; Kim, H.; Lee, J.; Sorcar, S.; Erkey, C.; In, S.I. Electrochemical CO2 Reduction to CO Catalyzed by 2D Nanostructures. Catalysts 2020, 10, 98. [Google Scholar] [CrossRef] [Green Version]
  222. Asadi, M.; Kumar, B.; Behranginia, A.; Rosen, B.A.; Baskin, A.; Repnin, N.; Pisasale, D.; Phillips, P.; Zhu, W.; Haasch, R.; et al. Robust Carbon Dioxide Reduction on Molybdenum Disulphide Edges. Nat. Commun. 2014, 5, 4470. [Google Scholar] [CrossRef] [Green Version]
  223. Kumar, K.; Jamnuch, S.; Majidi, L.; Misal, S.; Ahmadiparidari, A.; Dato, M.A.; Sterbinsky, G.E.; Wu, T.; Salehi-Khojin, A.; Pascal, T.A.; et al. Active States During the Reduction of CO2 by a MoS2 Electrocatalyst. J. Phys. Chem. Lett. 2023, 14, 3222–3229. [Google Scholar] [CrossRef] [PubMed]
  224. Linghu, Y.; Tong, T.; Li, C.; Wu, C. The catalytic mechanism of CO2 electrochemical reduction over transition metal-modified 1T’-MoS2 monolayers. Appl. Surf. Sci. 2022, 590, 153001. [Google Scholar] [CrossRef]
  225. Xie, Y.; Li, X.; Wang, Y.; Li, B.; Yang, L.; Zhao, N.; Liu, M.; Wang, X.; Yu, Y.; Liu, J.M. Reaction mechanisms for reduction of CO2 to CO on monolayer MoS2. Appl. Surf. Sci. 2020, 499, 143964. [Google Scholar] [CrossRef]
  226. Francis, S.A.; Velazquez, J.M.; Ferrer, I.M.; Torelli, D.A.; Guevarra, D.; McDowell, M.T.; Sun, K.; Zhou, X.; Saadi, F.H.; John, J.; et al. Reduction of Aqueous CO2 to 1-Propanol at MoS2 Electrodes. Chem. Mater. 2018, 30, 4902–4908. [Google Scholar] [CrossRef] [Green Version]
  227. Khan, H.; Kang, S.; Charles, H.; Lee, C.S. Epitaxial Growth of Flower-Like MoS2 on One-Dimensional Nickel Titanate Nanofibers: A “Sweet Spot” for Efficient Photoreduction of Carbon Dioxide. Front. Chem. 2022, 10, 837915. [Google Scholar] [CrossRef]
  228. Al-Ghiffari, A.D.; Ludin, N.A.; Davies, M.L.; Yunus, R.M.; Suait, M.S. Systematic review of molybdenum disulfide for solar cell applications: Properties, mechanism and application. Mater. Today Commun. 2022, 32, 104078. [Google Scholar] [CrossRef]
  229. Tsai, M.; Su, S.; Chang, J.K.; Tsai, D.S.; Chen, C.H.; Wu, C.I.; Li, L.J.; Chen, L.J.; He, J.H. Monolayer MoS2 Heterojunction Solar Cells. ACS Nano 2014, 8, 8317–8322. [Google Scholar] [CrossRef] [PubMed]
  230. Xu, H.; Xin, L.; Liu, L.; Pang, D.; Jiao, Y.; Cong, R.; Yu, W. Large area MoS2/Si heterojunction-based solar cell through sol-gel method. Mater. Lett. 2019, 238, 13–16. [Google Scholar] [CrossRef]
  231. Singh, R.; Giri, A.; Pal, M.; Thiyagarajan, K.; Kwak, J.; Lee, J.J.; Jeong, U.; Cho, K. Perovskite solar cells with an MoS2 electron transport layer. J. Mater. Chem. A 2019, 7, 7151–7158. [Google Scholar] [CrossRef]
  232. Iqbal, T.; Ahsan, S.; Saeed, F.; Sultan, M.S.; AlObaid, A.A.; Warad, I.; Masood, A. Improved Efficiency of MoS2-Au Multilayer Plasmonic-Based Solar Cells: Far- and Near-Field Analysis. Plasmonics 2023, 38, 1–11. [Google Scholar] [CrossRef]
