Chevral phase

The cathodes currently used in Li-ion rechargeable battery are mostly operated based on the intercalation/de-intercalation chemistry. The same concept has also been attempted to explore cathode materials for Mg batteries. However, despite numerous materials having been investigated, only one group of materials named as CP showed excellent cyclability and relative high rate capability. The general formula of CP is M _x Mo₆T₈, where M = metal, e.g., Li, Mg, Cu, Zn, etc., and T = S, Se, and Te. In their seminal paper, Aurbach et al. reported CP-Mo₆S₈ as reversible cathode material in Mg battery with the cell configuration of Mg/Grignard electrolyte/CP. ^{Reference Aurbach, Lu, Schechter, Gofer, Gizbar, Turgeman, Cohen, Moskovich and Levi6} Figure 1(a) shows a typical coin cell cycling curve using CP Mo₆S₈ as cathode material. The initial discharge capacity reached ∼80 mAh/g at a 0.3 mA/cm² using the electrolyte of 0.25 M Mg(AlCl₂BuEt)₂ in tetrahydrofuran (THF). Two voltage plateaus were observed at 1.3 and 1.1 V during discharge process. The most remarkable performance of this cell was its excellent cyclability. In their report, the cathode sustained more than 2000 charge–discharge cycles at 100% depth of discharge at practical rates (0.1–1 mA/cm²) in a wide temperature range (−20 to 80 °C), with capacity fading of less than 15%. Typical cycling performance was shown in Fig. 1(b).

Figure 1.

(a) Electrochemical behavior and the basic structure of the CP cathode. (b) Cycling performance of CP at a constant current of 0.3 mA/cm². The inset shows the voltage profile at certain cycle. Reprinted with permission from Ref. Reference Aurbach, Lu, Schechter, Gofer, Gizbar, Turgeman, Cohen, Moskovich and Levi6. Copyright 2000 Nature Publishing Group.

The mechanism of the intercalation/de-intercalation of Mg²⁺ ions in CPs has been intensively studied. ^{Reference Levi, Lancry, Mitelman, Aurbach, Ceder, Morgan and Isnard17–Reference Levi, Levi, Chasid and Aurbach21} The crystal structure of CPs consists of octahedral clusters of Mo (Mo₆) inside cubic anion frameworks as stacks of Mo₆T₈ blocks within a three-dimensional open structure as shown in the insertion of Fig. 1(a). Mo₆ cluster exhibits variable valence during the insertion and removal of Mg²⁺ ions, while the anionic framework is flexible with multidirectional paths for ionic diffusion. CP-Mo₆T₈ can theoretically sustain up to four electrons exchanging, which corresponds to the insertion of two bivalent Mg²⁺ ions. This unusual structure provides a large number of close vacant sites and the metallic Mo₆ clusters. Especially the Mo₆ clusters is speculated as a critical factor to ensure high Mg²⁺ diffusivity in solid state host because they can easily compensate the charge-unbalance due to the introduction of bivalent Mg²⁺ ions. ^{Reference Levi, Gofer and Aurbach20}

The synthesis of CPs typically starts with the preparation of Cu₂Mo₆S₈ followed by leaching out Cu²⁺ ions. Cu₂Mo₆S₈, chemically leached in I₂/acetonitrile or in HCl/H₂O, was able to accommodate the theoretical amount of Mg²⁺ ions upon the first discharge of the electrode (2 Mg atoms per formula unit). ^{Reference Lancry, Levi, Gofer, Levi, Salitra and Aurbach22} A specific capacity of 90–100 mAh/g was achieved with excellent stability upon long-term cycling. Kim et al. reported an effective method to control the composition of CP-Cu _x Mo₆S₈ by adopting a chemical intercalation process. ^{Reference Woo, Yoo, Cho, Park, Kim, Kim, Kim and Kim23} A high reversible capacity close to the theoretical value was achieved at the Cu_1.3Mo₆S₈ electrode with good discharge rate capability (1 C with 90% capacity retention) and cycling performance (0.05 C over 50 cycles) at room temperature. Recently, this group further investigated the reaction mechanism of Cu doped CP. ^{Reference Choi, Kim, Woo, Cho, Choi, Choi, Lee, Park and Kim24} They found that Cu metal-like shell formed during Mg²⁺ ions intercalation and this Cu shell disappeared as Mg deintercalation. This finding helped elucidate the origin of the additional capacity of the Mo₆S₈ cathode arising from Cu addition and improve the electrochemical performance of the Mo₆S₈ cathode for rechargeable Mg batteries.

Substituting Se for S in CP improved the capacity of the first discharge plateau, while negligibly affecting the second discharge plateau. ^{Reference Levi, Lancry, Mitelman, Aurbach, Isnard and Djurado18} The initial capacity of Mo₆S₆Se₂ reached 110 mAh/g. Impressively, the rate behavior was improved for Se substituted CP. At 1 C rate, the capacity of Mo₆S₆Se₂ decreased only by 10%, compared to the optimal value at 0.1 C rate. For comparison, the 1 C capacity of nonsubstituted Mo₆S₈ dropped to only half of the capacity at 0.1 C. The presence of Se in the anionic framework increased its polarizability and thus improved solid state diffusion of Mg²⁺ ions. Besides, the presence of Se changed the local geometry of Mg insertion sites and enhances Mg migration.

Typically, CPs are synthesized by high temperature solid state reactions of elemental blend of copper, molybdenum, and sulfur powders at ∼1423 K for 7 days or by a molten salt route using Mo–MoS₂–CuS reactants in a KCl salt, and heat treating the reaction mixtures at ∼1123 K for 60 h in Ar atmosphere. ^{Reference Aurbach, Lu, Schechter, Gofer, Gizbar, Turgeman, Cohen, Moskovich and Levi6} The as-prepared materials were leached with acid to remove Cu. Both methods are very time consuming and most importantly the as-synthesized particle is still within micro size range, which limits the rate performance. Ryu et al. investigated the relationship between Mo₆S₈ particle size and the ratio of KCl salt with precursors. ^{Reference Ryu, Park, Cho, Kim and Kim25} Increasing the ratio of KCl melting salt from 1:1 to 4:1 decreased the particle size of CP from 0.75 to 0.24 μm. Consequently, the initial discharge capacity changed from 73 to 85 mAh/g. Saha et al. also tried to control the particle size through a co-precipitation method followed by a conventional calcination process. ^{Reference Saha, Jampani, Datta, Okoli, Manivannan and Kumta26} The particle size of the target material decreased to ∼500 nm and a capacity over 60 mAh/g was observed at a rate up to 1.5 C. Cheng et al. used a facile process to precipitate the precursors on graphene to increase the conductivity of the final material and control its particle size. ^{Reference Cheng, Parent, Shao, Wang, Sprenkle, Li and Liu27} Using this method, Mo₆S₈ showed better rate performance (2 C at a capacity of 70 mAh/g) and cycling behavior (retain the capacity over 70 mAh/g over 150 cycles).

Despite the fascinating cyclability and high Mg mobility, the voltage of CPs is only ∼1.0 to ∼1.2 V against Mg/Mg²⁺. The utilization of a heavy transition metal cluster (Mo₆) also limits its capacity to less than 150 mAh/g. These facts suggest that CPs can only be considered as moderate or low energy density cathodes. In their original paper, Mg battery based on CP cathode was only suggested to be an alternative to Ni–Cd battery. ^{Reference Aurbach, Lu, Schechter, Gofer, Gizbar, Turgeman, Cohen, Moskovich and Levi6} Other cathode candidates with higher voltage and/or capacity must be pursued if Mg battery is competing with Li-ion technology. However, Mo₆S₈ is still considered as the best-known model cathode for magnesium battery and will continue to serve as the baseline system to evaluate the suitability of new magnesium electrodes and electrolytes.

