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Review

Achieving High Performance Electrode for Energy Storage with Advanced Prussian Blue-Drived Nanocomposites—A Review

1
Institute of Advanced Materials and Flexible Electronics (IAMFE), School of Chemistry and Materials Science, Nanjing University of Information Science and Technology, Nanjing 210044, China
2
Department of Materials Physics, School of Chemistry and Materials Science, Nanjing University of Information Science and Technology, Nanjing 210044, China
3
Australian Centre for Advanced Photovoltaics, School of Photovoltaic and Renewable Energy Engineering, University of New South Wales, Sydney 2052, Australia
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Materials 2023, 16(4), 1430; https://doi.org/10.3390/ma16041430
Submission received: 19 December 2022 / Revised: 2 February 2023 / Accepted: 6 February 2023 / Published: 8 February 2023
(This article belongs to the Special Issue Applications of High-Performance Electrolyte Materials in Batteries)

Abstract

:
Recently, Prussian blue analogues (PBAs)-based anode materials (oxides, sulfides, selenides, phosphides, borides, and carbides) have been extensively investigated in the field of energy conversion and storage. This is due to PBAs’ unique properties, including high theoretical specific capacity, environmental friendly, and low cost. We thoroughly discussed the formation of PBAs in conjunction with other materials. The performance of composite materials improves the electrochemical performance of its energy storage materials. Furthermore, new insights are provided for the manufacture of low-cost, high-capacity, and long-life battery materials in order to solve the difficulties in different electrode materials, combined with advanced manufacturing technology and principles. Finally, PBAs and their composites’ future challenges and opportunities are discussed.

1. Introduction

Environmental degradation and energy scarcity drive up demand for renewable energy. Energy storage and conversion is critical for renewable energy systems [1]. Governments all over the globe are becoming more conscious of the need of efficient green energy (solar energy, wind energy, and so on) and have made different efforts in green energy technology in accordance with global environmental standards. However, owing to material constraints, the performance of energy storage devices is far from meeting the needs due to the low performance of electrode materials [2]. In recent years, the family of Prussian blue (PB) and its analogue (PBA), a type of open frame structure materials, are widely used [3].
PB was discovered by chance by the Berlin artist Diesbach in 1704 and is thought to be the first synthetic metal–organic framework (MOF) reported in scientific literature. However, until the development of modern X-ray diffraction technology and its widespread application in structural determination, it lacked a clear crystal structure. PB is a mixed-valent ferrocyanide coordination polymer with a face-centered cubic structure composed of alternating Fe2+ and Fe3+ ions. Fe2+ and Fe3+ ions are surrounded by carbon and nitrogen atoms (Fe2+-C and Fe3+-N, respectively), leaving a large ion channel along the <100>direction. This unique structural arrangement in PB allows Fe to be replaced by other transition metal ions with different oxidation states, such as Cu2+, Mn2+, Ni2+, Zn2+, Co2+, and Co3+, resulting in PBA [4].
The unique structure of PB/PBA makes it a research hotspot [5]. Working as electrode materials in energy storage field, the family of PBA showed many advantages: (1) the unique open frame structure provides open channels allowing rapid anions and cations migration [6]; (2) the active site of the double redox reaction provides electrode with high specific charge/discharge capacity; (3) the manufacture of PBA is sample, inexpensive, and the form and type may be regulated manually. The excellent structure and performance of PBA make it widely used in various battery systems, such as Na-ion battery, Li-ion battery, K-ion battery, Ca-ion battery, Mg-ion battery, Al-ion battery, Zn-ion battery, etc. [7].
PBA’s unique structure provides several advantages in energy storage applications, yet it still has significant flaws. The main disadvantage of PBAs is their low crystal density. However, recent work found that composite materials combining PBA with other materials (such as oxides, sulfides, selenides, phosphates, borides, and carbides) can effectively neutralize the defects of the two materials [8]. When composite materials are used in energy storage, their cycle and electrochemical properties can improve significantly. As a result, it is possible to develop high-capacity, long-life, and cycle-stable energy storage materials [9]. As a result, electrode materials made by combining PBA with other materials have received considerable attention.
Unlike previous articles on the review of Prussian blue materials, we introduced the latest progress of PBAs-based electrode materials in this review, including oxides, sulfides, selenides, phosphates, borides, and carbides, under the guidance of advanced experimental methods and electrochemical characteristics (Table 1). We also discussed the formation of PBA in conjunction with other materials. The performance of composite materials improves the electrochemical performance of its energy storage materials [10]. Furthermore, new insights are provided for the manufacture of low-cost, high-capacity, and long-life battery materials in order to solve the difficulties in different electrode materials, combined with advanced manufacturing technology and principles [11]. Simultaneously, its development and use in supercapacitors and electrocatalysis are described (Figure 1). Finally, PBA and its composites’ future challenges and opportunities are discussed.

2. Prussian Blue and Its Analogues

2.1. Prussian Blue and Its Derivatives as Oxides

2.1.1. Mechanism of Oxide Derived from Prussian Blue as Energy Storage Material

Oxide derivatives with hollow nanostructures based on PB and PBA were investigated as anode materials for varous kind of rechargeable batteries system [12,13,30,31,32,33,34,35]. For example, PB cube can be derived as Fe2O3 [12]. These Fe2O3 microboxes have distinct physical architectures. The physical architectures of these Fe2O3 microboxes are unique. Their porous or hollow architectures may improve electrolyte diffusion and Li+ ions transport in the electrode, and this nano structure can effectively avoid volume change during the charging and discharging process [36]. At the same time, high crystallinity and hollow Fe2O3 microboxes provide structural stability during the long terms of charging and discharging process (Figure 2).
In addition to iron oxide, structure-related lithium storage properties can also be found in cobalt oxides derived from PBA. Co3O4 has been used in Li-ion battery because of its easy synthesis and high specific capacity. Because of the charge storage provided by the Faraday processes, cobalt oxide has attracted a lot of attention and has been studied for a long time as an energy storage material. Various forms of cobalt oxides are easy to synthesize and have very high theoretical capacitance. Co3O4 can be converted into CoOOH in an alkaline electrolyte, and then Co3O4 can be converted into CoO2 [37]. Although its theoretical capacitance is high, its practical capacitance is lower due to conductivity reduction and parasitic species formation during the long terms of charging and discharging process. Furthermore, it is noted that the expansion/contraction phenomenon limits the cycling life of cobalt oxide-based electrode. The main way to overcome these shortcomings is to design various high surface area morphologies.
Hu et al. successfully demonstrated Co3O4 derived from Co3[Co(CN)6]2 PBA and obtained the porous Co3O4 nanocages [15]. Yi et al. found that porous Co3O4 nanocages had a better electrochemical performance as the anode of lithium solid cage. This nanostructure also has a high capacity for lithium storage [4]. As an energy storage material, it also shows many advantages: (1) the porous shell facilitates Li+ diffusion; (2) the bimodal pore size distribution and larger surface area reduce electrolyte resistance by shortening Li+ diffusion length, increasing electrolyte/electrode area of contact, and increasing electrolyte contact area; (3) coating amorphous carbon can adapt to cyclic-induced strain; (4) surface atoms and structural strain are enriched by small nanoparticles. These characteristics enable PBA-derived porous Co3O4 nanocages to provide significant benefits in the application of Lithium-ion batteries (LIBs), which may be exploited to create high-performance LIBs (Figure 3). All of these discoveries demonstrate that PBA oxide derivatives perform greatly as energy storage materials, and that they may be used to enhance the performance of LIBs in the future.