  233. Sattari, F.; Mirershadi, S. Enhancement of absorption in a CH3NH3PbI3-based photonic crystal in the presence of the monolayer MoS2. Sci. Rep. 2023, 13, 5970. [Google Scholar] [CrossRef]
  234. Aymukhanov, A.K.; Seisembekova, T.E.; Zeynidenov, A.K.; Ilyasov, B.R.; Alekseev, A.M.; Zhakhanova, A.M. Effect of molybdenum disulfide nanoparticles on the properties of the zinc oxide electron transport layer of an organic solar cell. Mater. Sci. 2023, 20, 20–26. [Google Scholar]
  235. Luo, Z.; Guo, T.; Wang, C.; Zou, J.; Wang, J.; Dong, W.; Li, J.; Zhang, W.; Zhang, X.; Zheng, W. Enhancing the Efficiency of Perovskite Solar Cells through Interface Engineering with MoS2 Quantum Dots. Nanomaterials 2022, 12, 3079. [Google Scholar] [CrossRef] [PubMed]
  236. Pang, B.; Chen, X.; Bao, F.; Liu, Y.; Feng, T.; Dong, H.; Yu, L.; Dong, L. Improved charge extraction and atmospheric stability of all-inorganic Cs2AgBiBr6 perovskite solar cells by MoS2 nanoflakes. Sol. Energy Mater. Sol. Cells. 2022, 246, 111932. [Google Scholar] [CrossRef]
  237. Sabari Girisun, T.C.; Durairaj, M.; Vijaya, S.; Anandan, S. 1T and 2H phase molybdenum disulfide as a counter electrode for Pt free dye-sensitized solar cells. Mater. Sci. Eng. B 2023, 287, 116123. [Google Scholar] [CrossRef]
  238. Niu, S.; Cai, J.; Wang, G. Two-dimensional MoS2 for hydrogen evolution reaction catalysis: The electronic structure regulation. Nano Res. 2020, 14, 1985–2002. [Google Scholar] [CrossRef]
  239. Yin, Z.; Liu, X.; Chen, S.; Ma, T.; Li, Y. Interface Engineering and Anion Engineering of Mo-Based Heterogeneous Electrocatalysts for Hydrogen Evolution Reaction. Energy Environ. Mater. 2021, 6, e12310. [Google Scholar] [CrossRef]
  240. Li, P.Z.; Chen, N.; Al-Hamry, A.; Sheremet, E.; Lu, R.; Yang, Y.; Kanoun, O.; Baumann, R.R.; Rodriguez, R.D.; Chen, J.J. Inkjet-printed MoS2-based 3D-structured electrocatalysts on Cu films for ultra-efficient hydrogen evolution reaction. Chem. Eng. J. 2023, 457, 141289. [Google Scholar] [CrossRef]
  241. Liao, J.; Xue, Z.; Sun, H.; Xue, F.; Zhao, Z.; Wang, X.; Dong, W.; Yang, D.; Nie, M. MoS2 supported on Er-MOF as efficient electrocatalysts for hydrogen evolution reaction. J. Alloys Compd. 2022, 898, 162991. [Google Scholar] [CrossRef]
  242. Swathy, B.S.; Anamika, A.; Asha, A.S. Edge terminated and interlayer expanded pristine MoS2 nanostructures with 1T on 2H phase, for enhanced hydrogen evolution reaction. Int. J. Hydrogen Energy 2022, 47, 9579–9592. [Google Scholar]
  243. Wang, S.; Li, J.; Hu, S.; Kang, H.; Zhao, S.; Xiao, R.; Sui, Y.; Chen, Z.; Peng, S.; Jin, Z.; et al. Morphology Regulation of MoS2 Nanosheet-Based Domain Boundaries for the Hydrogen Evolution Reaction. ACS Appl. Nano Mater. 2022, 5, 2273–2279. [Google Scholar] [CrossRef]
  244. Xiao, Y.; Yao, J.; Zhang, T.; Ma, X.; Xu, D.; Gao, H. Three-dimensional cross-linked Co-MoS2 catalyst on carbon cloth for efficient hydrogen evolution reaction. Dalton Trans. 2022, 51, 638–644. [Google Scholar] [CrossRef] [PubMed]