Other cluster-type cathodes

A crucial factor that leads to the nice performance of CPs is the unique Mo₆ cluster contained in the structure. Levi et al. argued that the existence of a cluster-like redox center enables the fast electron re-distribution during the migration of guest Mg²⁺ ions. ^{Reference Levi, Gofer and Aurbach20} The local electron neutralization requests the distribution of two electrons simultaneously with the migration of Mg²⁺, which in classical intercalation-type cathode is kinetically sluggish. For CPs, however, the electron re-distribution only changes the formal charge of individual Mo ions by 1/3e. This greatly lowers the barrier for the electron re-distribution and consequently improves Mg²⁺ migration. Accordingly, they proposed that other materials that contain redox active clusters may also serve as Mg cathode candidates.

We recently reported another cluster-type cathode material that entirely consists of nonmetal ions, the fullerene (C₆₀). ^{Reference Zhang, Mizuno and Ling28} The C₆₀ cathode material contains a group of carbon atoms bonding together by interatomic forces to form clusters. The electrochemical performance of C₆₀ cathode was shown in Fig. 2(a). ^{Reference Zhang, Mizuno and Ling28} Two voltage plateaus at 1.4 and 1.1 V were observed. The initial capacity reached ∼50 mAh/g at the cut off voltage of 0.8 V. The most impressive performance of C₆₀ cathode was the remarkable rate capability compared to other Mg battery cathodes. Figure 2(b) shows the rate performance of C₆₀ cathode. Even at the current density of ∼1.5 mA/cm², the C₆₀ cathode still retained 44% of its capacity operated at 0.019 µA/cm². The excellent electrochemical performance of C₆₀ was related to its cluster structure which effectively delocalizes extra electrons to the whole cluster rather than on one or two atoms.

Figure 2.

(a) Voltage profiles of C₆₀ cathode at the current density of 19 μA/cm². The inset shows the cyclic voltammetry curve. (b). Discharge curves of C₆₀ cathode at different current densities. Reprinted with permission from Ref. Reference Zhang, Mizuno and Ling28. Copyright 2015 Royal Society of Chemistry.

Taniguchi et al. reported another cluster based material, Mo₉Se₁₁ as cathode material for Mg battery. ^{Reference Taniguchi, Yoshino, Gu, Katsura and Takagi29} Similar to CP, its structure contains Mo₉ clusters. The electrochemical test was carried out using Mo₉Se₁₁ cathodes and magnesium metal anodes in 0.25 M Mg(AlCl₂EtBu)₂/THF electrolyte solution. The derivative of the capacity with respect to the potential showed two distinct peaks for the cathodic process at 1.0 and 0.94 V, and the anodic process at 1.18 and 1.1 V, respectively. Because of the high molecular weight of Mo₉Se₁₁, the reversible capacity was less than 50 mAh/g.

These results suggest that cluster based materials have great potential to serve as Mg battery cathodes. Further investigation is necessary to better explore this area both theoretically and experimentally.

Oxide cathodes

Oxides, including MnO₂, V₂O₅, MoO₃, and spinels, have been intensively studied as Mg battery cathodes. Manganese dioxide (MnO₂) has been investigated in Li-ion batteries due to its environmentally benign properties and low cost synthesis process date back to 1980s. MnO₂ has many polymorphic forms, including several open channel structures (α phase: 2 × 2 channel; β-phase: 1 × 1 channel; γ-phase: 1 × 2 channel), layered δ phase and spinel phase. These phases have been found to be suitable for the insertion of various cations with different sizes. In the last 3 years, α-MnO₂ has been intensively studied in our group as a cathode material for rechargeable Mg battery. This material showed a high capacity up to 280 mAh/g (Fig. 3) at the first discharge cycle using hexamethyldisilazide magnesium chloride (HMDS–MgCl) as electrolyte. ^{Reference Zhang, Yu, Nam, Ling, Arthur, Song, Knapp, Erlic, Yang and Matsui30} The Columbic efficiency of the first cycle exceeded 100%, possibly due to side reactions in the charge process such as Mg deposition and electrolyte decomposition. The reversible magnesiation/demagnesiation was proven by x-ray photoelectron spectroscopy (XPS) and x-ray absorption spectroscopy (XAS) of Mn states. However, the pristine state was not recovered after the battery was recharged to 3.0 V, suggesting the electrochemical reaction was not completely reversible. In addition, the discharge capacity quickly dropped to only half of the initial value and further faded at the following cycles. Similar observation was reported by Rasul et al. They prepared the K⁺ ion stabilized α-MnO₂ through hydrothermal method. When testing the performance of K⁺ ion stabilized α-MnO₂ in a three-electrode cell using 1 M Mg(ClO₄)₂–acetonitrile solution as electrolyte, the discharge capacity quickly dropped in the second cycle. The capacity of α-MnO₂ was increased by adding carbon black during hydrothermal synthesis. However, the capacity fading issue was not significantly improved.

Figure 3.

Galvanostatic cycle of α-MnO₂ at 19 μA/cm². Reprinted with permission from Ref. Reference Zhang, Yu, Nam, Ling, Arthur, Song, Knapp, Erlic, Yang and Matsui30. Copyright 2012 Elsevier.

To understand the reaction mechanism between α-MnO₂ and Mg, advanced analysis about the discharge product was carried out using high resolution transmission electron microscopy (HR-TEM) and soft x-ray absorption spectroscopy (sXAS). ^{Reference Arthur, Zhang, Ling, Glans, Fan, Guo and Mizuno31} During the magnesiation (discharge), an amorphous layer was formed on the surface of α-MnO₂ while the core still remained its crystallinity. Electron energy loss spectroscopy and sXAS analysis revealed that the amorphous shell consisted of reduced Mn³⁺, Mn²⁺ as well as Mg²⁺ species. Therefore, we interpret the amorphous product as gradually reduced manganese oxides mixed with magnesium oxide. The proposed reaction mechanism follows ^{Reference Arthur, Zhang, Ling, Glans, Fan, Guo and Mizuno31}

Recently, we systematically analyzed the electrochemical performance of several MnO₂ samples with different physical and chemical properties. ^{Reference Zhang, Arthur, Ling and Mizuno32} It was found that the surface area of MnO₂ cathode significantly affected the initial discharge capacity. Below 60 m²/g the initial discharge capacity rapidly increased with surface area. Above this value the initial discharge capacity remained nearly constant at about 250 mAh/g. This trend was not affected by the exact polymorphism and chemical composition of MnO₂. Therefore the magnesiation process was mainly controlled by the surface of MnO₂, consistent with the conclusion that the magnesiation of MnO₂ is unlikely to occur via the intercalation of Mg²⁺.

To understand these experimental results, first-principles calculations were performed to analyze the magnesiation behavior of α-MnO₂ by comparing the reactions following different reaction routes. ^{Reference Ling, Zhang, Arthur and Mizuno33} It was found that the conversion reaction that forms amorphous (Mg,Mn)O _x is thermodynamically more preferable than the intercalation. Even if the metastable intercalation could occur due to possible kinetic barrier that prevents direct conversion, the concentration of intercalated Mg is limited to α-Mg_0.125MnO₂, beyond which the structure of intercalated compound undergoes a strong tetragonal to orthorhombic distortion. The thermodynamic driven force for the conversion reaction is attributed to the high stability of MgO. Therefore it was speculated that the conversion reaction may be a general phenomenon for oxide based Mg battery electrodes.