2.1.2. Application of Oxide Derived from PBAs as Energy Storage Material

In order to pursue higher performance energy storage materials, researchers have carried out extensive exploration to further improve the new materials with a high capacity, stable cycle, and fast charging capacity. Because of their ease of availability, low cost, and high theoretical specific capacity, transition metal oxides are regarded as good energy storage materials [30]. The use of PBA-derived oxide nanomaterials will improve the optimization and design of the nanostructured electrode materials, improve ion diffusion ability and structural stability, and enable the production of high-performance energy storage materials. For instance, Zhang et al. [12] have explored the effect of Fe2O3 box secondary cells made of PB cubes at varying temperatures as anode materials for LIBs. Porous Fe2O3 micro particles composed of Fe2O3 nano particles can be easily synthesized by the oxidation and decomposition of PB nano cubes at high temperatures. When used as anode material of LIBs, the porous Fe2O3 nano cube obtained also shows the excellent cycle performance and high specific capacity (∼800 mA h g−1 at 200 mA g−1). In another experiment, researchers discovered that the electrochemical properties of Fe2O3 microboxes are also affected by the shell complexity [13]. The expandable synthesis of anisotropic hollow structures with numerous shell structures was demonstrated by the oxidative decomposition of PB microcube and crystal growth of iron oxide shell. The cycle stability of Fe2O3 microboxes with multiple shells is dramatically higher than that of Fe2O3 microboxes with single and double shells. When it is used as the anode material of LIBs, Fe2O3 has a well-defined hollow structure and microboxes with a layered shell, showing high specific capacity (∼950 mAh g−1 at 200 mA g−1) and outstanding cycle performance.
Meanwhile, the combination of metal oxides and carbon materials is a beneficial way to enhance the performance of LIBs. Using two PB/graphene foam precursors, Shao et al. [14] successfully prepared Fe2O3/graphene foam composites. The prepared Fe2O3/graphene foam material was used as a LIB’s independent electrode, combining the advantages of lead-derived metal oxides and graphene foam. It exhibited better lithium storage performance than pure Fe2O3 and graphene foam due to the synergistic effect of the two components. These research findings will help to develop and improve electrode materials for the storage of energy.
In addition, Hu et al. [15] suggested a new and simple method for creating porous Co3O4 nanocages based on the Kirkendall effect, which includes the thermal decomposition of PBA Co3[Co(CN)6]2 truncated nano cubes at 400 °C. These nanocages overcame the inherent disadvantage of Co3O4 anodes by exhibiting stability, high capacity, and excellent cycle efficiency. When applied to the electrode material of LIBs, the prepared Co3O4 porous nanocage showed excellent battery performance. At a current density of 300 mA g−1, it still had a capacity of 1465 mA h g−1 after 50 cycles. Metal oxides have a huge storage capacity; however, they suffer from significant volume fluctuations and have low conductivity when charged and discharged. Zhu et al. overcame this challenge by calcining preformed PBA Zn3[Co(CN)6]2 nanospheres to create self-assembled ZnO/Co3O4 nanocomposites [16]. These ZnO/Co3O4 nanocomposites have good cycling and lithium storing capacity. The rational design of the formed cluster structure, together with the synergistic impact of the bicomponent functional nanoparticle system, considerably improves the electrochemical performance of the electrode material generated from it. This special nanostructure has superior lithium storage capacity, which provides a new direction for further optimization of LIBs.

2.2. Prussian Blue and Its Derivatives as Sulfide

2.2.1. Mechanism of Sulfide as Energy Storage Material

Metal sulfides have been shown to have higher conductivity, mechanical stability, thermal stability, and electrochemical activity than equivalent metal oxides in recent years [38,39,40]. Metal sulfides offer higher conductivity than comparable metal oxides, as well as a rich valence state, mechanical and thermal stability, all of which are beneficial to electrochemical performance [41]. Mixed metal sulfide is gaining popularity as a viable electrode material for electrochemical energy storage and conversion systems [42]. When compared to a single metal sulfide, mixed metal sulfide performs significantly better electrochemically [11,43], owing to better electronic conductivity and more diverse redox processes. Metal sulfide has emerged as a potential electrode material due to its extensive redox chemistry, high conductivity, and the synergistic action of two metal ions. Because of their better performance and widespread use in recent years, lithium sulfur batteries are a potential new energy storage technology that can fulfill the rising energy demand. A typical LIB is made up of a negative electrode, a positive electrode, an electrolyte, and a separator sandwiched between parallel electrodes [44,45,46]. The working principle of both devices is voltage-driven cation migration (Na+, Li+, H+, K+, etc.) or anions (OH, etc.) through electrolyte towards electrodes for reversible electrochemical reactions. At the same time, electrons flow via the external circuit to keep the charge balanced. These lithium batteries require appropriate and effective materials, particularly as matrix, sandwich, and laminated metal organic skeleton as a novel porous material. The chemical characteristics and physical architectures of electrode materials must be appropriate for an efficient energy storage system [47,48]. Metal–organic framework composites and MOF derivatives have a better performance, reducing the shortcomings of pure MOFs [49,50].
Previous research found that interstitial water promoted the insertion and extraction of multivalent ions. PBAs have excellent electrochemical performance because water weakens the electrostatic repulsion between ions, lowering the activation energy of ion diffusion and interface transfer [51]. Lithium ion is relatively easy to embed in PBAs for ion diffusion, whereas sodium or potassium are more difficult to embed due to defects that inhibit sodium/potassium diffusion and coordination water. The vacancy and water content in PBA will be significantly reduced through a well controlled crystallization process, so that the cycle capacity and capacity of sulfur ion battery (SIB) and LIB can be improved [52]. PBA and its sulfide derivatives play an important role in the application of energy storage materials because they provide sufficient gaps for the transfer of ions and electrolytes, as well as many active sites for the insertion of ions.