  245. Bui, H.T.; Linh, D.C.; Nguyen, L.D.; Chang, H.; Patil, S.A.; Shrestha, N.K.; Bui, K.X.; Bui, T.S.; Nguyen, T.N.A.; Tung, N.T.; et al. In-situ formation and integration of graphene into MoS2 interlayer spacing: Expansion of interlayer spacing for superior hydrogen evolution reaction in acidic and alkaline electrolyte. J. Mater. Sci. 2022, 57, 18993–19005. [Google Scholar] [CrossRef]
  246. Sundara Venkatesh, P.; Kannan, N.; Ganesh Babu, M.; Paulraj, G.; Jeganathan, K. Transition metal doped MoS2 nanosheets for electrocatalytic hydrogen evolution reaction. Int. J. Hydrogen Energy 2022, 47, 37256–37263. [Google Scholar] [CrossRef]
  247. Chen, X.; Sun, J.; Guan, J.; Ji, J.; Zhou, M.; Meng, L.; Chen, M.; Zhou, W.; Liu, Y.; Zhang, X. Enhanced hydrogen evolution reaction performance of MoS2 by dual metal atoms doping. Int. J. Hydrogen Energy 2022, 47, 23191–23200. [Google Scholar] [CrossRef]
  248. Gu, X.; Zhang, L.; Ma, X.; Wang, J.; Shang, X.; Wang, Z.; Kandawa-Schulz, M.; Song, W.; Wang, Y. A simple method for synthesizing Co, P-codoped MoS2 nanoflowers as electrocatalysts to enhance hydrogen evolution reaction. Ionics 2022, 28, 2337–2347. [Google Scholar] [CrossRef]
  249. Wei, H.; Tan, A.; Liu, W.; Piao, J.; Wan, K.; Liang, Z.; Xiang, Z.; Fu, Z. Interface Engineering-Induced 1T-MoS2/NiS Heterostructure for Efficient Hydrogen Evolution Reaction. Catalysts 2022, 12, 947. [Google Scholar] [CrossRef]
  250. German, E.; Gebauer, R. Why are MoS2 monolayers not a good catalyst for the oxygen evolution reaction? Appl. Surf. Sci. 2020, 528, 146591. [Google Scholar] [CrossRef]
  251. Bao, W.; Li, Y.; Zhang, J.; Ai, T.; Yang, C.; Feng, L. Interface engineering of the NiCo2O4@MoS2/TM heterostructure to realize the efficient alkaline oxygen evolution reaction. Int. J. Hydrogen Energy 2023, 48, 12176–12184. [Google Scholar] [CrossRef]
  252. Chen, S.; Cao, Z.; Gao, F.; An, H.; Wang, H.; Zhou, Z.; Mi, L.; Li, Y. 1T-MoS2/Co3S4/Ni3S2 nanoarrays with abundant interfaces and defects for overall water splitting. Colloids Surf. 2023, 661, 130930. [Google Scholar] [CrossRef]
  253. He, W.; Wang, L.; Zhang, H.; Gao, S.; Yu, W.; Yin, D.; Dong, X. SnO2@MoS2 heterostructures grown on nickel foam as highly efficient bifunctional electrocatalyst for overall water splitting in alkaline media. J. Alloys Compd. 2023, 938, 168678. [Google Scholar] [CrossRef]
  254. Tan, X.; Duan, Z.; Liu, H.; Wu, X.; Cho, Y. Core-shell structured MoS2/Ni9S8 electrocatalysts for high performance hydrogen and oxygen evolution reactions. Mater. Res. Bull. 2022, 146, 111626. [Google Scholar] [CrossRef]
  255. Rong, M.; Mo, Y.; Zhou, S.; Ma, X.; Wang, S.; Cao, Z.; Zhong, H. Ce and MoS2 dual-doped cobalt aluminum layered double hydroxides for enhanced oxygen evolution reaction. Int. J. Hydrogen Energy 2022, 47, 1644–1655. [Google Scholar] [CrossRef]