The performance of other MnO₂ polymorphs was also studied. Rasul et al. compared the discharge performance of layered-MnO₂ and α-MnO₂. ^{Reference Rasul, Suzuki, Yamaguchi and Miyayama34} They found that the layered phase showed an initial capacity of 109 mAh/g and α-MnO₂ had a very high capacity of 310 mAh/g. The capacity of α-MnO₂ was further increased to 475 mAh/g when it was tested at higher temperature, 60 °C. Recently, Rasul et al. also reported the magnesiation performance of MnO₂ with even bigger tunnel (octahedral molecular sieves with 4 × 2 tunnel) and got an initial capacity of 78 mAh/g before serious capacity fading. ^{Reference Rasul, Suzuki, Yamaguchi and Miyayama35}

Kim et al. compared the electrochemical performance of nanosized λMnO₂ and α-MnO₂. ^{Reference Kim, Chang, Kim, Kim, Han, Lee, Lee and Doo36} In a three-electrode cell using 0.5 M Mg(ClO₄)₂ in acetonitrile electrolyte, λMnO₂ showed a higher capacity (330 mAh/g) and better cycliability. They believed that it was due to the facile interfacial reaction on the particle surfaces with higher Mg binding energy.

It should be noted that all these reports failed to observe clear voltage plateau in any MnO₂ phase. Instead, the voltage profile developed as a sloped curve with large discharge–charge hysteresis. These characters are typically signs of high kinetic battier during the cycling. In addition, the dissolution of Mn³⁺ species in the electrolyte and structural deformation caused by Jahn–Teller active Mn³⁺ are common phenomena in Mn based cathode research. ^{Reference Ling and Mizuno37} These results indicate that significant research efforts are still necessary to improve the performance of MnO₂ based cathodes.

An unusually polymorph of MgMn₂O₄ was predicted to have potential as Mg battery owning to the high Mg mobility. ^{Reference Ling and Mizuno38} It has a structure analogue to that of CaFe₂O₄, with Mg replacing Ca and Mn replacing Fe in the lattice. With one-dimensional triangular-like channel in the structure, the diffusion barrier for Mg migration at the composition of MgMn₂O₄ was predicted to be ∼0.40 eV, which well matches Li diffusion for many Li-ion battery cathodes. Besides, the voltage to remove Mg from this phase is predicted to contain several plateaus, all of which lie within the stability window of current electrolytes. If the full capacity of this compound can be utilized, the energy density of this cathode is ∼1.3 times to current Li-ion battery cathode.

Unfortunately, this unusual polymorph of MgMn₂O₄ is only thermodynamically stable at high pressures. Although it may still be kinetically stable at ambient conditions, the synthesis with sufficient amount is still challenging. Three synthetic routes have been suggested to obtain this compound, all of which require a pressure of at least ∼6 GPa. ^{Reference Ling and Mizuno38}

Another oxide compound that has been widely studies as Mg battery cathode is layered V₂O₅. Jiao et al. tested the performance of V₂O₅ nanotubes in the Grignard electrolyte of 0.25 M Mg(AlBu₂Cl₂)₂/THF solution. ^{Reference Jiao, Yuan, Wang, Cao and Wang39} The initial capacity was about 80 mAh/g with a slope voltage profile averaged at 0.5 V. Imamura et al. prepared V₂O₅/carbon composition and obtained a high initial capacity up to 550 mAh/g in a three-electrode cell using 1 M Mg(ClO₄)₂/acetonitrile electrolyte. ^{Reference Imamura, Miyayama, Hibino and Kudo40} Imamura et al. further studied the structural evolution upon magnesiation/demagnesiation process through x-ray diffraction (XRD) and Fourier transform infrared spectroscopy (FT-IR) techniques, which clearly identified the intercalation of Mg²⁺ ion in the layered structure. ^{Reference Imamura and Miyayama41}

Recent work by Aurbach's group on V₂O₅ significantly advanced our understanding of this cathode material in Mg battery system. ^{Reference Gershinsky, Yoo, Gofer and Aurbach42} They systematically investigated the morphology and structural change of V₂O₅ thin film in the three-electrode cell using 0.1 M Magnesium bis(trifluoromethanesulfonyl)imide/acetonitrile (Mg(TFSI)₂/CAN) or 0.5 M Mg(ClO₄)₂/ACN as electrolyte and carbon paper as counter electrode. A voltage plateau at 2.3 V was observed with the typical discharge capacity of 150 mAh/g at the current density of 0.5 µA/cm². As shown in Fig. 4, the capacity of V₂O₅ thin film cathode was stabilized to at least 35 cycles. The electrochemical intercalation/deintercalation of Mg was highly reversible as proven through cyclic voltammetry, XRD, Raman characterization. Scanning electron microscope (SEM) revealed minor morphology change during the cycling.

Figure 4.

(a) Galvanostatic titration curve of V₂O₅ thin-film electrode. (b) Cycling performance and Columbic efficiency of V₂O₅ thin-film electrode. Reprinted with permission from Ref. Reference Gershinsky, Yoo, Gofer and Aurbach42. Copyright 2013 American Chemical Society.

Zhou et al. carried out first-principles calculations to elucidate the magnetization mechanism of V₂O₅ cathode. ^{Reference Zhou, Shi, Cao, Zhang and Jiang43} They predicted the open circuit voltage (OCV) of lithium cell using V₂O₅ cathode at 2.84 V, while the OCV of Mg cell was 3.06 V. The diffusion barrier of Mg²⁺ in V₂O₅, however, was predicted to be significantly higher than that of Li⁺. For Li⁺ diffusion, the lowest energy barrier was 0.35 eV along b-axis, while for Mg²⁺ the barrier was 1.26 eV. This large barrier actually indicated the insertion rate would not be practical. The authors also predicted possible phase transformation during the insertion of Mg²⁺ ions. They concluded that the slow diffusion and phase transition should be two main challenges when using V₂O₅ as Mg battery cathode.

Wang et al. considered the usage of single-layered V₂O₅ as cathode candidate for Mg battery. ^{Reference Wang, Su and Deng44} They predicted the adsorption of Mg ions adsorbs on single-layered V₂O₅ occurred at a voltage of 2.03 V. The diffusion of Mg, however, was not enhanced even in single-layered V₂O₅. Instead, the activation energy barriers of Mg diffusion in single-layered and bulk V₂O₅ were 1.40 and 1.36 eV, respectively. It indicates that Mg mobility cannot be enhanced by decreasing the thickness of V₂O₅ material.

Some other oxides have also been reported as Mg battery cathode in recent years. Sutto et al. investigated Co₃O₄ and RuO₂ as cathode materials for Mg batteries in ionic liquid electrolytes (MMBITFSI and MMOITFSI) using a two-electrode cell with Mg as counter and reference electrodes. ^{Reference Sutto and Duncan45,Reference Sutto and Duncan46} An initial capacity of 74 mAh/g with a voltage plateau at 1.4 V was observed for Co₃O₄ cathode. The first discharge capacity of RuO₂ reached ∼100 mAh/g with surprisingly high voltage plateau at 3.5 V. However, both cathode materials suffered serious capacity fading. The structures of both oxides were significantly changed after discharge. However the structure of the recharged phase was not analyzed.