2.2.2. Application of Sulfide as Energy Storage Material

PB and its sulfide derivatives are favored by many researchers because of their excellent performance, so PB and its sulfide derivatives have many applications in energy storage materials.
A graded iron sulfide nano cube was synthesized using PB as the starting material in a two-step in situ transformation process, and it was coated with several layers of graphene (Fe1−xS@C/rGO). When used as the anode of SIBs, the graded nano cube shows excellent rate capability of 323 mAh g−1 at a current density of 10 A g−1 [17]. For 150 cycles, the iron base sodium ion battery has a classification of Fe1−xS@C/rGO anode and the capacity of PB cathode is 323 mAh g−1. The Fe1−xS@C/rGO nano cube has good sodium ion storage performance due to the stable layered building structure and highly graphitized carbon obtained during the conversion process. The nano cube structure of graphene coating prevents the amalgamation of iron sulfide carbon core–shell nanoparticles and also adapts to the large volume expansion during the cycle. Carbon’s high crystallization degree conferred great electronic conductivity, enabled sodium ion accessibility, and enhanced mechanical durability on Fe1−xS@C/rGO nano cubes (Figure 4).
Zeng et al. created 3D hollow CoS2 nanoframes (HCSN) using partial anion replacement of Co-based PB nano cubes [53]. Because of its uniform broken hollow structure and excellent dispersion, the synthesized three-dimensional (3D) HCSN has a large specific surface area, leading to good electrochemical performance, such as the high specific capacitance of 568 F g−1 at 0.5 A g−1 and the excellent cycle stability of 88.3% specific capacitance retention after 5000 cycles. The HCSN supercapacitor has a great energy density of 32.3 Wh kg−1 and a power density of 4 kW kg−1. The HCSN also exhibit excellent structural stability and low density, indicating a potential application in energy storage materials.
The development of these new devices and their high performance show that PB sulfide derivatives play a significant role in the application of energy storage materials, as well as offering new ideas for the further development and utilization of sulfide in the future.

2.3. Prussian Blue and Its Derivatives as Selenide

2.3.1. Mechanism of Selenide as Energy Storage Material

Recently, many researchers have become interested in transition metal selenides, which have the advantages of a high conversion rate and capacity [54]. Compared with metal sulfides and metal oxides, transition metal selenides have weak metal selenium ion bonds, which is conducive to the rapid transport of Li+/Na+ [55,56]. Metal selenides have the potential of cycle stability and excellent charge discharge specific capacity due to the powerful electronic conductivity of Se (1 × 10−5 S m−1) and weak electronegativity. Among the discovered cathode materials for sodium ion batteries, metal selenides with huge theoretical capacity are regarded as a promising candidate. However, metal selenide anodes are still plagued by poor electron conductivity, low initial coulomb efficiency, and rapid volume change during charging and discharging. In addition, the “shuttle effect of polyselenides” (shuttle of polyselenides dissolved between positive and negative electrodes) will lead to capacity degradation during the cycle. As a result, numerous mitigation measures have been implemented in order to alleviate these issues. MOF has recently been used as a precursor for preparing hollow structures of metal oxides and sulfides due to its good morphology, high surface area, and uniform porous structure. Because of its special size and shape dependence, PB and its analogues are composed of metal ions coordinated with rigid organic cyano groups and have been evolved for the design and preparation of various porous nanostructures [33,57].

2.3.2. Application of Selenide as Energy Storage Material

PBA selenide derivatives can be used to build porous or hollow nanostructures with a high specific surface area and a unique shape that promotes electron transmission while avoiding significant volume expansion and thereby improving conductivity [58,59,60]. At the same time, by combining nanomaterials with different band gaps, it can promote the diffusion rate of Li+/Na+ and accelerate the surface reaction kinetics, which can form the design of bimetallic selenide architecture with unique interface effects. PBA selenide derivatives have a wide range of applications in energy storage materials. In addition, PBAs, as a MOF composed of metal centers and organic connectors, are available as self templates for the synthesis of porous materials [61]. MOF can limit and generate small size metal particles in situ, which can then be used to design metal selenides. Due to their excellent properties, many researchers are drawn to develop and use them.
Zhang et al. took full advantage of the porosity of PBA materials and the high capacity and high conversion of selenides, and used Zn-Fe PBA@polydopamine as a precursor to carbonization-selenization to design the microporous nanostructure ZnSe-Fe3Se4@NC successfully [18]. In addition, they investigated the electrochemical performance of N-doped Zn-Fe-Se heterostructures in LIBs. The ZnSeFe3Se4@NC anode exhibits excellent cycle stability and rate performance at 1 A g−1 after 723 cycles for LIBs (900 mA h g−1) because of the advantages of high conductivity carbon coating and porous structure (Figure 5). Previous research has shown that nanostructure fabrication and hybridization with carbonaceous materials are effective methods for mitigating mechanical strain caused by volume and structure changes during charge and discharge processes [62,63]. On the one hand, due to the short transmission path, reducing the electrochemical active materials to nano scale facilitates ions and electrons [64]. The carbonaceous reagent, on the other hand, can not only improve the transmittance of the electrode but also act as an effective buffer matrix to mitigate volume and structure changes during the cycle [65]. Wang et al. [19] successfully designed porous Mn-Fe-Se adhered/inserted with interlaced CNTs using a simple chemical precipitation approach and a one-step carbonization-selenization of the Mn-Fe PBA precursor process. Mn-Fe-Se/CNT exhibit remarkable electrochemical properties as well as high cycling and rate capabilities due to the synergistic effect of interlaced CNT (Figure 6). N-doped FeC@C box, which acts as the efficient polyselenide reservoir, is successfully created via a simple pyrolysis method using PB nano cubes as a precursor by Wang et al. [66]. Their results show that the PBA selenide derivative battery has high reversible specific capacity, better conduction rate, and cycle stability.
The above results indicate that PBA selenide is a promising electrode material for LIB. This result is expected to arouse people’s interest in energy storage and conversion of PBA selenide derivatives.