  256. Liu, G.; Ouyang, X.; Wei, X.-L.; Bao, W.-W.; Feng, X.-H.; Zhang, J.-J. Coupling Interface Construction of Ni(OH)2/MoS2 Composite Electrode for Efficient Alkaline Oxygen Evolution Reaction. Catalysts 2022, 12, 966. [Google Scholar] [CrossRef]
  257. Ran, N.; Song, E.; Wang, Y.; Zhou, Y.; Liu, J. Dynamic coordination transformation of active sites in single-atom MoS2 catalysts for boosted oxygen evolution catalysis. Energy Environ. Sci. 2022, 15, 2071–2083. [Google Scholar] [CrossRef]
  258. Zhao, C.; Zhang, X.; Xu, S.; Yang, G.; Fan, J.; Guo, J.; Cai, W.; Zhao, C. Construction of amorphous CoFeOx(OH)y/MoS2/CP electrode for superior OER performance. Int. J. Hydrogen Energy 2022, 47, 28859–28868. [Google Scholar] [CrossRef]
  259. Xue, Z.; Zhang, X.; Qin, J.; Liu, R. Constructing MoS2/g-C3N4 heterojunction with enhanced oxygen evolution reaction activity: A theoretical insight. Appl. Surf. Sci. 2020, 510, 145489. [Google Scholar] [CrossRef]
  260. Abd-Elrahim, A.; Chun, D. Nanosized Co3O4–MoS2 heterostructure electrodes for improving the oxygen evolution reaction in an alkaline medium. J. Alloys Compd. 2021, 853, 156946. [Google Scholar] [CrossRef]
  261. Mu, X.; Zhu, Y.; Gu, X.; Dai, S.; Mao, Q.; Bao, L.; Li, W.; Liu, S.; Bao, J.; Mu, S. Awakening the oxygen evolution activity of MoS2 by oxophilic-metal induced surface reorganization engineering. J. Energy Chem. 2021, 62, 546–551. [Google Scholar] [CrossRef]
  262. Samy, O.; El Moutaouaki, A. A Review on MoS2 Energy Applications: Recent Developments and Challenges. Energies 2021, 14, 4586. [Google Scholar] [CrossRef]
  263. Vedhanarayanan, B.; Shi, J.; Lin, J.Y.; Yun, S.; Lin, T.W. Enhanced activity and stability of MoS2 through enriching 1T-phase by covalent functionalization for energy conversion applications. Chem. Eng. J. 2021, 403, 126318. [Google Scholar] [CrossRef]
  264. Park, S.; Park, J.; Abroshan, H.; Zhang, L.; Kim, J.K.; Zhang, J.; Guo, J.; Siahrostami, S.; Zheng, X. Enhancing Catalytic Activity of MoS2 Basal Plane S-Vacancy by Co Cluster Addition. ACS Energy Lett. 2018, 3, 2685–2693. [Google Scholar] [CrossRef]
  265. Mohan, M.; Nagaraj, P.; Aminabhavi, T.M. Phase dependent performance of MoS2 for supercapacitor applications. J. Energy Storage 2023, 58, 106321. [Google Scholar] [CrossRef]
  266. Mouloua, D.; Kotbi, A.; Deokar, G.; Kaja, K.; El Marssi, M.; El Khakani, M.A.; Jouiad, M. Recent Progress in the Synthesis of MoS2 Thin Films for Sensing, Photovoltaic and Plasmonic Applications: A Review. Materials 2021, 14, 3283. [Google Scholar] [CrossRef] [PubMed]
  267. Agarwal, V.; Chatterjee, K. Recent advances in the field of transition metal chalcogenides for biomedical applications. Nanoscale 2018, 10, 16365–16397. [Google Scholar] [CrossRef]
Figure 1. The Ragone plot displays the relationship between energy and power density of various energy storage devices. Adapted from [20]. Copyright 2020, Energy Reports.