Another oxide attracted attention is layered MoO₃. Aurbach's group studied the magnesiation property of MoO₃ thin film. The experiment was performed in a three-electrode configuration using 0.1 M MgTFSI₂/AN as electrolyte and porous carbon as counter electrode. ^{Reference Gershinsky, Yoo, Gofer and Aurbach42} A voltage plateau at 1.7 V with the capacity of about 220 mAh/g was observed. Interestingly, the voltage hysteresis of MoO₃ was much higher than that of V₂O₅ thin film (0.4 V versus 0.1 V), which was attributed to the lower diffusivity of Mg²⁺ in MoO₃ and relatively bigger MoO₃ particle size.

Spinel oxides are one of the biggest families of cathodes that have been studied in Li-ion battery. Unlike layered LiCoO₂, the spinel compounds offer three-dimensional network of interstitial sites for Li diffusion. In Mg battery research, Ichitsubo et al. reported the study of Co and Ni spinel oxides as the potential high voltage cathode materials. ^{Reference Ichitsudo, Adachi, Yagi and Doi47} The performance of MgCo₂O₄ and Mg_0.67Ni_1.33O₂ were tested in two-electrode cell using Mg metal as anode and 1 M Mg(ClO₄)₂ in acetonitrile solution as electrolyte. Both showed relative high OCV (∼3.5 V). However, the rate capability was extremely low due to the sluggish Mg²⁺ diffusion in the host materials. For instance, the authors estimated it took about 300 h to charge 4% of the theoretical capacity of MgCo₂O₄ (260 mAh/g). Nevertheless, those Co and Ni spinel oxides can be promising cathode materials for magnesium battery providing that the Mg²⁺ diffusivity can be significantly improved and novel electrolyte can be developed to sustain the high working potential without passivation problem.

To find oxides suitable as Mg battery cathodes, Liu et al. performed first-principles calculation for a series of spinel compounds MgA₂O₄ with A = Ti to Ni. ^{Reference Liu, Rong, Malik, Canepa, Jain, Ceder and Persson48} All these compounds exhibit lower voltage than that of Li analogues. It is mainly a result of the high redox potential of Mg/Mg²⁺. However, the bivalency of Mg²⁺ ions still makes it promising as high energy density cathode. For instance, the capacity of LiMn₂O₄ is 143 mAh/g, whereas the gravimetric capacity of MgMn₂O₄ is ∼270 mAh/g, which compensate the sacrifice of the lower voltage.

The diffusion of Mg²⁺ ions was examined at high vacancy and dilute vacancy limitations, which were believed to set the bound for the diffusion. They found that the migration barrier at high vacancy limit is always higher compared to the dilute vacancy limit. For Li migration in M₂O₄ (M = Mn, Co, Ni, Cr), the barriers all lied within ∼400 to 600 meV in the empty lattice limit. However, Mg²⁺ has the barrier about ∼200 to 400 meV higher. It suggested that the diffusivity of Mg might be 4–5 orders of magnitude slower than Li in the spinel phase. Thus the sluggish diffusion of Mg²⁺ remains as the biggest challenge to use spinel cathode. The best candidate seems to be spinel MnO₂, which has a barrier ∼650 meV. ^{Reference Liu, Rong, Malik, Canepa, Jain, Ceder and Persson48}

Consistent with Liu et al.'s report, Kim et al. reported the observation of reversible Mg intercalation into spinel-MnO₂ using aqueous Mg(NO₃)₂ eletrolyte (1 M) and Pt as the counter electrode. ^{Reference Kim, Philips, Key, Yi, Nordlund, Yu, Bayliss, Han, He, Zhang, Burrell, Klie and Cabana49} The discharge delivered a capacity of 190 mAh/g. Using a combination of analysis techniques such as scanning transmission electron microscopy (STEM)/energy dispersive x-ray analysis (EDX) and XRD, they found the results were consistent with the formation of MgMn₂O₄, which was distinct with the amorphourization that was observed in the magnesiation of α-MnO₂. It should be noted that the spinel-MnO₂ was prepared by acidic leaching of lithium from spinel-LiMn₂O₄, which also generated nanoflake-like morphology potentially benefit to improve Mg diffusion with shorter migration distance.

Polyanion cathodes

Besides the oxide family, another classical type of intercalation cathodes is polyanion compound. Compared with oxides, the induction effect of the polyanion groups moves the oxygen p-orbital to deeper level, thus generally provides better chemical stability of the cathodes. Research for polyanion compounds as Mg battery cathode mostly used 3d transition metal (V to Ni) as redox center to balance the charge neutrality when guest Mg is inserted or removed.

The most prominent polyanion cathode in Li-ion battery is olivine LiFePO₄, which was first reported by Goodenough in 1997. ^{Reference Padhi, Nanjundaswamy and Goodenough50} After that other LiMPO₄ olivine compounds with M stands for Mn, Fe, Co, and Ni or their combinations have been extensively studied in Li-ion battery. In LiMPO₄ M exists as M²⁺ ions. If Li is replaced by Mg and phosphorus is replaced by silicon, it ends as MgMSiO₄ where M remains as M²⁺. In fact, the name of the mineral olivine comes from MgMnSiO₄. Fully extracting Mg from MgMSiO₄ ends at MSiO₄, where M exists as 4+. It gives a theoretical capacity of ∼308 mAh/g.

Nuli and her co-workers have systematically examined the performance of Mg olivine cathodes. The performance of these compounds as Mg battery cathode was first reported for Mg_1.03Mn_0.97SiO₄. ^{Reference Feng, Yang, NuLi, Wang, Wang and Wang51} Here the slight off-stoichiometry comes from the anti-site defects formed by switching the position of Mg and transition metal M ions, which is a common phenomenon in olivine compounds. The performance of Mg_1.03Mn_0.97SiO₄ cathode was examined using a CR2016 coin cell with Mg-strip counter electrode and Mg(AlCl₂EtBu)₂/THF (0.25 M) electrolyte. Figure 5 showed the discharge profile for Mg_1.03Mn_0.97SiO₄. Mg_1.03Mn_0.97SiO₄ prepared by solid-state reaction only delivered a capacity of 43.2 mAh/g at the current density of 6.3 mA/g. After ball-milling it with acetylene black, its capacity was improved to 64.5 mAh/g with discharge voltage plateaus at 1.6 and 1.1 V. For the sol–gel derived Mg_1.03Mn_0.97SiO₄/C electrode, the discharge capacities were further improved to 244, 126, and 76 mAh/g at current densities of 3.1, 6.3, and 15.7 mA/g, respectively. This increased capacity was contributed to the smaller particle size of the active material.

Figure 5.

(a) Discharge profile of Mg_1.03Mn_0.97SiO₄ and Mg_1.03Mn_0.97SiO₄/carbon cathode synthesized with solid state method. (b) Improved performance of Mg_1.03Mn_0.97SiO₄/C cathode prepared with sol–gel process. Reprinted with permission from Ref. Reference Feng, Yang, NuLi, Wang, Wang and Wang51. Copyright 2008 Elsevier.