2.4. Prussian Blue and Its Derivatives as Phosphide

2.4.1. Mechanism of Phosphide as Energy Storage Material

Transition metal phosphides are one of the candidates for LIBs polar materials, because they have good polarity, high catalytic activity, thermal stability, and chemical stability [67,68,69]. Therefore, it is critical to investigate the use of TMPs in Li-S batteries. Huang et al., using the density functional theory, showed that FeP can form a strengthening bond with polysulfides, promoting further redox conversion [70]. Cheng et al. [71] created double-layer Ni-Fe-P/N-doped carbon nanomaterials and demonstrated their stable cycle and excellent rate performance in LIBs. Hard carbon and soft carbon are the most common anode materials, but their capacities are limited (generally less than 300 mAh g−1) [72]. FeP has recently been considered as a potential candidate due to its good theoretical capacity (926 mAh g−1), medium operational potential, and environmental friendliness [73]. Nevertheless, major problems related to the non-negligible volume change of FeP particles and low inherent conductivity must be solved, which will greatly reduce the relationship between dynamics and cycle stability [74]. To address the previously mentioned tradeoff between specific capacity and cycle stability, particle size reduction can effectively decrease diffusion length while increasing sodium diffusion coefficient [75,76]. FeP nanoparticles (12 nm) anchored and uniformly dispersed on nitrogen-doped carbon frames (FeP@NC). It has a greater reversible capacity of 253.9 mAh g−1 under 2 A g−1 [77]. Considering the uniform distribution of Fe in the PB framework, it is expected that the phosphating/carbonization of PB will lead to the uniformly distributed of FeP nanoparticles in the carbon matrix.

2.4.2. Application of Phosphide as Energy Storage Material

The excellent properties of PBA phosphide derivatives in energy storage materials make them favorable to many researchers, and many researchers have developed and applied them.
Song et al. [20] used Fe-Ni-P@nitrogen-doped carbon (Fe-Ni-P@NC) derived from Fe-Ni PBA, which is used as the efficient sulfur host of Li-S batteries. Fe-Ni-P particles not only effectively promote the conversion of LiPS, but also improve the adsorption of LiPS. Furthermore, the CN- of PBAs is easily converted into nitrogen-doped carbon during pyrolysis, which can improve the composite’s conductivity. Because of these benefits, LIBs/SIBs with S@Fe-Ni-P@NC composite cathodes demonstrated excellent electrochemical performance, excellent rate capability, and a stable cycle of 500 cycles at 1 ℃, and the capacity decay rate of each cycle is low, 0.08%.
By combining the tubular PB cathode with its derived phosphating anode, Jiang et al. demonstrated an excellent sodium ion battery [22]. Because of the tubular configuration, the PB has fast reaction kinetics and, thus, a high specific capacity of 94.4 mAh g−1 even at a high rate of 5.0 A g−1. PB-derived phosphides are characterized by encapsulating FeP nanoparticles in a conductive carbon matrix, thereby achieving excellent sodium energy storage. The as-assembled sodium-ion full cell has a record capacity of 105.3 mAh g−1 at 2.0 A g−1 and a long cycling lifetime (Figure 7). Their research proposes a homologous design strategy for outstanding sodium-ion full cells based on PB and its derivatives.
By making full use of the structural advantages of FeP, Shi et al. discovered a new binder-free anode material for high-performance sodium ion storage made of electrospun free-standing FeP@NPC film with FeP nanoparticles wrapped in 3D interconnected N, P-codoped carbon fiber [75]. The 3D-linked carbon fiber network acts as an electron/ion transport path, accelerating reaction kinetics while also adapting to the volume expansion of FeP during the sodium/disodium formation process. The unique structure design provides several structural advantages: the polyacrylonitrile nanofiber confines the growth of FeP nanoparticles during synthesis, reducing agglomeration of FeP; the structure has a high reversible capacity and cycle stability. This study lays the groundwork for a novel strategy for fabricating a phosphides-based high-performance anode for use in energy storage devices.
These studies and applications demonstrate that PBA phosphide derivatives perform exceptionally well in the application of energy storage materials. PBA phosphide derivatives will continue to be developed and applied in the future, with an eye toward their use in flexible electronic materials.

2.5. Prussian Blue and Its Derivatives as Boride

2.5.1. Mechanism of Boride as Energy Storage Material

Metal borides’ electrochemical properties have been extensively researched due to their high chemical stability, low cost, conductivity, and unique electronic interaction between boron atoms and metal atoms [78]. Metal boride nanostructures can open up an entirely new dimension for harnessing these properties. Nanostructures can provide advantages such as increased surface area, easier access to exposed catalytic centers, faster reaction rate kinetics, tunable electronic structures, and lower charge transfer resistance [79,80]. Recent research has revealed that transition metal borides have the potential to be effective electrocatalysts for water splitting [81,82,83]. Bimetallic and ternary borides have been shown to have higher electrocatalytic activity than single-metal borides due to a synergistic effect [84,85]. Schuhmann et al. used operando X-ray absorption spectroscopy on ultrathin nickel boride nanosheets to demonstrate this aspect [82]. These studies clearly illustrate that the surface oxidation states change from Ni2+ to Ni3+ during the oxygen evolution reaction (OER) process, resulting in the formation of a NiO(OH) surface layer on a NiB@NiO(OH) core–shell structure. Amorphous cobalt boride nanosheets are also effective at OER electrocatalytic water splitting [86]. NiCoB and NiFeB nanosheet heterostructures with r-GO and single phase borated metal boride layers exhibit good performance in OER electrocatalysis [87,88]. The presence of heteroatoms is thought to reduce charge transfer resistance, increase the density of active catalytic sites, and ease electronic state regulation. As a type of MOF family, PBAs have been used as precursors or templates for metal hydroxides, phosphides, and sulfides. PBAs can be converted into various nanostructured metal borides by mild chemical reduction based on their different structures and metal ions. Many researchers worked on developing this material, which has excellent performance in the field of energy storage.