Figure 1. The Ragone plot displays the relationship between energy and power density of various energy storage devices. Adapted from [20]. Copyright 2020, Energy Reports.
Materials 16 04471 g001
Figure 2. Schematic representation of overview of this review article.
Figure 2. Schematic representation of overview of this review article.
Materials 16 04471 g002
Figure 3. (a) Top view of monolayer MoS2 with stick and ball crystal structure, (b) Side view of multilayer MoS2 with 2H structure, (c) Side view of multilayer MoS2 with 3R structure. The arrow marks indicate the number of layers in a repeat unit. Adapted from [45]. Copyright 2019 Nano Energy.
Figure 3. (a) Top view of monolayer MoS2 with stick and ball crystal structure, (b) Side view of multilayer MoS2 with 2H structure, (c) Side view of multilayer MoS2 with 3R structure. The arrow marks indicate the number of layers in a repeat unit. Adapted from [45]. Copyright 2019 Nano Energy.
Materials 16 04471 g003
Figure 4. Schematic representation of the (a) bottom-up approach and (b) top-down approach.
Figure 4. Schematic representation of the (a) bottom-up approach and (b) top-down approach.
Materials 16 04471 g004
Figure 5. Various applications of MoS2 in energy storage and energy conversion fields.
Figure 5. Various applications of MoS2 in energy storage and energy conversion fields.
Materials 16 04471 g005
Figure 6. (a) Schematic representation of the synthesis of C/MoS2 hybrid, (b) CV curves of C/MoS2 electrode at a scan rate of 1 mV s−1 within a potential window of 0.01–3.0 V, (c) GCD curves within a potential window of 0.01–3.0 V (vs. Li/Li+), (d) Cyclic performance of C/MoS2 electrode, and (e) Rate capability of C/MoS2 electrode. Adopted from [151]. Copyright 2023 Scientific Reports.
Figure 6. (a) Schematic representation of the synthesis of C/MoS2 hybrid, (b) CV curves of C/MoS2 electrode at a scan rate of 1 mV s−1 within a potential window of 0.01–3.0 V, (c) GCD curves within a potential window of 0.01–3.0 V (vs. Li/Li+), (d) Cyclic performance of C/MoS2 electrode, and (e) Rate capability of C/MoS2 electrode. Adopted from [151]. Copyright 2023 Scientific Reports.
Materials 16 04471 g006
Figure 7. Electrochemical performance of MoS2, MoS2/C, MoS2/CNT, and MoS2/C/CNT electrodes in sodium-ion batteries: (a) schematic representation of the performance of MoS2 and its composites in sodium-ion batteries, (b) GCD characteristics of MoS2 and its composites at 50 mA g−1, (c) cyclic test of MoS2 and its composites at 50 mA g−1 (the green arrow indicates that MoS2/C, MoS2/CNT composite electrode have high cyclic stability), (d) cyclic rate of MoS2 and its composites at various current densities, and (e) cycling performance MoS2/C/CNT//Na(Ni0.5Mn0.3Co0.2)O2 full-cell at 50 mA g−1. Adopted from [167]. Copyright 2021 Carbon Trends.
Figure 7. Electrochemical performance of MoS2, MoS2/C, MoS2/CNT, and MoS2/C/CNT electrodes in sodium-ion batteries: (a) schematic representation of the performance of MoS2 and its composites in sodium-ion batteries, (b) GCD characteristics of MoS2 and its composites at 50 mA g−1, (c) cyclic test of MoS2 and its composites at 50 mA g−1 (the green arrow indicates that MoS2/C, MoS2/CNT composite electrode have high cyclic stability), (d) cyclic rate of MoS2 and its composites at various current densities, and (e) cycling performance MoS2/C/CNT//Na(Ni0.5Mn0.3Co0.2)O2 full-cell at 50 mA g−1. Adopted from [167]. Copyright 2021 Carbon Trends.