Improved discharge capacities of 200 mAh/g (0.3 C rate) and 150 mAh/g (C/5 rate) were achieved using mesoporous Mg_1.03Mn_0.97SiO₄. ^{Reference NuLi, Yang, Li and Wang52} This performance improvement was attributed to the high surface area of the active mass. Nuli et al. also synthesized multiwalled carbon nanotubes/Mg_1.03Mn_0.97SiO₄ composite hierarchical nanostructure, which showed a steady and stable discharge capacity of 100 mAh/g (at C/2 rate) up to 30 cycle. ^{Reference NuLi, Yang, Wang and Li53}

The performances of MgFeSiO₄, MgCoSiO₄, and MgNiSiO₄ were also examined. MgFeSiO₄ exhibited a steady discharge capacity ∼125 mAh/g at C/10 rate and retain 91.4% of its initial capacity at 20th cycles. ^{Reference Li, NuLi, Yang, Yilinuer and Wang54} Micrometer sized MgNiSiO₄ olivine compound exhibited discharge capacity of 121 mAh/g at a rate of 10 mA/g. Bulk MgCoSiO₄ showed a small discharge capacity of 70.2 mAh/g at 0.1 C. ^{Reference Sun55} If hierarchically porous MgCoSiO₄ architecture was used, MgCoSiO₄ delivered a discharge capacity 80 mAh/g (1 C rate) at the 20th cycle. ^{Reference NuLi, Zheng, Wang, Yang and Wang56}

Besides olivine compounds, several other polyanion compounds were also reported as Mg battery cathodes. With the aim to improve Mg diffusion, Huang et al. synthesized a stoichiometric fluoro-phosphate, MgFePO₄F (MFPF). ^{Reference Huang, Masese, Orikasa, Mori, Minat, Tassel, Kobayashi, Kageyama and Uchimoto57} The monoclinic structure of MFPF (space group: I2/a) is isostructural to both triplite and wagnerite phases, which contains three-dimensional framework for Mg diffusion. When testing in a three-electrode configuration, the average working potentials of MFPF were measured at ∼2.6 V versus Mg/Mg²⁺ in Mg-ion cell and 3.1 V versus Li/Li⁺ in Li-ion cell. However, the capacity of MFPF was not high. The reversible capacity was ∼35 mAh/g at C/20 rate.

Orikasa et al. reported a metal-stable phase of MgFeSiO₄. ^{Reference Orikasa, Masese, Koyama, Mori, Hattori, Yamamoto, Okado, Huang, Minato, Tassel, Kim, Kobayashi, Abe, Kageyama and Uchimoto58} The synthesis of metal-stable MgFeSiO₄ included the electrochemical extraction of 2Li from Li₂FeSiO₄ followed by the electrochemical Mg insertion. The discharge processes in Mg electrolyte deliver a capacity of approximately 330 mAh/g. The average charge–discharge potential was 2.4 V. The energy density was estimated to be 746 W h/kg. Orikasa et al. also tested the performance of a magnesium battery using MgFeSiO₄ and Mg metal as the cathode and anode, respectively, and Mg(TFSI)₂–triglyme as the electrolyte. A reversible charge–discharge capacity of 166 mAh/g was obtained. Only half of the theoretical capacity of the cathode material could be obtained which was contributed to the high polarization effect.

The formal valence of the transition metal ions in olivine MgMSiO₄ is +2. Upon the full loss of Mg²⁺ ions, transition metal ions are oxidized to +4. First-principles calculations based on density functional theory (DFT) revealed that the insertion of magnesium occurs via two steps, each of which is characterized by a unique redox couple. ^{Reference Ling, Banerjee, Song, Zhang and Matsui59} In the first stage, from MgMSiO₄ to Mg_0.5MSiO₄, the redox couple is M²⁺/M³⁺. In the second stage, from Mg_0.5MSiO₄ to MSiO₄, the redox couple is M³⁺/M⁴⁺.Therefore the redox reactions are written as

The calculated voltages for Li and Mg insertion into olivine compounds are shown in Fig. 6. All the magnesiation voltages were 0.7–0.9 V lower than those of the lithiation. This difference mainly originates from the anodic potential difference (0.67 V) with additional contribution from the different stability of Mg and Li in the same cathode lattice. Except for Fe²⁺/Fe³⁺, the calculated voltages were 3–4 V for M²⁺/M³⁺ redox couples and about 4 V for M³⁺/M⁴⁺ redox couples. Note the voltages predicted for Mg insertion were much higher than the experimental value from Nuli et al.'s reports. This discrepancy was expected to come from side reactions during the charge–discharge process.

Figure 6.

Voltage calculated for the lithiation and magnesiation of olivine compounds. Reprinted with permission from Ref. Reference Ling, Banerjee, Song, Zhang and Matsui59. Copyright 2012 Royal Society of Chemistry.

Because the crucial challenge in the research of Mg battery cathode is to improve the mobility of Mg²⁺ ions, theoretical calculations can be extremely helpful to predict candidates with high Mg²⁺ mobility. Wu et al. predicted the performance of tavorite-Mg_0.5FeSO₄F as Mg battery cathode. ^{Reference Wu, Gao, Wu, Liu, Yang, Zhou and Wang60} The calculated voltage for Mg extraction from Mg_0.5FeSO₄F is about 2.52 V. This value was about 1.1 V lower than that of lithiation (3.62 V). The insertion of 1 Mg reduced two FeO₄F₂ units instead of reducing only one FeO₄F₂ unit, similar to that revealed for olivine compounds. The energy barrier for Mg-vacancy diffusion along the [010] direction is 0.36 eV, much lower than that of many bulk materials. An estimated diffusion coefficient using the calculated activation energy is on the order of 10⁻⁹ cm²/s. These results suggest Mg_0.5FeSO₄F can serve as a promising potential candidate for magnesium battery cathode materials.

Wu et al. predicted the performance of MgVPO₄F as Mg battery cathode. ^{Reference Wu, Gao, Wu, Liu, Yang, Zhou and Wang61} The structure of MgVPO₄F was adopted to be isostructural to LiVPO₄F. The theoretical capacity of MgVPO₄F is about 312 mAh/g. The average voltage to extract Mg was predicted to have two plateaus at 2.6 and 1.5 V, corresponding to the redox couples of V⁴⁺/V³⁺ and V³⁺/V²⁺, respectively. The diffusion barriers were calculated along [100], [010], [101], and [111] directions in MgVPO₄F. The lowest energy barrier for Mg ion diffusion along [111] direction is 0.704 eV. The activation energies for hops in other direction are at least 700 meV higher, suggesting MgVOPO₄F is indeed a 1D Mg conductor. The diffusion coefficient is estimated in the order of 10⁻¹⁴ cm²/s.

Transiton metal dichalcogenide

Transition metal dichalcogenides (MX₂, M = transition metal and X = S, Se, and Te) such as TiS₂ and VS₂ were among the first generation of Li-ion battery cathodes dated back to late 1970s. A few reports tested the performance of these compounds in Mg battery cells. Chen and his group investigated the performance of highly exfoliated graphene-like MoS₂ (G-MoS₂) composed single- and several-layer of highly exfoliated MoS₂. ^{Reference Liang, Feng, Yang, Ma, Liang and Chen62} To enhance the kinetics of the anode, Mg nanoparticle (N-Mg) anode was also prepared. The as-prepared samples were spread into Cu (cathode) or Al (anode) foam and the electrochemical test was carried out using CR2032 coin-type cells with a THF solution of Mg(AlCl₃Bu)₂ as the electrolyte. The performance of different cathode [G-MoS₂ and bulk MoS₂ (B-MoS₂)] and anode (N-Mg and bulk-Mg) combinations were shown in Fig. 7. All cells exhibited average operating voltages around 1.8 V except for the B-MoS₂/B-Mg cell, which worked at a slightly lower discharge voltage of 1.64 V. The best performing G-MoS₂/N-Mg cell exhibited a discharge capacity of 170 mAh/g. Subsequent discharge–charge cycling tests revealed excellent capacity retention of the G-MoS₂/N-Mg cell. After 50 cycles, 95% of the initial capacity was maintained.