2.5.2. Application of Boride as Energy Storage Material

PBA boride derivatives have been developed and utilized for their excellent properties in energy storage materials. He et al. synthesize amorphous Co-Ni-B-O nanosheets (CNBO-NSs) by chemically reducing bimetallic PBA (Co-Ni PBAs) with sodium borohydride [23]. The electrochemical catalytic activity and stability of the as-prepared CNBO-NSs are excellent. During 24 h operation, they can maintain a current density of 10 mA cm−2 at 140 mV over potential for hydrogen evolution and 300 mV for oxygen evolution. The formation of metal boron bonds, as well as an increase in surface area and conductivity in the CNBO-NS structure, are the factors that contribute to the increase in catalytic activity. This research can provide new insights for the application of MOF in the design of functional nanomaterials, as well as valuable insights for efficient electrolytic energy conversion and other aspects of crystallization engineering. As an efficient and durable electrocatalyst for OER, CoFe-based nanomaterials derived from PBA have increased specific surface area and rich catalytic active sites. Yang et al. [24] found that due to the adjustable chemical conformation and controllable 3D morphology, CoFe-B nano cube has a nano cube structure wrapped in ultra-thin nano sheets, and has excellent electrocatalytic performance and remarkable reaction kinetics in 1.0 m KOH aqueous solution. Furthermore, CoFe-B nano cubes have overpotentials of 261 and 338 mV at current densities of 10 and 200 mA cm−2, respectively, with a small Tafel slope of 61 mV dec1 for OER. The unique ultra-thin nano sheet wrapped nano cube structure is largely responsible for the excellent electrocatalysis performance. This work not only introduces a new method for using PBA, but it also introduces an efficient scheme for electrocatalysis.

2.6. Prussian Blue and Its Derivatives as Carbide

2.6.1. Mechanism of Carbide as Energy Storage Material

Metal carbides are ideal electrode materials for electrochemical storage devices (such as LIB and the supercapacitor) because of their excellent stability, good conductivity, and high theoretical capacity [89,90]. Metal carbides have greater electronic conductivity and mechanical stability, as well as corrosion resistance, due to their special atomic structure in which carbon atoms are found in the voids between densely packed metallic host atoms [90,91]. Gogotis et al. proved that two-dimensional layered carbides can be used as anode materials for LIBs, and found that the Li+ storage mechanism is the intercalation and de intercalation of Li+ layers. Furthermore, Gogotsi and his colleagues demonstrated the potential of layered carbides as electrode materials for supercapacitors [92]. When PBAs are combined with carbides, two-dimensional layered carbides act as a binder and conductive additive to connect the nanoparticles, facilitating charge transfer and avoiding the significant drop in electrode conductivity that would otherwise occur. PBAs can increase interlayer space, electrolyte diffusion, and battery electrochemical activity, making them perfect for all aspects of the energy storage sector. In addition, metal carbides and carbon-encapsulated metal/metal alloys exhibit outstanding electrocatalytic activity due to the synergistic impact between carbon materials and metals. PB/PBA nanoparticles with uniform element distribution and abundant cyanide ligands are also being investigated as chemical precursors for the preparation of catalytic metal carbides and carbon-encapsulated metal/metal alloys [93]. Because of the superior features of metal carbides, they offer significant benefits in the fields of energy storage and electrocatalysis, and they are frequently investigated and implemented in practice.

2.6.2. Application of Carbide as Energy Storage Material

It is an effective method to use PBA as the precursor and provide two metal elements at the same time to form bimetallic carbide and carbon skeleton nanocomposites with distinct structures. Ma et al. developed a method of implanting uniformly distributed carbide nanoparticles into a spherical porous carbon framework to form microspheres similar to pitaya [25]. The synthesized pitaya-shaped microspheres can effectively buffer volume changes and prevent Co3ZnC nanoparticles from aggregating during the charging/discharging process of LIBs due to their unique composition and structural characteristics. The porous carbon framework allows unimpeded electron transmission and Li diffusion, and restricts the thin solid electrolyte interface layer to the outer surface of the carbon shell. After 300 charge/discharge cycles, the anodes in LIBs deliver a high capacity of 608 mA h g−1 at 100 mA g−1 and ultrahigh cyclic stability and rate performance with a capacity of 423 mA h g−1 even after 1150 consecutive cycles at 1000 mA g−1 (Figure 8).
The thermal decomposition of PB produced Fe/Fe3C without altering its original morphology, but the surface area and porosity increased significantly [94]. Due to the presence of metallic iron, each of these Fe/Fe3C nanoparticles is uniformly coated with several layers of graphite carbon, which enhances its stability and electronic conductivity. Kumar et al. reported for the first time a one-step method for manufacturing the unique superstructure of carbon-encapsulated Fe/Fe3C nanocomposites for supercapacitor electrodes [26]. Nanocomposites with carbon encapsulation have excellent cycle stability and no capacitance decay after 20000 CV cycles. Asymmetric supercapacitors exhibit good electrochemical performance in terms of capacitance, energy, power density, and cycle stability when assembled, which is practical for future applications. The detailed investigation of PBA carbide derivatives provides us with a new idea in the research and development of energy storage materials.

3. Application

3.1. Application of PBAs in Batteries

PB/PBA and its derivatives are unique materials. They have recently regained much interest due to their unique characteristics, and some of them are ideal for energy storage. (1) They have theoretically high specific capacity [95]. (2) Their geometric form varies extremely little throughout the ion insertion process, leading in a cycle life that is astonishingly lengthy [96]. (3) Coprecipitation processes utilizing water precursors create these chemicals, resulting in easy and low-cost preparation procedures [97]. (4) Their cubic geometry, wide nanopore channels, and open framework structure enable ions to conduct rapidly and efficiently [98].
PBAs are suitable as ion hosts due to their ease of preparation, tunable composition/structure, and unique open framework, particularly for large cations such as Li+ and K+ [99]. In order to put PBA into large-scale, low-cost, high-performance practical applications, it is necessary to further improve the rate capability and cycle life, and significantly improve the ion conductivity and electronic conductivity of PBAs [100]. Not only does the increased size of multivalent cations have an adverse effect on cation diffusion, but so does the increased electrostatic repulsion. In this case, increasing the amount of vacancy and co-ordination water can reduce the electrostatic force and improve the transport and storage of cations. A macroporous morphology, on the other hand, can facilitate electrolyte access and accelerate cation diffusion. Combining or coating conductive carbons such as graphene, carbon nanotubes, and carbon black can significantly improve PBA’s limited electric conductivity, which hinders its electrochemical performance. Furthermore, those interested in designing multi-component metal oxides as catalysts for metal-air batteries can take advantage of PBAs’ simple preparation process and composition diversity. Considering all these, it is believed that the basic research on PBA materials will be helpful to develop high-performance battery electrode materials.
PBAs are useful templates for producing different metal oxides, metal sulfides, metal selenides, metal phosphides, metal borides, and metal carbides in nanostructure synthesis. The electrode materials derived from Prussian blue nanocomposites may fully use the benefits of all parties to create a new generation of high-performance ordering devices. The use of PBAs in multivalent batteries is a novel research topic that is still in its early stages. Future research will be required, such as the PBA storage mechanism and the construction of a novel PBA framework with a lengthy life cycle. PB/PBAs and their derivatives are being investigated as novel electrode materials. These researches provide new ideas and directions for the development of new battery materials in the future.

3.2. Application of PBAs in Capacitors

PB/PBAs and their derivatives have been considered as potential candidates for efficient supercapacitors. The intrinsic metal center in the original PB/PBA and its derivatives provides redox active sites for the Faraday reaction, increasing charge storage capacity. For the first time, Yi et al. successfully developed a new method of CoPBA@Ni(OH)2 core–shell structure. This method uses in situ etching and growth to cover the surface of a CoPBA nano cube with a Ni(OH)2 nano sheet before vulcanizing it into a CoS2@NiS2 hierarchical porous structure. Because of its excellent structure, this CoS2@NiS2 composite material has become a high-performance supercapacitor. PBA, as the central core of the cubic skeleton in this structure, can provide an effective electron conduction path to reduce resistance. In addition, it effectively prevents Ni(OH)2 and CoS2@NiS2 agglomeration, and its large surface area and mesoporous structure reduce ion diffusion paths, improving cycle stability. This material has a very high specific capacitance value of 1731.2 F g−1 at 1 A g−1 and cycle performance of 87.1% retention after 5000 cycles [27].
Although PB/PBA showed promising results, the poor conductivity of the original PB/PBA frame largely destroyed the capacitance. Many researchers have explored the use of conductive carbon substrates (such as graphene, activated carbon, or carbon fiber) to give PB/PBA frames higher conductivity, thereby improving conductivity and stability. For example, Wang et al. successfully fabricated high-quality graphene@PB (G@PB) nanocomposite sheets using a one-step in situ hydrothermal method in which uniform PB nanoparticles completely covered both sides of graphene sheets by controlling the etching of the raw material and the growth of the target products [28]. Graphene not only prevents the aggregation of PB nanoparticles, but also provides a conductive network for rapid electron transport. The G@PB-5 hybrid composite, in particular, shows the highest capacitance of 388.09 F g−1 at a current density of 1 A g−1, as well as enhanced rate capability and long-term stability with 97.2% retention over 5000 cycles and coulombic efficiency of nearly 100%. By combining the optimized nanocomposite electrode with the active carbon negative electrode, an asymmetric supercapacitor with a reversible working voltage of 2.0 V was constructed. The G@PB-5 nanocomposite sheets are promising for energy-storage hybrid electrodes due to their high electrochemical performances.
In addition to using the original PB/PBA as the supercapacitor electrode, researchers also studied the capacitive charge storage capacity of its derived nanostructures and the resulting energy storage density of asymmetric and hybrid supercapacitor devices. Yu and co-workers proposed a new structure-induced anisotropic chemical etching/anion exchange method for converting Ni-Co PBA nano cubes into tunable NiS nano frameworks [29]. The reaction of Ni Co PBA nano cube template with Na2S in solution leads to the formation of a well-defined NiS nano framework. The different reactivity of the edge and plane surfaces of the Ni Co PBA nano cube is discovered to be the key factor in the formation of the NiS nano frame. Due to the structural advantages of 3D open structure, namely a high specific surface area, the small size of primary nanoparticles, and good structural robustness, the derived NiS nano framework shows excellent electrochemical performance for supercapacitors.
Due to its superior properties, PB/PBA is widely employed in the field of energy storage devices. Although PB/PBA have good qualities, their conductivity is rather low, which poses a significant barrier to their implementation. PB/PBA derivatives have a larger surface area, conductivity, and more open diffusion channels than the original PB/PBA with porous and hollow morphology. These have a substantial impact on electrochemical performance. As a result, PB/PBA has been frequently employed as a precursor or sacrificial template in the production of derivatives. Adding conductive fillers, such as carbon materials and other metal compounds, improves the conductivity of PB and PBA materials. When compared to its original form, the addition of functional elements can improve its electrochemical performance, allowing high-performance supercapacitors to be created. We look forward to further research and development of PB/PBA in future supercapacitors.

4. Outlook

Because of their unique chemical and physical properties, PBAs are widely used as electrode materials for electrochemical energy storage and conversion. We found that when PBA is combined with various compounds to use electrodes as energy storage materials, its unique open frame structure allows ions to pass through quickly, solving the low conductivity problem of various compounds and greatly improving the conductivity of the energy storage system. On the other hand, PBA can endow materials with high capacity and alleviate the problems of effective material loss, volume expansion or capacity attenuation caused by material dissolution in electrolyte.
For the synthesis of PBAs, the key is to form a hollow structure, so that the formed PB/PBA template or the precursor and the final product can be evenly distributed with thermodynamic stability. Second, researchers still do not know much about the nucleation and crystallization processes of PBAs materials due to differences in nucleation rates and solubility precipitation constants. As a result, precisely controlling the microstructure, particularly the ion content, coordination water content, and lattice defects, is difficult. Further in situ studies should be carried out to fully understand its structure, grasp the synthesis mechanism, and accurately control the synthesis results in order to better understand its growth kinetics and control its synthesis.
At the same time, the hollow structure of PBA is an excellent catalytic structure because it can provide a larger catalytic interface area, which improves electrocatalytic performance significantly. To reduce the activation energy and improve the conversion rate in the important hydrogen evolution reaction, oxygen evolution reaction, and oxygen evolution reduction reaction, an electro catalyst with high efficiency, durability, low cost, and sustainability is usually required. Metal phosphides, sulfides, and borides derived from PBA can be used for electrocatalytic hydrogen evolution in acidic and alkaline solutions, according to the findings. There is currently little research on the use of PBA as a catalyst, and researchers can further investigate its use as a catalyst.
In the future, introducing new elements into PBA-derivative materials and studying their modified functions will be the brand-new research direction of PBA-based electrode materials in the field of energy storage. In terms of increased electrochemical surface area, the morphology development of PBA-derived materials holds great promise. PBA-derived materials can also be formed into a variety of two-dimensional and three-dimensional hollow, porous, and core–shell forms, making full use of their open framework to build channels conducive to ion transport, which is also a future way to improve the electrochemical performance of PBA materials in various ion battery electrodes.
We believe that the unique structure of PBA makes it widely used in the future electronic device applications. To fully investigate the properties of PBA, it will be a future research hotspot to develop high-performance materials or make composites with PBA as the precursor.

5. Conclusions

We introduced in depth the structure and properties of PB/PBA, as well as spectacular examples of their interaction with other types of chemicals, in this work. Based on this assumption, we investigated anode materials (oxides, sulfides, selenides, phosphides, borides, and carbides) based on Prussian blue analogues (PBAs), which have gained widespread recognition in the field of energy conversion and storage due to their distinct properties (including high theoretical specific capacity, environmental protection, and low cost). We discovered that PBA’s distinctive open frame structure may give open channels for ions, which is favorable to fast ion conduction, and the active sites of the redox reaction provide high-capacity materials via the research of numerous PBA electrode materials. PBA is a widely used electrode material with considerable promise for future improvement. Composite materials synthesized with PBA as a precursor fully integrate the great properties of diverse materials, which is the direction of constructing high-performance energy storage materials. These PBA composites outperform in every way. Their distinctive open frame construction and superior performance provide significant benefits in the production of high-performance batteries, novel supercapacitors, and electrocatalysts. These novel composite materials, which use PBA as a precursor, offer a wide range of possibilities in future flexible electronic devices.

Funding

The work was supported by the National Natural Science Foundation of China (22005150) and Natural Science Foundation of Jiangsu (BK20200825). And financially supported by The Startup Foundation for Introducing Talent of NUIST.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Acknowledgments

The work was supported by the National Natural Science Foundation of China (22005150) and Natural Science Foundation of Jiangsu (BK20200825). W.B. also acknowledges the financial support of The Startup Foundation for Introducing Talent of NUIST.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Schematic Diagram of PBA Application in Energy Storage Materials.
Figure 1. Schematic Diagram of PBA Application in Energy Storage Materials.
Materials 16 01430 g001
Figure 2. (a) Schematic illustration of the formation of hollow Fe2O3 microboxes and the evolution of the shell structure with the increasing calcination temperature. (I At temperatures below 350 °C, PB is converted to iron oxide in the near-surface region. II When the annealing temperature rises to 550 °C, the Fe2O3 microcapsules change into highly porous microcapsules. III When the annealing temperature rises to 650 °C, the highly porous shell is transformed into a layered shell composed of Fe2O3 nanoflakes.) (b) Discharge-charge voltage profiles of porous Fe2O3 microboxes obtained at 550 °C. (c) Cycling performance of Fe2O3 microboxes (350 °C), porous Fe2O3 microboxes (550 °C), and hierarchical Fe2O3 microboxes (650 °C), and Coulombic efficiency of porous Fe2O3 microboxes (550 °C) over the voltage range 0.01–3.0 V and Li/Li+ at the same current density of 200 mA g−1. Ref. [12] Copyright Journal of the American Chemical Society, ACS Publications.
Figure 2. (a) Schematic illustration of the formation of hollow Fe2O3 microboxes and the evolution of the shell structure with the increasing calcination temperature. (I At temperatures below 350 °C, PB is converted to iron oxide in the near-surface region. II When the annealing temperature rises to 550 °C, the Fe2O3 microcapsules change into highly porous microcapsules. III When the annealing temperature rises to 650 °C, the highly porous shell is transformed into a layered shell composed of Fe2O3 nanoflakes.) (b) Discharge-charge voltage profiles of porous Fe2O3 microboxes obtained at 550 °C. (c) Cycling performance of Fe2O3 microboxes (350 °C), porous Fe2O3 microboxes (550 °C), and hierarchical Fe2O3 microboxes (650 °C), and Coulombic efficiency of porous Fe2O3 microboxes (550 °C) over the voltage range 0.01–3.0 V and Li/Li+ at the same current density of 200 mA g−1. Ref. [12] Copyright Journal of the American Chemical Society, ACS Publications.
Materials 16 01430 g002
Figure 3. (a) Co3O4 porous nanocages have been prepared from Co3[Co(CN)6]2·nH2O truncated nano cubes based on the Kirkendall effect. (b) The first three CV curves of the Co3O4 porous nanocages based anode material recorded at a scan rate of 0.5 mV s−1. (c) The 1st, 2nd, 10th, and 20th discharge curves of the Co3O4 porous nanocage based anode materials at a current density of 300 mA g−1. (d) Rate capability of the as-prepared Co3O4 porous nanocages. Ref. [15] Copyright A European Journal, Wiley Online Library.
Figure 3. (a) Co3O4 porous nanocages have been prepared from Co3[Co(CN)6]2·nH2O truncated nano cubes based on the Kirkendall effect. (b) The first three CV curves of the Co3O4 porous nanocages based anode material recorded at a scan rate of 0.5 mV s−1. (c) The 1st, 2nd, 10th, and 20th discharge curves of the Co3O4 porous nanocage based anode materials at a current density of 300 mA g−1. (d) Rate capability of the as-prepared Co3O4 porous nanocages. Ref. [15] Copyright A European Journal, Wiley Online Library.
Materials 16 01430 g003
Figure 4. (a) Illustration of the formation process of Fe1−xS@C/rGO. (b) Galvanostatic discharge/charge curves of sodium ion full cells at different cycles at a current density of 200 mA g−1. (c) Cycle performance of sodium ion full cells at a current density of 200 mA g−1 (capacities are calculated based on anode mass). Ref. [17] Copyright Electrochimica Acta, Elsevier.
Figure 4. (a) Illustration of the formation process of Fe1−xS@C/rGO. (b) Galvanostatic discharge/charge curves of sodium ion full cells at different cycles at a current density of 200 mA g−1. (c) Cycle performance of sodium ion full cells at a current density of 200 mA g−1 (capacities are calculated based on anode mass). Ref. [17] Copyright Electrochimica Acta, Elsevier.
Materials 16 01430 g004
Figure 5. (a) Schematic diagram of synthesis process of the ZnSe-Fe3Se4@NC. (b) XRD pattern of ZnSe-Fe3Se4@NC. (c) Discharge and charge profiles of ZnSe-Fe3Se4@NC anode. (d) Long cycling performance of ZnSe-Fe3Se4@NC and NC anodes at 1 A g−1. Ref. [18] Copyright Journal of Alloys and Compounds, Elsevier.
Figure 5. (a) Schematic diagram of synthesis process of the ZnSe-Fe3Se4@NC. (b) XRD pattern of ZnSe-Fe3Se4@NC. (c) Discharge and charge profiles of ZnSe-Fe3Se4@NC anode. (d) Long cycling performance of ZnSe-Fe3Se4@NC and NC anodes at 1 A g−1. Ref. [18] Copyright Journal of Alloys and Compounds, Elsevier.
Materials 16 01430 g005
Figure 6. (a) Schematic representation of Mn-Fe-Se/CNTs composite. (b) XRD analysis of Mn-Fe-Se and Mn-Fe-Se/CNTs composites. (c) CV profiles at different scan rates. (d) Contribution ratio of capacitive current and diffusion-controlled current versus scan rate of Mn-Fe-Se/CNTs electrode for PIBs. Ref. [19] Copyright Chemical Engineering Journal, Elsevier.
Figure 6. (a) Schematic representation of Mn-Fe-Se/CNTs composite. (b) XRD analysis of Mn-Fe-Se and Mn-Fe-Se/CNTs composites. (c) CV profiles at different scan rates. (d) Contribution ratio of capacitive current and diffusion-controlled current versus scan rate of Mn-Fe-Se/CNTs electrode for PIBs. Ref. [19] Copyright Chemical Engineering Journal, Elsevier.
Materials 16 01430 g006
Figure 7. (a) Schematic diagram of the preparation of S@Fe-Ni-P@NC composites. (b) CV profiles of Fe-Ni-P@NC and Fe-Ni@NC in symmetric cell. (c) Galvanostatic charge–discharge curves.[20] (d) Schematic diagram for the synthesis of T-PB and T-FeP. (e) Rate capability at different current densities from 0.1 to 5.0 A g−1. Ref. [22] Copyright Journal of Power Sources, Elsevier.
Figure 7. (a) Schematic diagram of the preparation of S@Fe-Ni-P@NC composites. (b) CV profiles of Fe-Ni-P@NC and Fe-Ni@NC in symmetric cell. (c) Galvanostatic charge–discharge curves.[20] (d) Schematic diagram for the synthesis of T-PB and T-FeP. (e) Rate capability at different current densities from 0.1 to 5.0 A g−1. Ref. [22] Copyright Journal of Power Sources, Elsevier.
Materials 16 01430 g007
Figure 8. (a) Schematic illustration of the formation process of pitaya-like microspheres. (b) Charge/discharge profiles of pitaya-like microspheres as anode material of LIBs at 100 mA g−1. (c) Rate performance of pitaya-like microspheres at various current densities range from 100 to 1000 mA g−1. Ref. [25] Copyright Journal of Materials Chemistry A, pubs.rsc.org.
Figure 8. (a) Schematic illustration of the formation process of pitaya-like microspheres. (b) Charge/discharge profiles of pitaya-like microspheres as anode material of LIBs at 100 mA g−1. (c) Rate performance of pitaya-like microspheres at various current densities range from 100 to 1000 mA g−1. Ref. [25] Copyright Journal of Materials Chemistry A, pubs.rsc.org.
Materials 16 01430 g008
Table 1. The electrochemical performance of PB and its derivatives for energy storage.
Table 1. The electrochemical performance of PB and its derivatives for energy storage.
PrecursorsStructuresSpecific CapacityApplicationsRef.
PBFe2O3~800 mA h g−1 at 200 mA g−1LIBs[12]
PBMulti shell Fe2O3~950 mA h g−1 at 200 mA g−1LIBs[13]
PB/grapheneFe2O3/graphene~654 mA h g−1 at 100 mA g−1LIBs[14]
Co3[Co(CN)6]2 PBACo3O4 nanocages~1465 mA h g−1 at 300 mA g−1LIBs[15]
Zn3[Co(CN)6]2 PBAZnO/Co3O4 nanocomposite cluster~957 mA h g−1 at 100 mA g−1LIBs[16]
PBFe1−xS@C/rGO~323 mA h g−1 at 10 A g−1SIBs[17]
PBHollow CoS2 nanoframes568 F g−1 at 0.5 A g−1capacitor[17]
Zn-Fe PBA@polydopamineZnSe-Fe3Se4@NC~900 mA h g−1 at 1 A g−1LIBs[18]
Mn-Fe PBAMn-Fe-Se/CNT~411 mA h g−1 at 800 mA g−1PIBs/SIBs[19]
Fe-Ni PBAS@Fe-Ni-P@NC~470.8 mA h g−1 at 1 CLIBs/SIBs[20]
Fe4[Fe(CN)6]3Fe/Fe3C@N-rGO Electroctalysts[21]
PBFeP nanoparticles~105.3 mAh g−1 at 2.0 A g−1LIBs[22]
Co-Ni PBACNBO-NSs Electroctalysts[23]
PBACoFe-B nano cubes Electroctalysts[24]
PBApitaya-like microspheres~608 mA h g−1 at 100 mA g−1LIBs[25]
PBFe/Fe3C nanocomposites223 F g−1 at 10 mV s−1capacitor[26]
CoPBACoPBA@Ni(OH)287.1%/5000 cyclescapacitor[27]
PBG@PB-597.2%/5000 cyclescapacitor[28]
Ni-Co PBANiS nanoframes capacitor[29]
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Cui, D.; Wang, R.; Qian, C.; Shen, H.; Xia, J.; Sun, K.; Liu, H.; Guo, C.; Li, J.; Yu, F.; et al. Achieving High Performance Electrode for Energy Storage with Advanced Prussian Blue-Drived Nanocomposites—A Review. Materials 2023, 16, 1430. https://doi.org/10.3390/ma16041430

AMA Style

Cui D, Wang R, Qian C, Shen H, Xia J, Sun K, Liu H, Guo C, Li J, Yu F, et al. Achieving High Performance Electrode for Energy Storage with Advanced Prussian Blue-Drived Nanocomposites—A Review. Materials. 2023; 16(4):1430. https://doi.org/10.3390/ma16041430

Chicago/Turabian Style

Cui, Dingyu, Ronghao Wang, Chengfei Qian, Hao Shen, Jingjie Xia, Kaiwen Sun, He Liu, Cong Guo, Jingfa Li, Feng Yu, and et al. 2023. "Achieving High Performance Electrode for Energy Storage with Advanced Prussian Blue-Drived Nanocomposites—A Review" Materials 16, no. 4: 1430. https://doi.org/10.3390/ma16041430

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