Materials 16 04471 g007
Figure 8. (a) Schematic representation of the synthesis process of NiCo2S4/MoS2 composite (State I: shows the mixing of all precursors, State II: illustrates the formation of MoS2, State III: demonstrates the formation of NiCo2S4 over MoS2 with sheet- and rod-like morphologies), (b) Comparative CV curves of MoS2, NiCo2S4, and NCMS-L (NiCo2S4/MoS2 composite with sheet-like morphology) at a scan rate of 100 mV s−1, (c) Comparative GCD curves of MoS2, NiCo2S4, and NCMS-L at a current density of 1 mA g−1, (d) CV curves of the hybrid supercapacitor device of NCMS-L and activated carbon at various scan rates, (e) GCD curves of the hybrid supercapacitor device of NCMS-L and activated carbon at various current densities. Adopted from [187]. Copyright 2023 Nanomaterials.
Figure 8. (a) Schematic representation of the synthesis process of NiCo2S4/MoS2 composite (State I: shows the mixing of all precursors, State II: illustrates the formation of MoS2, State III: demonstrates the formation of NiCo2S4 over MoS2 with sheet- and rod-like morphologies), (b) Comparative CV curves of MoS2, NiCo2S4, and NCMS-L (NiCo2S4/MoS2 composite with sheet-like morphology) at a scan rate of 100 mV s−1, (c) Comparative GCD curves of MoS2, NiCo2S4, and NCMS-L at a current density of 1 mA g−1, (d) CV curves of the hybrid supercapacitor device of NCMS-L and activated carbon at various scan rates, (e) GCD curves of the hybrid supercapacitor device of NCMS-L and activated carbon at various current densities. Adopted from [187]. Copyright 2023 Nanomaterials.
Materials 16 04471 g008
Figure 9. (a) Schematic representation of fabrication of MSC using MoS2 nanosheets, (b) Response of CV curves at a scan rate of 100 mV s−1 under various bending angles of MSC, (c) Demonstrating the flexibility of MSC under various bending radius, (d) Demonstrating the cyclic stability of MSC at 10 μA cm−2 up to 8000 cycles, (e) Comparing the performance of fabricated flexible MSC with the other devices using Ragone plot. Adopted from [207]. Copyright 2020 ACS Applied Materials & Interfaces.
Figure 9. (a) Schematic representation of fabrication of MSC using MoS2 nanosheets, (b) Response of CV curves at a scan rate of 100 mV s−1 under various bending angles of MSC, (c) Demonstrating the flexibility of MSC under various bending radius, (d) Demonstrating the cyclic stability of MSC at 10 μA cm−2 up to 8000 cycles, (e) Comparing the performance of fabricated flexible MSC with the other devices using Ragone plot. Adopted from [207]. Copyright 2020 ACS Applied Materials & Interfaces.
Materials 16 04471 g009
Figure 10. (a) Schematic representation of the synthesis of MoS2 thin film over the glass/FTO substrate using the microwave-assisted method, (b) MoS2 thin film created on a glass/FTO substrate and a bare glass/FTO substrate can be shown in a camera image, (c) image of a synthesized thin MoS2 film captured using High-resolution FESEM, (d) Raman peaks for E1 2g and A1g vibrational modes of MoS2 are displayed in the Raman spectrum of a thin film of MoS2. Adopted from [231]. Copyright 2019 Journal of Materials Chemistry A.
Figure 10. (a) Schematic representation of the synthesis of MoS2 thin film over the glass/FTO substrate using the microwave-assisted method, (b) MoS2 thin film created on a glass/FTO substrate and a bare glass/FTO substrate can be shown in a camera image, (c) image of a synthesized thin MoS2 film captured using High-resolution FESEM, (d) Raman peaks for E1 2g and A1g vibrational modes of MoS2 are displayed in the Raman spectrum of a thin film of MoS2. Adopted from [231]. Copyright 2019 Journal of Materials Chemistry A.