Figure 7.

Cycling behaviors of the cells fabricated with B- or G-MoS₂ cathode and B- or N-Mg anode with a discharge rate of 20 mA/g. Reprinted with permission from Ref. Reference Liang, Feng, Yang, Ma, Liang and Chen62. Copyright 2011 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

Chen et al. carried out a first-principles DFT study focusing on key issues relating to magnesium adsorption sites, theoretical capacity, and diffusion kinetics. ^{Reference Yang, Li, Zhang, Tao and Chen63} In their simulation, MoS₂ was treated as zigzag nanoribbons. A maximum theoretical capacity of 223.2 mAh/g was achieved by double-side Mg adsorptions. It was noted that the observed experimental capacity was ∼170 mAh/g. The difference was contributed to possible different crystal structures of MoS₂ host in the experiments.

The Mg diffusion pathway on the zigzag MoS₂ nanoribbon was identified as passing two adjacent top sites mediated by the nearest neighboring hollow site. The activation barrier of this process was 0.48 eV, much smaller than the barrier in bulk MoS₂, 2.61 eV. This theoretical result combined with the experimental observation emphasized the necessity of rational morphology control of electrode materials to enhance the performance of rechargeable Mg electrodes.

The performance of nanostructured MoS₂ in Mg battery was reported by Li and Li. ^{Reference Li and Li64} The as-prepared samples was fabricated as cathode in nickel form matrix, and the electrochemical test was conducted using THF solution of Mg(AlCl₃Bu)₂ as the electrolyte and Mg as the anode. The performance varied cell by cell in the experiments. It was believed that the different sizes and nanostructures of MoS₂ caused the different features of the Mg²⁺ intercalation. The MoS₂ nanorods and fullerene-like nanoparticles had small particle size and relative large amount of broken tips, which might be suitable for ions intercalation. Moreover, the interlayer distance of MoS₂ fullerene-like nanoparticles were slightly expanded because of the tension. This might also make it easy for the intercalation of Mg²⁺ ions. For comparison, the commercial MoS₂ powder with an average particle size of about 400 nm showed nearly zero capacity for Mg insertion.

Because the diffusion of cations is strongly affected by the distance between slabs, a general strategy to enhance Mg diffusion is to expand the interlayer distance of layered cathode. ^{Reference Doe, Downie, Fischer, Lane, Morgan, Nevin, Ceder, Persson and Eaglesham65,Reference Liang, Yoo, Li, Shuai, Calderon, Hernandez, Grabow and Yao66} With this approach, Liang et al. successfully improved the performance of MoS₂ by expanding the interlayer distance from 0.62 to 1.45 nm with controlled pre-insertion of poly(ethylene oxide). ^{Reference Liang, Yoo, Li, Shuai, Calderon, Hernandez, Grabow and Yao66} The average Mg diffusivity over the entire intercalation process measured with galvanostatic intermittent titration technique is 4.4 × 10⁻¹² cm²/s for expanded MoS₂, while for in commercial MoS₂ the diffusivity is in the order of 10⁻¹³ cm²/s once the intercalation begins. Such two orders-of-magnitude boost of Mg diffusion greatly improved the electrochemical performance of MoS₂ cathode. The voltage profile for the expanded MoS₂ at different current densities is shown in Fig. 8. The capacity at low current density was 75 mAh/g. Even at current density as high as 500 mA/g, the expanded MoS₂ still kept a capacity of ∼20 mAh/g. Remarkably, the expanded MoS₂ also showed good cyclability at least to 30 cycles, as well as good Columbic efficiency especially at high current densities.

Figure 8.

Performance of MoS₂ expanded by the insertion of poly(ethylene oxide) in Mg battery. Reprinted with permission from Ref. Reference Liang, Yoo, Li, Shuai, Calderon, Hernandez, Grabow and Yao66. Copyright 2015 American Chemical Society.

Another transition metal dichalcogenide that was tested in Mg cell was WSe₂. ^{Reference Liu, Luo, Mu, Wang, Chen and Shen67} The electrochemical properties of WSe₂ nanowires with diameters of ∼100 nm were evaluated in coin-shaped cells. The discharge platform was approximately 1.6 V with very little decay of specific capacity during cycling. The reversible specific capacity was around 203 mAh/g. The rate performance of the WSe₂ nanowire-based electrode was measured at different current densities ranging from 100 to 800 mA/g for 50 cycles between 0.3 and 3 V. Even at a high current density of 800 mA/g, the specific capacity is still kept at 142 mAh/g. These results indicated the very good structural stability of the WSe₂ nanowire-based electrodes.

Oxygen (air) cathode

Motivated by recent progress on Li-oxygen battery, Shiga et al. studied the direct usage of oxygen as cathode for Mg–oxygen battery. ^{Reference Shiga, Hase, Kato, Inoue and Takechi68,Reference Shiga, Hase, Yagi, Takahashi and Takechi69} Ideally the reaction between Mg and O₂ occurs via a four-electron transfer in organic solvents as

The theoretical voltage for this reaction is 3.124 V. Thus the Mg–O₂ battery has the potential to deliver energy levels of 1000 (W h)/L if the cathode delivers a capacity more than 320 (mA g)/cc. Unfortunately, the conductivity of the product, magnesium oxide, is very low, while its stability is very high thermodynamically and electrochemically. At ambient temperatures, MgO formed at the O₂-electrode cannot be decomposed. ^{Reference Shiga, Hase, Kato, Inoue and Takechi68}

To make a rechargeable Mg–O₂ battery, Shiga et al. proposed to add redox active species into the electrolyte solution to enhance the dissolution and decomposition of MgO. One of such additives is iodine, which forms complex with organic solvent by a charge-transfer interaction between the functional group in the solvent and the s bond of the iodine molecule. ^{Reference Shiga, Hase, Kato, Inoue and Takechi68} Figure 8 shows discharge–charge curves of a Mg–O₂ battery at 60 °C with a carbon electrode containing MgI₂ in 0.5 M Mg(ClO₄)₂–Dimethyl sulfoxide (DMSO). The battery showed two steps in the cell voltage during the first discharging, corresponding to the reaction of Mg²⁺ with iodine at ∼1.5 V and the discharge of Mg–O₂ battery at ∼1.25 V. The total discharge capacity was 2131 mAh/g cathode. In the charge, a plateau was observed at about 2.2 V with a total charge capacity was 1590 mAh/g. If no iodine was added in the electrolyte, the Mg–O₂ battery had a large discharge capacity but no charging activity.

Shiga et al. also reported the usage of the 2,2,6,6-tetramethylpiperidine-oxyl–anion complex to catalyze the decomposition of MgO in the charge of Mg–oxygen battery. ^{Reference Shiga, Hase, Yagi, Takahashi and Takechi69} Figure 9 shows the discharge–charge voltage profile for Mg–oxygen battery with a poly(2,2,6,6-tetramethylpiperidinyloxy-4-yl methacrylate) (PTMA) cathode at 60 °C. The discharge capacity of the first cycle was 737 mAh/g while the initial cycle charging capacity was 460 mAh/g. In the second cycle, the discharging capacity was 399 mAh/g, and the charging capacity was as high as 175 mAh/g. The Mg–O₂ battery exhibited rechargeable behavior over several discharge/charge cycles.

Figure 9.

Discharge–charge profiles of the non-aqueous Mg–O₂ battery with iodine at 60 °C. Reprinted with permission from Ref. Reference Shiga, Hase, Kato, Inoue and Takechi68. Copyright 2013 Royal Society of Chemistry.

Sulfur cathode

Another oxygen family element, sulfur, also reacts with magnesium. The theoretical capacity of sulfur is 1671 mAh/g or 3459 mAh/cc. The combination of a magnesium anode and a sulfur cathode is of great interest because the theoretical energy density of this battery is estimated to be over 4000 W h/L, which is approximately twice that of a Li ion battery composed of a graphite anode and a cobalt oxide cathode. It indicates Mg–S battery can serve as a high energy storage system. ^{Reference Kim, Arthur, Allred, Zajicek, Newman, Rodnyansky, Oliver, Boggess and Muldoon7}

Compared to the substantial progress made on Li/S batteries, the Mg/S battery is still in a very early stage of research and development. The biggest challenge to realize a rechargeable Mg–S cell is to avoid the direct reaction between the electrophilic sulfur cathode and the nucleophilic electrolyte. ^{Reference Kim, Arthur, Allred, Zajicek, Newman, Rodnyansky, Oliver, Boggess and Muldoon7} Therefore, the development of Mg–S battery heavily relies on the research of novel electrolyte. The first proof-of-concept of Mg–S battery was reported by Muldoon et al. at Toyota, using a metallic magnesium anode, a sulfur cathode dispersed in carbon black, combined with a nonnucleophilic electrolyte based on a recrystallized HMDS–AlCl₃ in a coin cell configuration. ^{Reference Kim, Arthur, Allred, Zajicek, Newman, Rodnyansky, Oliver, Boggess and Muldoon7} A typical Mg/S coin cell displayed a capacity of 1200 mAh/g for the first discharge. The starting potential is 0.55 V and slowly increases up to 0.89 V during the discharge process. The second discharge capacity dramatically decreased to 394 mAh/g. The severe capacity fading was attributed to the polysulfide or sulfur dissolution, which also explains the overcharging behavior observed in Fig. 10.

Figure 10.

Discharge and charge profiles of Mg/S coin cell. Reprinted with permission from Ref. Reference Kim, Arthur, Allred, Zajicek, Newman, Rodnyansky, Oliver, Boggess and Muldoon7. Copyright 2011 Nature Publishing Group.

To improve the performance of Mg–S battery Zhao-Karger et al. used (HMDS)₂Mg based diglyme and tetraglyme electrolyte solutions to build Mg/S batteries and N-methyl-N-butylpiperidinium bis(trifluoromethanesulfonyl)imide (PP14TFSI) as an additive to the electrolytes. ^{Reference Zhao-Karger, Zhao, Wang, Diemant, Behm and Fichtner70} The active sulfur cathode used a highly ordered mesoporous carbon (CMK-3) for the encapsulation of sulfur. The highest discharge capacity was recorded around 800 mAh/g in the first cycle and decreased to 350 mAh/g in the second cycle. After more than 20 cycles it remained a reversible capacity of about 260 mAh/g.

Based on their data, Zhao-Karger et al. proposed that the discharge process of Mg–S battery is divided in three reductive steps. ^{Reference Zhao-Karger, Zhao, Wang, Diemant, Behm and Fichtner70} The first step is a solid–liquid two-phase reduction from elemental sulfur to MgS₈, followed by subsequently dissolving of MgS₈ into electrolyte to become a liquid cathode and transforms to low-order polysulfides (MgS₄). The overall electrochemical reaction for the first step of Mg/S battery could be described as

The second step is a liquid–solid two-phase reduction from the dissolved low-order polysulfide to MgS₂ corresponding to the second discharge plateau, which results in a theoretical capacity of the Mg/S cell up to 840 mAh/g and can be described as

The third discharging step is a reduction from MgS₂ to MgS expressed as

The final product, MgS, is insoluble in ethereal solvents and the process shown in Eq. (7) consequently suffers from high kinetic barriers and high polarization. The latter stages of the conversion reactions in Mg/S batteries proceed sluggishly and limits the initial discharge capacity of about 800 mAh/g, corresponding to the electrochemical reduction of S₈ to MgS₂.

Mg–anion battery

Due to the low diffusivity of Mg²⁺ ions in solid state lattice, an alternative solution to secure practically high rate capability is to utilize another redox reaction on the cathode side that replaces the intercalation reaction and balances the electron transfer. This actually is a novel concept for rechargeable Mg battery reported by our group, where the charge transfer is achieved via simultaneous transport of Mg²⁺ cations and halide anions during electrochemical cycling and the charge balance derived from Mg²⁺ and X⁻ is compensated in the electrolyte media. We have successfully demonstrated the high rate capability of this conceptual Mg battery using AgCl as cathode material and Cl⁻ containing Grignard electrolyte [Fig. 11(a)]. ^{Reference Zhang, Ling and Mizuno71} The electrochemical reaction during the operation of this battery is the decomposition and formation of metal chloride on the cathode, together with the dissolution and deposition of metallic Mg on the anode. The electrochemical reactions can be described as follows:

Figure 11.

(a) Discharge–charge voltage profiles of Mg/AgCl battery at constant current of 0.1 mA. (b) Cycling performance of this cell at different C rates. The inset shows the voltage profiles at 5 C rate. Reprinted with permission from Ref. Reference Zhang, Ling and Mizuno71. Copyright 2015 Royal Society of Chemistry.

Figure 11(b) shows the discharge profiles at different C rates. The theoretical capacity of this cathode is 186 mAh/g. This value was almost achieved at 0.1 C rate. The capacity observed at 10 C still remains 104 mAh/g (55% of the theoretical capacity).

Fitchner's group reported the usage of Mg anode in a halide ion battery cell. ^{Reference Zhao, Li, Zhao-Karger, Gao, Fink, Shen and Fichtner72} They applied metal oxychlorides (BiOCl, FeOCl) as cathode materials, Mg/C composition as anode and a mixture of 0.5 M PP14Cl in PP14TFSI as electrolyte. The BiOCl cathode had an initial discharge capacity of 102 mAh/g, which is 99% the theoretical capacity (103 mAh/g). A charge capacity of 69 mAh/g was recovered in the first cycle, showing a Columbic efficiency of 68%.

Mg–cation battery

Another hybrid ion configuration is Mg–cation cell, where the anode reaction utilizes the electrochemical deposition/dissolution of Mg and the cathode reaction is the insertion of another cation species. Cheng et al. applied Mg metal, mixture of All-Phenyl Complex (APC) and LiCl in THF solution and CP-Mo₆S₈ as anode, electrolyte and cathode, respectively. ^{Reference Cheng, Shao, Zhang, Sprenkle, Liu and Li73} Due to the difference of diffusivity of Li⁺ and Mg²⁺ in CP, Li⁺ ion intercalates into cathode ahead of Mg²⁺ ion. On the other hand, the relative higher standard potential of Mg²⁺ allows Mg metal deposits on anode side. Figure 12 shows typical charge–discharge profiles of a hybrid cell operated at different C-rates. The hybrid cells had two discharge plateaus at 1.66 and 1.29 V and reached a specific capacity of 126 mAh/g at 0.1 C. The capacity had a slight decrease with increase of the C-rate, but still maintained 105 mAh/g at 15 C (83% retention).

Figure 12.

Charge–discharge profiles of the Mg–Li hybrid cell at different C-rates with CP cathode. Reprinted with permission from Ref. Reference Cheng, Shao, Zhang, Sprenkle, Liu and Li73. Copyright 2014 Royal Society of Chemistry.

Cho et al. investigated the reaction mechanism of Mg–Li hybrid battery both experimentally and theoretically. ^{Reference Cho, Aykol, Kim, Ha, Wolverton, Chung, Kim and Cho74} Using DFT calculations, they found that the intercalation of Mo₆S₈ cathode can be tuned by varying the activity of Li⁺ ions in the electrolyte. With high Li⁺ activity the cathode reaction prefers the insertion of Li instead of Mg. By controlling the insertion chemistry using a Li–Mg ions dual-salt electrolyte, they achieved ultrafast discharge at 20 C with 93.6% of capacity retention and at 30 C with 87.5% of capacity retention, respectively, at room temperature.

Similar Mg–Li hybrid battery was also explored by Yagi et al. They used metal Mg as the anode, LiFePO₄ as the cathode and THF solution of two kinds of salts, LiBF₄ and phenylmagnesium chloride (PhMgCl) as the electrolyte. ^{Reference Yagi, Ichitsubo, Shirai, Yanai, Doi, Murase and Matsubara75} The discharge capacity at the 1st cycle was about 124 mAh/g while the 1st charge capacity was 170 mAh/g in the hybrid electrolyte. The discharge capacity in 2nd cycle dropped to about 96 mAh/g, which was attributed to possible electrolyte decomposition during charge in addition to the self discharge. Especially, the possible reaction between BF₄ and PhMgCl would generate B(Ph)₄, which might lower the stability of the electrolyte.

It is now recognized that the design of Mg–Li hybrid cell request special attention to the choice of hybrid electrolyte and Li cathode. The presence of lithium salt in the Mg complex electrolyte directly affects its electrochemical properties. The chosen cathode must be compatible with the complex electrolyte, i.e., it should have redox potential within the electrochemical stability window of the complex electrolyte and also remains chemically inert to electrolyte components to avoid any parasitic reactions. On the basis of these considerations, Gao et al. used TiS₂ as the cathode and APC–LiCl in THF as the electrolyte in their experiments. ^{Reference Gao, Han, Zhu, Suo, Luo, Xu and Wang76} TiS₂ cathode barely delivers any capacity in pure Mg cell. ^{Reference Amir, Vestfrid, Chusid, Gofer and Aurbach77} In Mg–Li hybrid cell, stable electrochemical chemical activity was recorded as shown in Fig. 13. Despite a low initial Columbic efficiency of 90% due to the trapping of inserted Li between TiS₂ layers, the discharge–charge curve showed highly reversible performance. No capacity decay was observed for at least 400 cycles with Columbic efficiency as high as 99.5% except for the first few cycles. The theoretical specific capacity and specific energy of the mixed-ion battery are 161.0 mAh/g and 209.3 W h/kg taking into account the weight of lithium salt.

Figure 13.

Voltage profile of Mg/PhMgCl–AlCl₃–LiCl/TiS₂ battery. Reprinted with permission from Ref. Reference Gao, Han, Zhu, Suo, Luo, Xu and Wang76. Copyright 2015 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

Prussian blue based cathode

Because of the cost-friendly synthesis and the good rate performance, Prussian blue and its analogues recently have attracted much attention as a potential choice of grid scale storage electrodes. Research in this field focuses on Li and Na battery, with little attention paid to Mg battery. Theoretically it was predicted that the magnesiation of iron hexacyanoferrate, Fe(Fe[CN]₆), occurs with two voltage plateaus at 1.93 and 1.40 V, respectively. ^{Reference Ling, Chen and Mizuno78} The maximum capacity is ∼200 mAh/g, corresponds to the insertion/extraction of 1 Mg per formula. Thus the energy density of this compound is not comparative to current Li-ion battery cathode. Nonetheless, the low cost and potentially high rate performance still indicate it may have potential in large scale energy storage.

Cui and his group have extensively studied the performance of hexacyanoferrates in aqueous solutions. Recently they reported the performance of nickel hexacyanonferrate (NiHCF) as divalent ion battery electrode in aqueous electrolyte solutions. ^{Reference Wang, Wessells, Huggins and Cui79} The half-charge reaction potentials versus standard hydrogen electrode (SHE) were 0.60 V (Fig. 14). There was a distinct second plateau in the potential profile at high C rates, suggesting the possibility of a two-step insertion reaction. From C/5 to 10 C rate the retention of specific capacity of 63% was recorded. Besides, only marginal voltage hysteresis was observed at high cycling rate. These results suggested excellent rate performance of NiHCF for Mg (de)intercalation.

Figure 14.

(a) Discharge–charge voltage profile of NiHCF upon galvanostatic cycling with Mg²⁺. (b) Cycling profile of this cell at 5 C rate. Reprinted with permission from Ref. Reference Wang, Wessells, Huggins and Cui79. Copyright 2013 American Chemical Society.

NiHCF also exhibited excellent cycling stability. When cycled between 0.22 and 0.92 V versus SHE at 5 C it retained 65% of initial capacity after 2000 cycles. Round-trip energy efficiency reached 82% after 2000 cycles. If a small concentration of additional Ni²⁺ (20 mM) was added in the electrolyte to prevent the dissolution of the active material, the energy efficiency was improved to 93%. The capability to react with divalent insertion cations at high rates with unprecedented cycle life and efficiency is essentially interesting for the usage in large scale applications.

Mizuno et al. examined the performance of K_0.1Cu[Fe(CN)₆]_0.7·3.6H₂O in a 1 M Mg(NO₃)₂ aqueous electrolyte. ^{Reference Mizuno, Okubo, Hosono, Kudo, Oh-ishi, Okazawa, Kojima, Kurono, Nishimura and Yamada80} A specific capacity of approximately 60 mAh/g was reversibly obtained for both cathodic and anodic processes, corresponding to 0.3 Mg²⁺ intercalation/deintercalation per formula unit if this capacity is assumed to entirely come from Mg²⁺ (de)intercalation. The redox process involved the participation of both Fe and Cu ions with the voltage profile containing a considerable slope over the entire voltage range. At the specific current of 0.1 and 1 A/g, the capacity dropped to 50 and 37 mAh/g, respectively. The retained capacity at 1 A/g reached 74% of the initial maximum capacity, suggesting high rate capability of this material in aqueous solutions.

An interesting question that remains for future research is the intercalation mechanism in aqueous solutions. ^{Reference Wang, Wessells, Huggins and Cui79,Reference Mizuno, Okubo, Hosono, Kudo, Oh-ishi, Okazawa, Kojima, Kurono, Nishimura and Yamada80} The ionic size of Mg²⁺ is quite small compared to typical ions (K⁺, Ba²⁺, etc.) that stabilize the hexacyanonferrate framework. However, the intercell bottleneck radius of the hard sphere model of Prussian blue analogues is about 1.6 Å, while the size of hydrated Mg²⁺(H₂O)₆ is about 2.1 Å. Therefore the hydrated Mg²⁺ may undergo partially dehydration at the interface before the intercalation. This interface process is strongly affected by the choice of solvent. Therefore replacing water with nonaqueous electrolytes may have great impact on the rate performance of Prussian blue electrodes.