Materials 16 04471 g010
Figure 11. (a) Schematic representation of synthesis process of 1T-MoS2/NiS composite, (be) Electrochemical characterization of NiS, 2H-MoS2, 1T-MoS2, Ni-MoS2, and 1T-MoS2/NiS catalyst at 1.0 M KOH, (b) Polarization curves (without iR correction) (c) Overpotential at a current density of 10 mA cm−2 and 100 mA cm−2, (d) Tafel plots, (e) Durability tests of the 1T-MoS2/NiS catalyst at a constant potential of −0.12 V and −0.21 V vs. RHE, (f) Projected density of states of 1T-MoS2 and 1T-MoS2/NiS catalysts with the Fermi level set to zero, (g) The electron transfer process from NiS to 1T-MoS2 is represented through the side view of the charge density distribution of 1T-MoS2/NiS with cyan and pink colors indicate an increase and decrease in electron density, respectively. Adopted from [249]. Copyright 2022 Catalysts.
Figure 11. (a) Schematic representation of synthesis process of 1T-MoS2/NiS composite, (be) Electrochemical characterization of NiS, 2H-MoS2, 1T-MoS2, Ni-MoS2, and 1T-MoS2/NiS catalyst at 1.0 M KOH, (b) Polarization curves (without iR correction) (c) Overpotential at a current density of 10 mA cm−2 and 100 mA cm−2, (d) Tafel plots, (e) Durability tests of the 1T-MoS2/NiS catalyst at a constant potential of −0.12 V and −0.21 V vs. RHE, (f) Projected density of states of 1T-MoS2 and 1T-MoS2/NiS catalysts with the Fermi level set to zero, (g) The electron transfer process from NiS to 1T-MoS2 is represented through the side view of the charge density distribution of 1T-MoS2/NiS with cyan and pink colors indicate an increase and decrease in electron density, respectively. Adopted from [249]. Copyright 2022 Catalysts.
Materials 16 04471 g011
Figure 12. (a) Schematic representation of synthesis process of Ni(OH)2/MoS2/NF composite electrode, (be) Electrochemical characterization of Ni(OH)2/MoS2/NF, MoS2/NF, Ni(OH)2/NF and bare NF electrodes, (b) The polarization curves with iR corrected, (c) The overpotentials at 50 mA cm−2 and 100 mA cm−2, (d) Electrochemical impedance spectroscopy, (e) Tafel plots, (f) The multi-potential steps of Ni(OH)2/MoS2/NF electrode, (g) The multi-current steps of Ni(OH)2/MoS2/NF electrode. Adopted from [256]. Copyright 2022 Catalysts.
Figure 12. (a) Schematic representation of synthesis process of Ni(OH)2/MoS2/NF composite electrode, (be) Electrochemical characterization of Ni(OH)2/MoS2/NF, MoS2/NF, Ni(OH)2/NF and bare NF electrodes, (b) The polarization curves with iR corrected, (c) The overpotentials at 50 mA cm−2 and 100 mA cm−2, (d) Electrochemical impedance spectroscopy, (e) Tafel plots, (f) The multi-potential steps of Ni(OH)2/MoS2/NF electrode, (g) The multi-current steps of Ni(OH)2/MoS2/NF electrode. Adopted from [256]. Copyright 2022 Catalysts.
Materials 16 04471 g012
Table 1. Comparison of various synthesis methods of MoS2.
Table 1. Comparison of various synthesis methods of MoS2.
Synthesis MethodMeritsDemerits
Mechanical exfoliationHigh-quality crystal structure;
Same crystal structure as their bulk;
Simple method;
No chemical reaction involved.
Less yield produced;
Substrate assistance is needed;
Thickness of the layer was not controllable.
Ball millingHigh yield/Massive production;
High surface area;
Reaction parameters are controllable.
The inert condition required;
Yield has a few-layered thickness.
Liquid phase exfoliationHigh yield/Massive production;
Scalable method;
Low-cost method.
Toxic organic solvents involved;
Yield has a few-layered thickness.
Chemical vapor depositionHigh-quality crystal with purity;
Size and thickness are scalable;
High surface area films;
High deposition rate.
Solid substrate assistance is needed with a vacuum;
High operating temperature;
Possibility of toxicity of precursors.
Physical vapor depositionAtomic-level control of chemical deposition;
Safer than CVD.
Low deposition rate;
Requirement of annealing time;
Line-of-sight deposition.
Wet chemical synthesisHigh yield with low cost;
Easy hybridization with other nanomaterials;
Controllable size and shape.
Large degree of agglomeration may occur,
Difficult to obtain nanoparticles with a single layer.
Table 2. MoS2 nanocomposites as electrode materials for FSC applications.
Table 2. MoS2 nanocomposites as electrode materials for FSC applications.
ElectrodesSynthesis MethodSpecific
Capacitance
Retention after Bending/
Twisting
Retention Rate
(Cycles)
Energy DensityPower DensityRef.
MoS2/GrHydrothermal method208 F g−1NA86.5% (10,000)65 Wh kg−10.33 kW kg−1[205]
MoS2/NGQDs/
HCNT@CC
Hydrothermal method1893
mF cm−2
NA86%
(2500)
673 μWh cm−25687
μW cm−2
[210]
CC-CNC@
MoS2
Hydrothermal method120.7
mF cm−2
NA88.2%
(10,000)
0.016
mWh cm−2
8.3 mW cm−2[211]
MoS2/NCCPlasma method3834.28
mF cm−2
NA83.3%
(10,000)
138.12
µWh cm−2
7417.33
µW cm−2
[212]
1T-MoS2/
Cu(OH)2@CFP
wet-mold
papermaking
technology
1124
mF cm−2
NA90.8%
(20,000)
0.130
mWh cm−2
0.375
mW cm−2
[213]
MoS2@SSMDC sputtering method214.90 F g−192%88%
(3000)
28.05 Wh kg−10.26 kW kg−1[214]
MoS2-AlN@SSbinder-free
sputtering method
372.35 F g−195%93%
(5000)
28.05 Wh kg−10.26 kW kg−1[215]
MoS2@CoS2calcination and sulfuration950 F g−1NA94.6%
(10,000)
33.94 Wh kg−11040 W kg−1[216]
MoS2-Cu3NMagnetron
Sputtering
215.47 F g−191%90%
(2000)
30 Wh kg−1138 W kg−1[217]
MoS2/PANI/CNTSonication method245 F cm−3NA80%
(2000)
0.013 Wh cm−31.0 W cm−3[218]
Note: NA—Information not available.
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Ismail, K.B.M.; Arun Kumar, M.; Mahalingam, S.; Kim, J.; Atchudan, R. Recent Advances in Molybdenum Disulfide and Its Nanocomposites for Energy Applications: Challenges and Development. Materials 2023, 16, 4471. https://doi.org/10.3390/ma16124471

AMA Style

Ismail KBM, Arun Kumar M, Mahalingam S, Kim J, Atchudan R. Recent Advances in Molybdenum Disulfide and Its Nanocomposites for Energy Applications: Challenges and Development. Materials. 2023; 16(12):4471. https://doi.org/10.3390/ma16124471

Chicago/Turabian Style

Ismail, Kamal Batcha Mohamed, Manoharan Arun Kumar, Shanmugam Mahalingam, Junghwan Kim, and Raji Atchudan. 2023. "Recent Advances in Molybdenum Disulfide and Its Nanocomposites for Energy Applications: Challenges and Development" Materials 16, no. 12: 4471. https://doi.org/10.3390/ma16124471

APA Style

Ismail, K. B. M., Arun Kumar, M., Mahalingam, S., Kim, J., & Atchudan, R. (2023). Recent Advances in Molybdenum Disulfide and Its Nanocomposites for Energy Applications: Challenges and Development. Materials, 16(12), 4471. https://doi.org/10.3390/ma16124471

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop