Open Access Article
This Open Access Article is licensed under a Creative Commons Attribution-Non Commercial 3.0 Unported Licence

Positioning versatile inorganic cathode materials in the aqueous zinc-ion battery landscape

Kang Guo a, Yaokang Lv d, Ziyang Song *ab, Lihua Gan *ac and Mingxian Liu *ac
aShanghai Key Lab of Chemical Assessment and Sustainability, School of Chemical Science and Engineering, Tongji University, 1239 Siping Rd., Shanghai, 200092, P. R. China. E-mail: ganlh@tongji.edu.cn; liumx@tongji.edu.cn
bState Key Laboratory of Pollution Control and Resource Reuse, College of Environmental Science and Engineering, Advanced Research Institute, Tongji University, 1239 Siping Rd., Shanghai, 200092, P. R. China. E-mail: songziyang@tongji.edu.cn
cState Key Laboratory of Cardiovascular Diseases and Medical Innovation Center, Shanghai East Hospital, School of Medicine, Tongji University, 150 Jimo Rd., Shanghai, 200120, P. R. China
dCollege of Chemical Engineering, Zhejiang University of Technology, 18 Chaowang Rd., Hangzhou 310014, P. R. China

Received 5th December 2025 , Accepted 31st January 2026

First published on 2nd February 2026


Abstract

Rechargeable aqueous zinc-ion batteries (AZIBs) have attracted great attention due to their inherent advantages such as high safety, low cost, and environmental friendliness, making them one of the most promising alternatives to traditional lithium-ion batteries. The rational design and continuous optimization of versatile inorganic cathode materials play a crucial role in achieving practical applications. In this review, we first systematically classify inorganic cathode materials and their design strategies, including manganese oxides with rich redox chemistry, vanadium compounds with multiple oxidation states, Prussian blue analogues with open skeleton channels, layered transition metal disulfides with unique interlayer ion storage capabilities, and halogens with reversible multielectron capacity. Furthermore, the structural characteristics, electrochemical performances, and crucial improvement methods of these cathode materials are discussed in detail. Finally, we outline the challenges and the prospects of inorganic cathodes in AZIBs to guide the future development of next-generation energy communities.


image file: d5sc09531j-p1.tif

Kang Guo

Kang Guo is currently a PhD student at School of Chemical Science and Engineering in Tongji University under the supervision of Professor Mingxian Liu. He received his master's degree (2022) from Shanghai Electric Power University. His research interests focus on the structural design and functional modulation of inorganic materials in aqueous batteries.

image file: d5sc09531j-p2.tif

Ziyang Song

Ziyang Song received his PhD degree from School of Chemical Science and Engineering in Tongji University (2021). He started his postdoctoral researches at Tongji University (2021–2025). After that, he joined College of Environmental Science and Engineering in Tongji University, and became a specially appointed researcher in 2025. His research interest focuses on the structural design of redox-active aromatic organic materials and self-assembled nanostructured carbon materials towards electrochemical energy storage applications involving versatile aqueous batteries and capacitors.

image file: d5sc09531j-p3.tif

Lihua Gan

Lihua Gan received his PhD degree in materials physics and chemistry in Tongji University, and became a professor in Department of Chemistry, Tongji University (2005). His research interests include the design and application of nanomaterials, which cover porous metal oxides, various carbonaceous materials and carbon-based materials. These nanomaterials are used for adsorbents, supercapacitors, and batteries.

image file: d5sc09531j-p4.tif

Mingxian Liu

Mingxian Liu received his PhD degree in physical chemistry in Tongji University (2009). He started his postdoctoral researches in East China University of Science and Technology (2009–2011). After that, he joined School of Chemical Science and Engineering in Tongji University, and became a professor in 2016. His current research interests focus on the structural design of electrode materials for electrochemical storage including carbon-based supercapacitors, zinc-ion hybrid supercapacitors, and zinc-ion batteries.


1. Introduction

With the rapid progress of modern technologies, the extensive use of portable electronics and electric vehicles has intensified the demand for efficient storage systems capable of accommodating fluctuating and intermittent renewable energy, highlighting the necessity for high energy density devices.1–6 Lithium-ion batteries have established themselves as the cornerstone of modern rechargeable energy storage, owing to their high energy density and exceptional cycle stability.7,8 Yet, concerns over safety stemming from flammable organic electrolytes alongside environmental impact, volatile pricing, and constrained supply of critical metals such as lithium and cobalt, have cast growing doubt on their long-term viability.9–11 These limitations have spurred increasing interest in alternative chemistries based on earth-abundant elements such as sodium and potassium.12–17 While resource accessibility is a clear advantage, the large ionic radii and high reactivity of these species impose significant challenges in identifying stable and efficient electrode materials. Aqueous electrolyte systems, by contrast, offer a compelling path forward, combining high ionic conductivity, intrinsic safety, and low cost positioning them as promising candidates for next-generation sustainable energy storage.18–27

Among aqueous-based energy storage systems, aqueous zinc-ion batteries (AZIBs) have garnered significant interest due to several inherent advantages:28–33 (1) a low redox potential of Zn/Zn2+, suitable for both neutral and mildly acidic media (−0.76 V vs. standard hydrogen electrode, SHE), and even lower in alkaline environments; (2) high theoretical specific capacity and exceptional volumetric capacity; (3) aqueous electrolytes have higher ionic conductivity; (4) they are non-flammable, environmentally benign, and compatible with ambient-air assembly benefiting from the richness and stability of metallic zinc. These merits make AZIBs promising for safe, low-cost applications. However, their energy density remains suboptimal compared to organic electrolyte-based systems.34–36 Challenges such as the narrow electrochemical stability window of water, limited discharge capacity, parasitic side reactions, and relatively low output voltage significantly constrain their practical performance.37–39 In response, intensive research efforts have been directed toward enhancing the capacity and energy density of aqueous AZIBs through materials innovation and system-level design.

The practical implementation of AZIBs is hindered by the scarcity of inorganic cathode materials capable of meeting multiple critical requirements simultaneously.40–42 To date, different inorganic cathode materials have been explored in AZIBs, which show versatile advantages of broad structure–function tunability (i.e., heteroatom doping, lattice defects, interlayer extension, interface heterojunction engineering), different charge storage mechanisms of Zn2+/H+ insertion/extraction and halogen multivalent conversion; (iii) board-range performance optimization (capacity, rate capability, energy density, and life) in aqueous conditions. These requirements encompass sufficient structural adaptability to accommodate the strong electrostatic interactions of divalent Zn2+ ions, high specific capacity, appropriate and stable operating voltage, robust cycling stability, as well as environmental friendliness and economic feasibility. The electrochemical and economic advantages of aqueous zinc ion batteries largely depend on the inherent properties of the inorganic cathode materials used.43 Specifically, the rate performance is strongly governed by the ion and electron transport kinetics, together with the interfacial reaction behavior between the electrode and the electrolyte, while the cycle life is largely dependent on the structural integrity and stability of the electrode framework during repeated (dis)charge processes.44–46 Thus, the rational engineering and optimization of versatile inorganic cathode materials that simultaneously deliver high capacity, structural robustness, and sustainability represent a key strategy to overcome current limitations and to accelerate the practical application and industrialization of AZIBs technology.

As shown in Fig. 1, the historical development of AZIBs cathode materials have undergone continuous evolution, reflecting extensive efforts to improve their electrochemical performance and structural stability. So far, various strategies for designing high-performance versatile cathodes have been explored, including manganese (Mn)-based compounds with rich redox activity, vanadium(V)-based materials with multiple oxidation states, Prussian blue analogues (PBAs) with open framework channels, layered transition metal sulfides with unique interlayer ion storage capabilities, and multi electron reversible, high-capacity halogen cathode materials. These systems not only showcase the diversity of material chemistry, but also highlight the challenges of achieving high capacity, long-term cycling stability, and fast ion transport simultaneously. Thus, this review emphasizes the latest advances of different inorganic cathode materials in controlled synthesis, potential electrochemical mechanisms, and rational design strategies (Fig. 2). By consolidating these advances, we aim to provide comprehensive analysis and direction for the rational design of next-generation inorganic cathode materials, ultimately accelerating the practical application of high-performance AZIBs in large-scale energy storage systems.


image file: d5sc09531j-f1.tif
Fig. 1 Timeline of the historical development of inorganic cathode materials for AZIBs.

image file: d5sc09531j-f2.tif
Fig. 2 Schematic diagram of different inorganic cathode materials and design strategies.

2 Mn-based cathodes

Manganese-based compounds are recognized as prospective versatile inorganic cathode candidates for AZIBs owing to the abundant redox chemistry and resource availability.47–50 Manganese is widely distributed in the Earth's crust, predominantly in the form of oxide ores, providing a solid material basis for large-scale deployment in energy storage. These compounds can undergo multiple valence transitions (e.g., Mn4+/Mn3+ and Mn4+/Mn2+), often accompanied by single- or two-electron transfer processes, which endow them with high capacity and considerable energy output. Moreover, manganese oxides typically feature high operating voltages and favorable theoretical capacities, further underscoring their potential as attractive inorganic cathode systems. To this end, various crystalline frameworks have been explored, ranging from different polymorphs of MnO2 to spinel-type ZnMn2O4.51–54

Despite these advantages, several challenges hinder their practical implementation. Although its ionic radius is comparable to lithium, Zn2+ exhibits strong coulomb interactions with the electrode skeleton, which severely limits diffusion and slows down the intercalation process. In the absence of rational structural engineering, it is difficult to realize efficient and reversible Zn2+ storage. In addition, the inherently low electrical conductivity and sluggish ion transport of manganese oxides further restrict their rate capability. Compounding these issues, long-term cycling often triggers structural distortions, Mn dissolution, and active component depletion, ultimately result in severe capacity fading and limited battery lifespan.55–57

2.1 MnO2 materials

The porous skeleton (tunnel/layered configuration) of MnO2 can stably support reversible insertion/deintercalation of Zn2+, making it the preferred Mn-based versatile inorganic cathode material for AZIBs.58–62 However, the delayed ion migration kinetics, insufficient intrinsic conductivity, and manganese leaching effect still constrain its performance improvement.63–65 In recent years, researchers have been continuously advancing the practical application of MnO2 lattice and interface composition in AZIBs to enhance cycling stability.66–68

Research has shown that doping with non-metallic heteroatoms can effectively regulate the electronic structure and surface chemistry of MnO2, improve conductivity and ion diffusion channels, thereby enhancing its specific capacity and cycling stability. Liu team enhanced the cycling stability of MnO2 by doping nitrogen and sulfur into MnO2 (NS-MnO2) through a simple annealing strategy (Fig. 3a).69 Research shows that N/S co-doping establishes Mn–N and Mn–S bonds within the lattice. The Mn–N configuration suppresses Jahn–Teller distortion in Mn3+ species, while Mn–S bonding reduces Zn2+-cathode electrostatic interactions, enabling reversible Mn4+/Mn3+ redox without by-product formation (Fig. 3b). This co-doping strategy simultaneously elevates intrinsic conductivity, significantly accelerating reaction kinetics. Benefitting from these synergistic effects, the NS-MnO2 cathode delivers exceptional electrochemical performance, outstanding cycling durability (295 mAh g−1 at 0.2 A g−1) and maintains structural stability (1500 cycles at 1 A g−1, Fig. 3c).


image file: d5sc09531j-f3.tif
Fig. 3 Multiscale structural engineering of MnO2. (a) Synthesis process, (b) charge density difference distribution, and (c) cycling performance of the NS-MnO2 material.69 Copyright 2025, Wiley-VCH. (d) Schematic birnessite structures and Density functional theory (DFT) calculated structures of pristine δ-MnO2 (K-birnessite MnO2) and Ce doped δ-MnO2 (Ceinter-MnO2, Cein/inter-MnO2, Ceexcess-MnO2).70 Copyright 2023, Wiley-VCH. (e) Synthesis schematic of HE-MnO/C.72 Copyright 2024, Elsevier. (f) Schematic illustration of the NAPD pre-intercalation process.73 Copyright 2024, Elsevier. (g) Schematic illustration of the cascaded orbital-oriented hybridization mechanism.74 Copyright 2022, Wiley-VCH (h) adsorbing energy and charge difference density simulations of Mn2+ on the surface of the 3DP CMs, carbon cloth, and Ti mesh.75 Copyright 2022, Wiley-VCH.

Compared with non-metallic heteroatom doping, metal ion doping can significantly improve the zinc storage capacity and cycle life of MnO2 by adjusting the lattice structure and valence state distribution, expanding the interlayer spacing, enhancing structural stability, and introducing more reversible redox sites. Xu group developed Ce-doped δ-MnO2 as a high-performance AZIBs inorganic cathode and investigated the effects of different doping positions (Fig. 3d).70 At low Ce content, cations occupy interlayer sites (Ceinter-MnO2), while higher doping introduces Ce into both interlayer and lattice positions (Cein/inter-MnO2), forming alternating layered structures. Excessive doping may trigger phase transitions (Ceexcess-MnO2). Cein/inter-MnO2 notably enlarges the interlayer spacing, providing more zinc storage sites and faster ion diffusion. Ce doping also generates oxygen vacancies and loosens the flower-like structure, enhancing conductivity and increasing electrochemical active sites. As a result, Cein/inter-MnO2 delivers a maximum capacity of 393.0 mAh g−1 at 300 mA g−1 and maintains 148.9 mAh g−1 after 2000 cycles at 3 A g−1 with nearly 100% retention.

Zhao et al.71 mitigated the conflict between electrochemical kinetics and durability in AZIBs by developing Al-doped, defect-rich MnO2 nanosheets (Alx–MnO2) via electrochemical oxidation of MnAl-LDHs. Al3+ vacancies served as 3D Zn2+ diffusion channels, while residual Al suppressed lattice distortion, preserving structural integrity. The modified Al0.1–MnO2 showed high capacity, fast kinetics, and longer cycle life, exceeding most of the current Mn- and V-based versatile inorganic cathodes. Compared to a single metal, the doping effect of multiple high entropy materials is more pronounced. Wang et al.72 introduced multiple metal dopants into a single oxide matrix and formed high entropy HE-MnO/C composites through in situ confinement, achieving a robust cathode for AZIBs (Fig. 3e). The dopants selected for ionic radius compatibility and electrochemical function, enhanced voltage (Cr, Cu), structural stability (Co, Zn), and redox activity (Ni). Compared to single doping, entropy-driven stabilization suppressed Mn dissolution, as supported by theoretical insights showing stronger Mn–O bonding. Defect-induced kinetics further improved durability (after 10[thin space (1/6-em)]000 cycles at 10 A g−1, the capacity retention rate was 93.2%). This study highlights the promise of high-entropy materials for advanced AZIBs versatile inorganic cathodes.

In addition to inserting metal ions into the interlayer, the insertion of organic materials is also very effective in enhancing the framework stability, charge storage capability, and conductivity of Mn-based oxides. Huang et al.73 designed a hybrid cathode by pre-intercalating 1,5-diaminonaphthalene (NAPD) into potassium manganese oxide (KMO), yielding KMO-NAPD with enhanced electrochemical performance (Fig. 3f). The incorporation of NAPD modulated the d-electron spin states of Mn, boosting Zn2+ intercalation activity and reducing Zn2+–host interaction through weakened electrostatic forces, thereby facilitating ion diffusion. So that, the assembled AZIBs also exhibited an impressive energy density of 294.3 Wh kg−1 alongside a maximum power output of 8.6 kW kg−1. Yang et al.74 proposed a cascaded orbital-oriented hybridization strategy by introducing 1,3-propanediamine (DP) to construct an organic–inorganic hybrid framework. The Px and Pz orbitals of the nitrogen atoms in DP engage in antibonding σ-hybridization with Mn dx2y2 orbitals near the Fermi level, thereby elevating the energy of Mn dx2y2 state and enabling its further hybridization with O Py orbitals in the MnO2 lattice (Fig. 3g). This orbital reconstruction selectively accelerates proton-storage kinetics while exerting a negligible effect on the Zn2+ insertion pathway. Consequently, the resulting DP-MnO2 composite exhibits outstanding rate capability and long-term cycling stability.

Repeated ion insertion/extraction of MnO2 can easily lead to crystal structure collapse and pulverization, causing contact failure between the active substance and the current collector, resulting in rapid capacity decay. Introducing carbon materials to form composite structures has become an effective strategy to overcome these bottlenecks. Yang et al.75 abdicated 3D-printed carbon microlattices (3DP CMs) using graphene and carbon nanotubes via direct ink printing followed by high-temperature annealing (Fig. 3h). The printing enabled periodic architectures, while annealing enhanced conductivity and introduced surface defects. These features promoted uniform electric field distribution and enhance the controlled growth of MnO2. Notably, 3DP CM electrode incorporating MnO2 delivered an unprecedented specific capacity of 282.8 mAh g−1 (mass loading: 28.4 mg cm−2) and, offering an effective route toward designing advanced AZIBs electrodes. Fan et al.76 designed CNT-MnO2 (C-MnO2) nanorods using carbonylated CNTs as a “defense shield” to promote proton insertion and ensure stable, fast-charging Zn–Mn batteries. The CNT network shortened ion diffusion paths and offered abundant proton sites, enhancing charge transport and structural reversibility. Meanwhile, carboxyl groups and Mn–O–C bonds suppressed Mn2+ dissolution and improved redox stability. Therefore, C-MnO2 cathode has achieved high capacity and excellent cycling performance. In order to ensure sustainable material sources, low costs, and environmental friendliness, Lv et al.77 successfully prepared γ-MnO2 uniformly loaded on nitrogen doped carbon in grapefruit peel using biomass materials (γ-MnO2@CP). After 3000 cycles under the condition of 5 A g−1, the capacity retention rate reached as high as 92.17%.

MnO2-based cathodes face critical limitations, including poor electronic conductivity, structural collapse during cycling, active material dissolution, and sluggish Zn2+ diffusion. Recent advances have introduced several targeted strategies to mitigate these issues.78,79 First, elemental doping and defect modulation effectively reshape the electronic environment and surface reactivity, thereby enhancing charge transport, stabilizing redox reactions, and preventing irreversible phase changes. Second, interlayer engineering via the pre-intercalation of guest species into layered MnO2 helps maintain interplanar spacing, promoting ion diffusion and structural reversibility. Third, compositing with carbon-based frameworks improves conductivity and mechanical resilience, while also increasing surface area and exposing more active sites. These multifaceted strategies pave the way for next-generation, high-efficiency MnO2 versatile inorganic cathodes in AZIBs systems.

2.2 Other Mn-based materials

In addition to MnO2, other Mn-based oxides such as Mn3O4, MnO, and spinel-type compounds (e.g., MxMn2O4, where M = Zn, Mg, etc.) have also been explored as versatile inorganic cathode materials for AZIBs.80–82 These materials exhibit distinct energy storage mechanisms: Mn3O4 and Mn2O3 typically undergo multivalent redox reactions involving Mn3+/Mn2+ or Mn4+/Mn3+ transitions during Zn2+ intercalation or phase transformation. MnO, with a simpler cubic structure and lower valence state, stores charge primarily through reversible redox conversion reactions. Spinel-type MxMn2O4 compounds, where Zn2+ or other metal ions are pre-intercalated into the lattice, enable structural stabilization during Zn2+ reinsertion and reversible Mn redox processes. Despite their structural diversity, these Mn-based oxides often suffer from rapid capacity fading, manganese dissolution, poor intrinsic electronic conductivity, and sluggish Zn2+ diffusion, all of which limit their long-term cycling stability and rate capability.

Manganese dissolution is one of the key issues leading to a decrease in the cycling stability of Mn-based oxide cathode materials, such as Mn3O4. The limited redox kinetics and sustained manganese dissolution jointly lead to low activity, rapid capacity decay, and shortened cycle life of Mn3O4 electrode. For this, Deng et al.83 proposed a novel strategy combining vanadium vacancy engineering with Mn-ion confinement, yielding a composite cathode denoted as VMn-Mn3O4@C (Fig. 4a–c). The introduction of cationic V vacancies created additional active site significantly enhancing capacity. Simultaneously, the carbon matrix restricted Mn ion migration, effectively suppressing dissolution and improving structural durability. Thus, Zn/VMn-Mn3O4@C cell achieved a performance of 280.9 mAh g−1 at a low current of 0.1 A g−1 and ion diffusion coefficient. More notably, the capacity remained nearly unchanged after 5000 cycles at 1 A g−1, offering a promising pathway for designing high-performance Mn-based cathodes in AZIBs.


image file: d5sc09531j-f4.tif
Fig. 4 Phase change engineering in Mn-based cathodes. (a) XRD pattern, (b) TEM image, and (c) long-term cycling performance of VMn-Mn3O4@C.83 Copyright 2024, Wiley-VCH. (d) XRD pattern, (e) cycling performance, and (f) XRD patterns before and after cycling of α-Mn2O3. (g) Schematic diagram of the electrochemical reaction process of the Zn0.17MnO2·0.52H2O cathode.84 Copyright 2024, Wiley-VCH. (h) Schematic illustration of phase transition mechanism.85 Copyright 2023, Elsevier. (i) Theoretical calculations of proton intercalation in Zn0.5Mn2O4.86 Copyright 2022, Wiley-VCH.

Tailoring reversible and robust crystal structures in Mn-based materials remains a critical yet challenging task. To this end, Liu group developed a controllable electrochemical oxidation-induced phase transformation strategy, enabling the conversion of cubic α-Mn2O3 into an amorphous Zn0.17MnO2−n·0.52H2O (Fig. 4d–f).84 This amorphous phase, serving as the active Zn2+ host, offers abundant and accessible Zn-affinitive sites while alleviating lattice strain during Zn2+ (de)intercalation (Fig. 4g). Structural evolution analyses and theoretical simulations confirm that this amorphous phase exhibits excellent electronic conductivity and low Zn2+ migration barriers, and can reversibly transform into crystalline ZnMn3O7·3H2O during cycling. The stabilized dynamic transformation equilibrium underpins a remarkable specific capacity of 558 mAh g−1, a high energy density of 696 Wh kg−1 at 6 kW kg−1, and exceptional long-term cycling stability over 5000 cycles. Moreover, this strategy is extendable to other Mn-based systems such as Mn3O4 and α-MnO2, offering new insights into electrochemical oxidation-driven crystal engineering for highly reversible and durable AZIBs.

MnO suffers from limited redox activity due to its stable Mn2+ state and lacks Mn3+/Mn4+ conversion. Its poor conductivity and sluggish Zn2+ diffusion further restrict rate capability. To overcome these drawbacks, Li et al.85 synthesized a composite cathode materia by embedding ultrafine VN quantum dots and MnO nanoparticles in a nitrogen-doped carbon matrix (NC@VN/MnO) via in situ self-polymerization (Fig. 4h). The VN-MnO heterostructure induces interfacial polarization and a built-in electric field, enhancing ion/electron transport and structural stability. So that, the cathode delivers 108.3 mAh g−1 after 12[thin space (1/6-em)]000 cycles at 10 A g−1, showing outstanding durability and electrochemical performance.

In AZIBs, protons actively contribute throughout the entire energy storage process. Nevertheless, the proton transport mechanism in metal oxide cathodes remains highly debated, largely due to the lack of suitable model systems, particularly with respect to how cation distribution modulates proton-conducting pathways. Using spinel-type ZnMn2O4 as a prototype, Pan and co-workers demonstrated that reducing the Zn content in the lattice by half nearly doubled the high-rate capacity, primarily owing to enhanced proton storage (Fig. 4i).86 Detailed analysis revealed that in Zn-deficient structures, protons migrate efficiently through cooperative transport, whereas in stoichiometric counterparts, proton insertion follows a much slower and sequential process. Moreover, the intrinsically restricted Zn mobility within the spinel framework confers strong structural stability, preventing external Zn2+ from occupying Zn vacancies during cycling and thereby preserving proton storage advantages. These findings highlight that tailoring non-stoichiometric features represents a promising strategy to optimize proton conduction and storage performance in aqueous batteries.

The modification for MnO2 targets their main issues of poor electronic transport, slow ion diffusion, and structural instability during interfacial electrochemical reactions in AZIBs: (i) regarding the poor electronic transport of MnO2 cathodes (e.g., high polarization, charge-transfer resistance and severe rate decay), mixing MnO2 with highly conductive skeletons (carbon and polymers) is efficient to build continuous conductive networks for enhancing electron percolation and accelerating reaction kinetics towards efficient charge storage; (ii) to alleviate the problem of slow ion diffusion within MnO2 host (e.g., low GITT diffusion coefficient and low capacity contribution), it is beneficial to design Mn/O vacancies, expand Mn–O interlayers, or construct p–n heterojunctions (e.g., MnO2/MoS2 hybrid), which provide desirable platforms to optimize Zn2+ diffusion channels and surface wettability with low energy barriers; (iii) to avoid the structural change and dissolution (e.g., Mn dissolution, collapse, irreversible phase evolution), lattice-stabilized metal-ion doping is preferred to strengthen Mn–O bonding and suppress Jahn–Teller distortions/phase transitions. It should be pointed out that each strategy has boundary conditions and usage standards, and the most suitable regulatory strategy should be selected based on the target indicators.

In summary, Mn-based oxides, particularly MnO2, have shown great potential as versatile inorganic cathodes for AZIBs owing to their open frameworks and rich redox chemistry, but their practical performance is still restricted by poor intrinsic conductivity, sluggish Zn2+ diffusion, structural collapse, and Mn dissolution.87 Recent studies have demonstrated that elemental doping/defect modulation, interlayer engineering (via guest species pre-intercalation), and compositing with conductive carbon frameworks can effectively reshape the electronic environment, stabilize the host structure, and accelerate ion/electron transport, thereby improving capacity, rate capability, and cycling stability. Other Mn-based oxides such as Mn3O4, Mn2O3, MnO, and spinel-type MxMn2O4 also benefit from defect, phase, and interface engineering to construct more reversible and robust Zn2+/H+ storage hosts.

Despite this progress, significant challenges remain, including capacity degradation under practical mass loading, competitive Zn2+/H+ reactions, and insufficient understanding of dissolution and phase evolution. Future research should therefore focus on: (i) designing precisely doped and defect-regulated Mn-based lattices, including high-entropy and non-stoichiometric systems, to simultaneously optimize electronic structure, ion transport, and Mn stability; (ii) constructing interlayer-engineered and organic–inorganic hybrid frameworks that decouple and co-optimize Zn2+ and proton storage while maintaining structural integrity under long-term operation; (iii) developing multidimensional conductive architectures and biomass-derived carbon scaffolds to realize thick, flexible, and mechanically robust Mn-based cathodes with high areal capacity; and (iv) integrating advanced in situ/operando characterizations with multiscale simulations to elucidate redox mechanisms and transport pathways, thereby guiding rational material design. Additionally, by embedding Mn-based oxides into printable, self-supporting carbon frameworks, binder-free and potentially biocompatible electrodes can be constructed, which may be extended to flexible and implantable AZIBs, further broadening the application landscape of Mn-based versatile inorganic cathodes.

3 V-based cathodes

Vanadium based compounds have become another versatile inorganic cathode material for AZIBs due to their multivalent properties (from V2+ to V5+), adjustable crystal structure (including layering, tunneling, 3D framework, etc.), high theoretical capacity, fast reaction kinetics, and excellent cycle life at high current densities.88 Due to its uniqueness, AZIBs has aroused great interest among people. To date, a wide array of vanadium-containing materials has been explored as cathodes, including vanadium oxides (layered or tunneled structures), vanadium nitrides, chalcogenides, V–C composites, and NASICON-type phases such as Na3V2(PO4)3.

3.1 V2O5-based materials

Layered V2O5 stands out as one of the most widely studied and structurally stable V-based oxides.89–91 It offers a high theoretical capacity of 589 mAh g−1 and a favorable interlayer spacing of ∼4.7 Å, which facilitates the diffusion of charge carriers.92 Nevertheless, its practical application in aqueous electrolytes is limited by several factors, including a comparatively reduced working voltage (∼0.8 V vs. Zn), sluggish ionic conductivity, and the tendency of vanadium to dissolve into the electrolyte.93,94 To address such issues, various strategies have been introduced to enhance structural stability, redox kinetics, and electrochemical performance of materials.95–97 Considering the rapid progress in this field, a timely and comprehensive review of recent advances in V2O5-based AZIBs is essential for providing insights into their underlying mechanisms and guiding future research directions.

Introducing cations (M+) into the interlayer can increase the interlayer spacing, enhance structural stability, and promote the migration of Zn2+. Notably, the type of inserted cation plays a critical role in modulating material properties. To this end, Hu et al.89 developed a universal supramolecular self-assembly strategy to fabricate ultrathin MxV2O5 nanosheets incorporating a wide range of single and multiple cations (Fig. 5a). Single-cation intercalation significantly enhanced Zn2+ diffusion kinetics and specific capacity, while multi-cation systems improved structural stability and cyclic reversibility via cooperative pillar effects. The optimized configuration exhibited a remarkable Zn2+ diffusion coefficient of 7.5 × 10−8 cm2 s−1, outperforming the majority of previously reported vanadium-derived cathode materials (Fig. 5b and c). This work presents a versatile multi-cation confinement strategy for advancing AZIBs inorganic cathodes and offers new insights into supramolecular guest-ion regulation of ion transport. To address the challenges associated with vanadium oxides, such as limited interlayer spacing, poor reversibility, and high solubility. Liu's group proposed an inorganic–organic co-intercalation strategy and successfully developed a layered cathode material, [Al0.16(C5H14ON)0.12]V2O5·0.39H2O (IO-V2O5).98 This hybrid system expands the interlayer distance to 13.7 Å and reinforces structural integrity, enabling enhanced performance in AZIBs (Fig. 5d). In this structure, Al3+ and betaine act as dual interlayer pillars, establishing rapid 2D Zn2+ transport channels. The quaternary ammonium group in betaine strongly interacts with the lattice oxygen of V2O5, further stabilizing the layered framework, while the carboxyl group weakens Zn2+/V–O interactions, enhancing Zn2+ transport dynamics and lowering the energy barrier. Therefore, IO-V2O5 cathode achieves an impressive capacity (549.5 mAh g−1 at 0.2 A g−1), fast ion diffusion coefficients (10−8–10−7 cm2 s−1), excellent cycling stability (80.1% retention after 20[thin space (1/6-em)]000 cycles at 30 A g−1), and a remarkable energy density of 416.3 Wh kg−1. This research by Liu group offers a promising pathway for developing high-capacity inorganic–organic co-intercalated V-based cathodes for next-generation AZIBs.


image file: d5sc09531j-f5.tif
Fig. 5 Multi angle optimization strategy for V2O5 cathode. (a) Schematic supramolecular self-assembly strategy, and (b and c) analysis of ion diffusion coefficients for MxV2O5.89 Copyright 2023, Wiley-VCH. (d) Schematic mechanisms and structural advantages of IO-V2O5 cathode in AZIBs.98 Copyright 2025, Wiley-VCH. (e) PTS conduction mechanism, (f) DFT calculations, and (g and h) electrochemical performance of PEDOT-SO3-ZnVO.99 Copyright 2024, Wiley-VCH. (i) Energy storage mechanism. (j) Schematic energy bands and its discharged state. (k) Charge density distribution.100 Copyright 2024, Wiley-VCH.

Conventional electrodes, concentration polarization induced by unbalanced charge transport and solid-state diffusion resistance significantly hinders reaction kinetics, limiting the practical application of AZIBs. To address this, Zhu et al.99 proposed an integrated hybrid electronic–ionic conductor featuring spatially coupled charge transport pathways, enabling efficient redistribution and rapid of Zn2+ and electrons (Fig. 5e and f). Through vanadium oxide confinement, dual-conductive networks were self-assembled at the nanoscale, offering enhanced charge storage capability and accelerated ion diffusion within the bulk. This architecture not only increased the density of active sites and improved reaction kinetics but also mitigated proton-induced dissolution of the active material by enabling reversible ion transport during self-doping/dedoping processes. As a result, the tailored cathode (PEDOT-SO3-ZnVO) demonstrated outstanding rate performance, delivering 310 and 148 mAh g−1 at 0.2 and 10 A g−1, respectively, under a mass loading of 10 mg cm−2 (Fig. 5g and h). This work highlights a promising strategy for precisely tuning the electrochemical behavior of functional nanomaterials in high-performance AZIBs.

Constructing multiphase heterojunctions with tailored surface and interface properties offers a promising approach to address sluggish kinetics and limited redox activity. Yang et al.100 developed a thermal oxidation strategy to fabricate a triphasic heterostructure composed of a VSSe core with VO2 and V2O5-rich interfaces (Fig. 5i–k). The enlarged surface area and optimized interfacial coordination enhance electrode/electrolyte interactions and promote synergistic multi-anion (S/Se/O) and cation (V) redox reactions. Strengthened p–d orbital hybridization and spin polarization at the heterointerface accelerate charge transfer and improve structural robustness. This integrated architecture overcomes the limitations of single-phase materials, enabling stable cycling and reliable operation even under harsh conditions. This study presents a viable design strategy for versatile inorganic cathodes based on interfacial engineering of heterostructures.

3.2 Other V-based materials

Among the range of V-based cathode materials, V3O7·H2O has a mixed valence state (V5+/V4+), which has attracted considerable attention due to its layered structure and interlayer water. Compared with V2O5, it faces severe irreversible structural collapse and dissolution intercalation under repeated Zn2+ action, and further optimization is needed to achieve high-rate capability and long-term cycling durability. For example, Huang group proposed an effective strategy to address the rapid capacity fading of V3O7·H2O cathodes, which is typically caused by active material dissolution during cycling (Fig. 6a).101 By doping high-valence Sn4+ into V3O7·H2O (referred to as Sn-V3O7·H2O), they successfully enhanced the structural stability of AZIBs. The incorporation of Sn4+ thermodynamically reduced the formation energy of the host material and increased the dissolution energy of VO2+ ions, effectively mitigating vanadium loss (Fig. 6b and c). Moreover, Sn4+ doping improved electronic conductivity and broadened Zn2+ diffusion channels, thereby accelerating Zn2+ intercalation/deintercalation kinetics and boosting the overall electrochemical performance (Fig. 6d). In addition, composite with conductive materials is also an effective method to improve V3O7 cathode. Liu et al.102 anchored a conductive metal–organic framework composed of Cu and hexahydroxy benzene ligands (Cu-HHTP) onto V3O7·H2O nanobelts via π–d conjugation. This anchored Cu-HHTP markedly enhanced the electrical conductivity of the V3O7·H2O nanobelts, enabling faster reaction kinetics and providing abundant active sites for efficient Zn2+ storage.
image file: d5sc09531j-f6.tif
Fig. 6 V-based cathode modification strategies. (a) Solubility test, (b) post immersion image, (c) dissolution energy, and (d) cathodic stability schematic diagram of V3O7·H2O and Sn-V3O7·H2O.101 Copyright 2024, Wiley-VCH. (e) Schematic diagram of the influence of electrode arrangement related to material morphology on tunnel orientation and ion diffusion behavior.32 Copyright 2024, Wiley-VCH. (f) Schematic illustration of the synthesis process. (g) Rate performance of HNVO-Glu. (h) Cycling stability.104 Copyright 2024, Wiley-VCH. (i) NVPF@C and HE-NVPF@C crystal structure.105 Copyright 2024, Elsevier.

VO2 is regarded as a prospective versatile inorganic cathode material for AZIBs owing to its unique tunnel or layered structures and the multivalent redox states of vanadium. However, unlike layered oxides with adjustable interlayer spacing, improving ion transport within tunnels of fixed dimensions remains challenging. Zhao and co-workers revealed that electrode architecture significantly influences tunnel orientation and thus ion diffusion kinetics (Fig. 6e).32 Their study demonstrated that VO2(B) nanoribbons with dispersed (001) facets preferentially align along the c-axis, enabling directional and rapid Zn2+ diffusion, which translates into superior rate performance and prolonged cycling durability. In contrast, aggregated VO2(B) samples with random orientations exhibit isotropic and sluggish ion transport, resulting in poor electrochemical performance. These results highlight that regulating exposed crystal planes in combination with morphology-controlled electrode assembly provides a viable approach to optimize Zn2+ diffusion behavior in tunnel-type V-based cathodes.

Vanadate salts have attracted wide interest in AZIBs, as interlayer cations can expand spacing, suppress structural deformation, and enhance cycling stability. Their variable oxidation states further stabilize the framework and provide abundant Zn2+ storage sites, making sodium vanadate a highly promising anode candidate. Among various strategies, synthesis strategy mediated by guest materials has unique advantages. Hu et al.103 developed Na2V6O16·1.63H2O (H-NVO) nanowires exhibiting an electrical conductivity of 67 S m−1. In the initial discharge phase, Zn2+ ions were incorporated into the host framework facilitated by water molecules, enabling reversible migration between the cathode and anode during subsequent cycles. The electrode demonstrated exceptional long-term stability, maintaining 90% of its initial capacity after 6000 cycles at a high current density of 5000 mA g−1, with a retained capacity of 158 mAh g−1. Although pre-inserted cations contribute to structural stabilization and enhanced ion transport kinetics, significant interlayer electrostatic interactions persist. To mitigate the strong electronegative environment imposed by oxygen atoms, the introduction of polar functional molecules can effectively modulate the local charge distribution. Zhang et al.104 eveloped a guest-mediated strategy for synthesizing NVO, in which glutamic acid (Glu) was utilized to induce proton substitution of sodium, thereby achieving a crystalline transformation (Fig. 6f). This approach not only prevents structural phase transitions and collapse but also, via the polar groups on Glu, weakens the interaction between ions and the host material, thus enhancing the zinc-ion transport rate. The HNVO-Glu electrode therefore exhibited excellent cycle life of 12[thin space (1/6-em)]000 cycles at a capacity retention of 87.2%.

The NASICON-type polyanionic compound with the general formula M3V2(PO4)3(M = Li, Na) possesses a stable 3D structure framework and represents a significant class of V-based materials for Zn2+ storage. Owing to their wide ion-conduction pathways and favorable ion transport kinetics, NASICON-structured compounds have emerged as promising versatile inorganic cathode candidates for AZIBs. Despite their potential, implementation is challenged by issues such as limited cycling stability, low intrinsic electronic conductivity, and sluggish Zn2+ diffusion. Among various modification strategies, cation doping has proven to be an effective approach to tailor the electrochemical properties and overcome these inherent limitations of NASICON-type cathodes. Liu group developed a high-entropy doped, carbon-coated NASICON-type Na3V2(PO4)2F3 (HE-NVPF@C) cathode, through a rational high-entropy engineering strategy (Fig. 6i).105 This work presents the first comprehensive experimental and theoretical investigation of charge storage mechanism in multi-component NASICON-type systems. The multi-element doping effectively suppresses Jahn–Teller distortion, minimizes structural deformation throughout Zn2+ (de)intercalation, and lowers the Zn2+ migration energy barrier, collectively enhancing cycling stability. Therefore, the cathode exhibits outstanding long-term durability, with an ultra-low-capacity decay rate of just 0.0031% after 6000 cycles at 20C. This high-entropy strategy offers a promising avenue for designing practical AZIBs with prolonged lifespan and high areal performance.

Overall, V-based compounds have become highly attractive multifunctional inorganic cathode materials in aqueous zinc ion batteries due to their diverse crystal structures, multi electron redox chemistry, and high theoretical specific capacity. However, its practical application is still limited by slow ion/electron transport, unstable structure (phase transition, interlayer collapse), and severe dissolution of vanadium in aqueous electrolytes. In recent years, Zn2+ has significantly improved the storage capacity, rate performance, and cycling stability of V-based cathodes through interlayer engineering (pre-insertion/co-insertion of metal cations and organic guests), construction of integrated electron/ion transport networks, and optimization of vanadium surfaces/interfaces. However, there are still several key challenges to be addressed in the future, including: how to effectively suppress the dissolution of VOx without sacrificing the utilization rate of high valence vanadium; how to balance high load and structural integrity under actual high surface capacity conditions; and how to elucidate the coupling contributions of Zn2+, H+, pre-embedded cations, and structural water to the entire energy storage process.

Therefore, future research should focus on: (i) elucidating and actively regulating the synergistic storage pathways and water mediated structural evolution in multi ion (Zn2+/H+/M+ (Li+/Mg2+/Al3+, etc.)) layered/tunneling vanadate salts to achieve valence state transitions while avoiding side reactions; (ii) collaborative design of electrolyte interfaces for vanadium based cathodes, constructing specialized electrolyte systems and interface layers (such as buffering or weakly acidic media, coordination adjustable anions, functional additives, and artificial coatings), while suppressing vanadium dissolution and improving long-term cycling stability; (iii) expand the system beyond oxide systems, including vanadium nitride, sulfur/selenides, V–C complexes, and multi anionic multi-component frameworks, to construct a Zn2+/H+ synergistic energy storage framework with a wider voltage window and intrinsic stability; (iv) develop scalable and low-cost synthesis and densification processes to prepare vanadium based electrodes with high packing density and excellent mechanical stability, enabling them to operate stably under practical conditions such as high load, low electrolyte, and limited excess zinc, while considering safety, environmental friendliness, and recyclability. With the continuous development of these directions, V-based compounds are expected to play an important role in constructing high-energy density, long-life, and feasible AZIBs.

4 PBAs-based cathodes

Prussian blue analogues (PBAs) are promising versatile inorganic cathodes for AZIBs owing to their open framework (∼10 Å), which enables wide Zn2+ diffusion channels and fast, reversible ion transport. Their robust structural integrity ensures long-term cycling stability, while a moderate operating voltage (0.9–1.2 V vs. Zn/Zn2+) balances energy density and safety. Furthermore, the green, economically viable, and scalable aqueous synthesis of PBAs supports broad-scale application, highlighting their potential as next-generation high-performance versatile inorganic cathode materials.106–108

Due to the structural defects inherent in PBAs, their capacity deteriorates over long-term cycling. By doping with metal or non-metal ions, the crystal structure and electronic conductivity can be optimized, effectively improving cycling stability. Luo group developed Cu-substituted Mn-based Prussian Blue analogue (CuMn-PBA DSNBs) double-shelled nanoboxes via a surface modification and ion-exchange strategy, which achieved excellent Zn2+ storage capability (Fig. 7a and b).109 The distinctive hollow double-shell architecture provides abundant electroactive sites and effectively buffers the volume fluctuations during cycling. Furthermore, the partial doping of Cu and the resulting Mn vacancies are beneficial for reducing the Jahn–Teller distortion of the material octahedra, thereby contributing to improved cycling life (Fig. 7c). Yu group synthesized copper (Cu)-doped Mn PBA (CuMn PBA-2) hybrid architectures using water-based co precipitation technology. Adding Cu can partially improve the conductivity of the electrode and promote faster transport of Zn2+ within the electrode framework.110


image file: d5sc09531j-f7.tif
Fig. 7 Modification strategies for PBAs and TMD cathodes. (a) FESEM image, (b) TEM image, and (c) cycling performance of CuMn PBA DSNBs.109 Copyright 2022, Wiley-VCH. (d) Nucleation and crystal growth processes.111 Copyright 2024, Wiley-VCH. (e) Schematic diagram of the synthesis process of V-PBA. (f) Galvanostatic discharge curves and comparison of rate performance.112 Copyright 2024, Wiley-VCH. (g) Schematic illustration of the energy storage mechanism and (h) redox potential of the AgHCF-3 electrode.113 Copyright 2024, Wiley-VCH. (i) Schematic synthesis, (j) rate performance, and (k) cycling stability of MoS2 and MoS2-β-CD.119 Copyright 2021, Elsevier. (l) Schematic synthesis and (m) rate capability of the MoS2/rGQDs.121 Copyright 2023, Wiley-VCH.

The low utilization rate of active sites and abundant structural vacancies have always hindered the potential of PBAs. Zhang et al.111 first used porous MXene as a multifunctional host material to improve the growth and crystallinity of PBAs (Fig. 7d). By targeted modification, CoHCF/MXene composite materials have achieved high surface area and low defects, resulting in impressive specific capacity cycle life. This synthesis strategy provides an effective method for inducing the growth of high surface area, low vacancy PBA-based materials for high-performance AZIBs. Pang team first reported an environmentally friendly and mild in situ generation and conversion strategy for synthesizing uniform V-based PBA nanocubes, using V6O13 nanobelts as the vanadium source.112 This method produced highly crystalline V-PBA nanocubes with ordered channels, enabling additional redox reactions associated with V3+/V4+ and V4+/V5+ couples (Fig. 7e). As a result, the as-prepared V-PBA achieved a superior specific capacity of approximately 200 mAh g−1, outperforming conventional metal-based PBAs (M = Co, Cu, Mn, Ni) synthesized via co-precipitation (Fig. 7f).

To address the challenges of limited Ion transport kinetics and structural water in PBAs, Li group developed a defect-free and anhydrous silver hexacyanoferrate (AgHCF-3), by precisely tuning the K/Ag ratio within the framework (Fig. 7g).113 Through two consecutive oxidation–reduction reactions (Fig. 7h), this material can accommodate nearly four electrons, delivering an electrochemical performance of 179.6 mAh g−1 at 20 mA g−1 while maintaining almost full coulombic efficiency. The reversible formation of Ag0 during cycling contributes to excellent rate capability, maintaining 80.3% battery performance after long cycles. This study lays the foundation for designing PBAs cathodes that can provide high charge storage. Wang team prepared dislocation engineered potassium ferrocyanide (FeHCF) by using PVP additives, which reduced the crystal water content and induced crystal dislocations.114 The low content of crystal water in FeHCF is related to the formation of dislocations. The dislocation effect effectively enhances the electrochemical reactivity and reaction kinetics of FeHCF. When used as a cathode, AZIBs exhibits a high voltage of 2.6 V, fast charging capability (<5 minutes), and satisfactory cycling stability.

In summary, PBAs is an attractive multifunctional inorganic cathode for AZIBs due to their open 3D framework, wide ion diffusion channels, and moderate voltage. Despite recent improvements in doping, defect strategies, and advanced host framework engineering, key challenges still exist, including how to simultaneously control vacancy concentration and crystal water to balance ion transport and structural stability, how to improve intrinsic conductivity without damaging the open framework, and how to suppress framework degradation and possible cyanide bridge dissolution under long-term cycling and high-quality loading. Therefore, future research should focus on: (i) atomic level regulation of defects, vacancies, and hydrochemistry to maximize the utilization of active sites while maintaining lattice integrity; (ii) reasonably design multi metal and multi electron PBA frameworks (such as adding high redox activity transition metals in addition to traditional Fe/Co/Mn) to overcome capacity limitations; (iii) electrolyte and interface synergistic engineering to stabilize PBAs electrolyte in real Zn2+, reduce side reactions and structural decay; and (iv) developing scalable routes to achieve dense, mechanically robust, and even flexible PBAs electrodes that can operate under high area loads, poor electrolyte, and device related configurations. With continuous efforts in these directions, PBA is expected to develop from a model host material into a truly practical cathode for high-energy, fast charging, and durable.

5 Transition metal sulfide cathodes for AZIBs

Two-dimensional transition metal dichalcogenides (TMDs) have garnered significant attention as versatile inorganic cathodes materials due to their unique layered architectures, in which adjacent planes are maintained through weak interlayer van der Waals interactions.115 This structural feature not only facilitates rapid charge carrier transport but also imparts mechanical flexibility, allowing the material to buffer the volumetric fluctuations associated with multivalent ion insertion and extraction. Additionally, their intrinsic semiconducting nature with tunable bandgaps supports efficient electron conduction. Among various TMDs, molybdenum disulfide (MoS2) has emerged as a prototypical candidate for AZIBs, owing to its favorable electrochemical properties.116–118 However, its inherent drawbacks including poor electrical conductivity, limited structural integrity, and rapid capacity fading continue to impede its practical deployment. Consequently, advanced strategies are required to lower Zn2+ intercalation energy barrier and enhance overall performance.

A novel approach was introduced by Liu and co-workers, employing oxygen mediated interlayer chemical coupling to significantly enhance the electrochemical behavior of MoS2 cathodes in high load electrodes (Fig. 7i–k).119 Inserting oxygen rich β-CD into the MoS2 interlayer can promote the formation of oxygen mediated Mo–O and S–O bonds. This strategy not only effectively widens the interlayer spacing, but also reduces the coulombic interactions of Zn2+ with the layered structure, thereby endowing the anode with faster kinetics and stability. The poor diffusion kinetics of Zn2+ in MoS2 remains a key challenge for its practical deployment. Jia et al.120 developed a vertically stacked heterostructure of reduced graphene oxide (rGO) and mixed-phase MoS2 (1T-2H) via a bottom-up assembly approach. The MoS2/rGO vertical structure reduced the ion migration barrier and bandgap, thereby leading to enhanced Zn2+ migration and improved charge mobility. Consequently, the composite delivered a high capacity of 294.6 mAh g−1 at 0.2 A g−1 and excellent cycling stability with 96.8% retention after 1600 cycles at 3 A g−1. This strategy offers a universal route for designing vertically stacked 2D heterostructures as high-performance AZIBs cathodes.

In order to improve the utilization of storage sites in MoS2 and optimize storage performance, Liu group designed a MoS2/reduced graphene quantum dot (rGQDs) hybrid with enlarged interlayer spacing, enhanced charge transport ability, wettability, and robust layered structure via electrostatic self-assembly (Fig. 7l).121 The hybrid electrode, operated in a ZnSO4 + 0.5 M (NH4)2SO4 electrolyte, demonstrated a unique Zn2+/NH4+/H+ co-storage mechanism, where NH4+ and H+ ions occupy interstitial sites between Zn2+ to fill inactive gaps and boost active site utilization. This synergistic “gap-filling” strategy significantly improved charge storage, enabling a superior electrochemical capacity of 439.5 mAh g−1 at 0.1 A g−1 and remarkable capacity retention of 89.7% after 8000 cycles (Fig. 7m). DFT calculations revealed that Zn2+ and NH4+ preferentially adsorb at octahedral and tetrahedral sites in the MoS2 lattice, while H+ prefers sulfur-top positions, supporting the multi-ion co-insertion behavior and validating the theoretical basis for enhanced electrochemical performance.

Featured with robust lamellar frameworks, WS2 and VS2 as composite partners are often integrated with metal sulfides to give Zn2+-accessible layered paths, improved electron conductivity and structural buffering for boosting Zn2+ storage. Xun et al.122 grew enlarged-interlayer MoS2 nanosheets on carbon cloth (CC) via further in situ WS2 coating to form MoS2@WS2@CC. Benefiting from the conductive CC networks and WS2-expanded layers, it achieves enhanced ion diffusion and buffered volume changes to liberate high capacity (440 mAh g−1) and life (200 cycles). Sun et al.123 reported a self-constrained growth route to build rich-anion-vacancy VSSe/V2CTx heterostructures with multiscale V2CTx inner layer and selenized/sulfurized VSSe surface layer, which stabilize Zn2+ insertion/extraction, affording high capacity (350 mAh g−1) and cycling life (10[thin space (1/6-em)]000 cycles).

In conclusion, the optimization strategies for layered TMDs align closely with those employed for other two-dimensional materials, focusing on enhancing ion accessibility, electrical conductivity, and structural integrity. In future studies, advanced in situ and operando characterization techniques are expected to provide deeper insights into the relationship between interlayer structure evolution and electrochemical behavior, thereby clarifying Zn2+ storage mechanisms of TMD-based versatile inorganic cathodes. By integrating multiple modification approaches, such as doping, hybridization, interlayer engineering, and surface functionalization in a synergistic manner, it is anticipated that the performance limitations of layered TMDs can be effectively addressed, accelerating their practical application in high-performance AZIBs.

6 Halogen cathodes

Aqueous zinc–halide cathodes (Cl2, Br2, I2) have attracted considerable attention, especially Zn–Br2 and Zn–I2 systems, due to their abundant resources, reversible anion-redox chemistry, wide operating voltages, and high theoretical capacities.124,125 Unlike conventional cation-based batteries, these systems rely on halogen dissolution–deposition at the cathode and reversible Zn2+ plating at the anode. During oxidation, strong halogen–halogen interactions promote the formation of highly soluble polyhalides, which readily migrate and trigger severe shuttle effects, lowering coulombic efficiency and shortening cycle life. As a result, zinc–halide batteries mainly face two issues: (i) dissolution and shuttling of halide species and (ii) large polarization coupled with sluggish redox kinetics.

Halogen cathodes (Cl2/Br2/I2/polyhalides) generally rely on the reversible redox conversion reactions during (dis)charge, which liberate high theoretical capacity, high operating voltage, and rapid redox kinetics, providing a powerful complementary for AZIBs.125 However, halogen cathodes still face key challenges of shuttle, side reactions, and scale-up considerations. Specifically, soluble polyhalides (X3/X5) tend to migrate to the zinc anode under concentration gradient and electric field drive, leading to shuttle effects. The strong oxidizing properties of halogens can cause side reactions with electrolytes/electrodes, resulting in loss of active substances. In addition, the excellent performance of halogen cathodes is based on low mass loading (<2 mg cm−2), which is far from the actual demand (>10 mg cm−2). To address these issues, two efficient methods can be considered: (i) designing multi-level porous carbon/polymer hosts to fix halogens via physical confinement within micropores or cavities;126,127 (ii) introducing chemical adsorption sites (e.g., heteroatom doping, polar –OH/–COOH function groups, Zn/Fe metal coordination sites) into hosts to anchor polyhalides for reducing dissolution and improving reaction reversibility and stability.128–130

Therefore, designing halogen-confined host materials has become essential (Fig. 8). Focusing on structure and interface design is the core path to improve the performance of zinc halide batteries. Halogens have intrinsically low conductivity, resulting in poor redox reversibility and sluggish kinetics, and they are also unstable at room temperature, prone to volatilization and side reactions that cause active material loss and hinder practical use. Introducing halogen host materials with strong adsorption capacity is an effective way to address these issues. Through pore confinement and surface chemical adsorption, such hosts can spatially confine halogens/polyhalides and uniformly disperse them in the cathode. In this context, porous carbon materials with high conductivity and structural robustness are ideal halogen hosts, accommodating elemental halogens and polyhalide intermediates for high-performance zinc halide cathodes.


image file: d5sc09531j-f8.tif
Fig. 8 Strategies for enhancing the performance of ZHBs through cathode regulation.

For example, Wu et al.126 constructed a carbon-based framework PTCC900 using annealing strategy and assembled it as an iodine carrier to form the cathode of Zn–I2 battery PTCC900@I2 (Fig. 9a). This material constructs a multi-level pore network of nanopores (1.3–1.8 nm), which can achieve effective spatial confinement of I2 and multi-iodine species. Additionally, the disordered graphite structure inside PTCC900 enhances electron transfer, significantly improving conductivity. Consequently, PTCC900@I2 exhibits high capacity, excellent cycling stability, and outstanding rate performance. However, it is still difficult to develop a carbon-based halogen matrix that provides both high conductivity and precise design while maintaining controllable halogen diffusion. Tang et al.131 constructed hollow core–shell carbon nanospheres (HCSC) with an inner cavity structure based on the concept of structural confinement (Fig. 9b). This material has a developed hierarchical porous system, which can significantly enhance the specific surface area and bromine adsorption capacity of carbon felt, thereby endowing the electrode with higher catalytic activity. More importantly, by utilizing the adsorption and confinement effect of cavities on bromine, active bromine is effectively trapped inside the carbon spheres, significantly reducing the self-discharge behavior of the system. This work indicates that hollow carbon spheres as bromine-based materials provide a fresh structural control path for constructing excellent zinc halide batteries.


image file: d5sc09531j-f9.tif
Fig. 9 Design strategies for halogen cathodes. (a) Schematic illustration of the synthesis of PTCC900@I2.126 Copyright 2023, Elsevier. (b) Schematic diagram of working mechanism.131 Copyright 2025, Elsevier. (c) Schematic synthesis of cubic Zn-MOF derived NC and I2@NC.132 Copyright 2025, Wiley-VCH. (d) The adsorption energy and charge density patterns of different bromine compounds.133 Copyright 2023, Elsevier. (e) Prepare the program and working mechanism diagram. (f) Density functional theory calculations.135 Copyright 2025, Royal Society of Chemistry. (g) Schematic diagram of Zn–Cl2@MnO2 battery. (h) Photos of electrolyte after cycling. (i) Density functional theory calculations.136 Copyright 2023, Wiley-VC.

Relying solely on weak van der Waals interactions between pore walls and halides/polyhalides is insufficient to effectively suppress polyhalide shuttling. To strengthen polyhalide anchoring, heteroatoms such as oxygen, nitrogen, and sulfur, along with corresponding polar functional groups, are commonly introduced into the carbon framework to enhance halogen conversion efficiency and extend battery lifespan. Such heteroatom-regulated porous carbons, with increased polarity and tunable electronic structures, are regarded as highly promising halogen hosts because they significantly reinforce the interactions between the carbon matrix and halide ions. Pang group developed a nitrogen-doped carbon (NC) material derived from Zn-MOF as a cathode host for aqueous Zn–I2 batteries.132 CTAB, acting as a surfactant and capping agent, regulates the growth of Zn-MOF nanocubes. The resulting high surface area micropores enhanced the conversion kinetics of iodine, suppressed the I3 shuttle effect, and provided abundant active sites (Fig. 9c). Mesopores further improve iodine accommodation and facilitate electron/ion transfer. Additionally, pyridine-N/graphite-N doping aids iodine species adsorption and conversion. I2@S3-1000 cathodes exhibit excellent long-term cycling stability due to these benefits.

Sun et al.127 proposed a dual-doping strategy with boron and nitrogen to locally regulate the electronic environment of carbon hosts, thereby boosting Zn–I2 battery performance. Combined experimental and DFT results indicate that N–B sites effectively suppress the shuttle effect, strengthen interactions with iodide species, and accelerate their catalytic conversion kinetics. Wang et al.128 fabricated a Prussian blue-modified nitrogen-doped carbon (PB@NC) composite via a simple anion-exchange route and loaded it onto a carbon membrane. The nitrogen-doped carbon provides high conductivity and strong adsorption toward bromine species, enabling efficient electron transport and local bromine enrichment at the reaction interface. Under the electronic assistance of NC, Prussian blue can rapidly switch between oxidized and reduced states, then selectively engage in redox reactions with Br2. This offers an alternative bromine redox pathway, markedly accelerating electrochemical kinetics and realizing targeted, reversible redox catalysis.

The non-polar carbon skeleton only provides weak physical adsorption, which is not sufficient to effectively suppress the shuttle of polyhalides. In contrast, host materials with polar functional groups can form stronger interactions with halide ions through chemical adsorption or hydrogen bonding, thereby anchoring polyhalides on the cathode surface, limiting their dissolution and diffusion in the electrolyte, and ultimately extending battery life. For example, Zeng et al.129 developed asphalt-derived carbon (PPCMK) with a microporous structure and abundant oxygen groups (C[double bond, length as m-dash]O, –COOH, –OH) using a one-step method to create iodine-based cathodes (I2/PPCMK). The micropores in PPCMK efficiently prevent I2 dissolution and I3 formation, while its high surface area boosts iodine loading. DFT calculations show that the oxygen groups (C[double bond, length as m-dash]O, –COOH, –OH) in PPCMK strengthen the adsorption of free I3 through strong chemical interactions. Due to its dual iodine-confining mechanism, PPCMK maintains excellent stability under both standard and high-load conditions. Indeed, COFs are more closely related to organic material systems and thus cannot be classified as an inorganic material. It should be pointed out that COFs are often selected as the redox-nonactive supporter materials for loading halogen cathodes (e.g., I2/Br2, polyhalides), which can effectively anchor halogen species to suppress their dissolution/shuttling and provide fast interfacial ion/electron transport paths. Liu and co-worker constructed a trifluoromethyl-functionalized covalent organic framework (F-COF) as an iodine host to suppress the shuttle effect.133 The strong electron-withdrawing trifluoromethyl functional groups redistribute charge in the COF backbone, enhancing iodine uptake and stabilizing polyiodide species. Theoretical calculations confirm that F-COF exhibits strong adsorption toward polyiodides, effectively inhibiting their migration (Fig. 9d). Consequently, Zn–I2 batteries employing F-COF as the iodine host deliver highly reversible behavior and ultralong cycling stability (40[thin space (1/6-em)]000 cycles at 50C).

Building efficient catalysts is an important way to achieve high energy density and long lifespan of zinc–halide cathodes. Metal catalysts accelerate halogen oxidation-reduction by adjusting X–X (X = I, Br, Cl) bond structure and reducing the conversion energy barrier, and are therefore commonly introduced as carbon-based hosts to enhance electrochemical performance. For example, Zhi group designed a mesoporous carbon-based conductive bromine host (FeSAC-CMK) in which isolated iron single atoms (FeN5 sites) are coordinated by nitrogen.130 These FeN5 centers can strongly immobilize neutral bromine (Br0), effectively suppress the formation of Br3, and bifunctionally catalyze the Br/Br0 redox conversion. By releasing one-third of Br that would otherwise be locked in Br3 complexes, FeN5 sites enhance bromine utilization and reversibility. As a result, Zn–Br2 batteries equipped with this dual-functional catalytic host achieve higher discharge capacity, elevated voltage plateau, improved rate performance, and prolonged cycling life. Tulchinsky et al.134 constructed and verified a cobalt MOF based on N-containing imidazole ligands, in which unsaturated Co(II) sites are quantitatively oxidized by halogens to form stable solids bearing terminal Co(III)–halogen bonds. Upon thermal treatment, these Co(III)–halogen bonds undergo homolytic cleavage, regenerating Co(II) and releasing elemental halogen. This work clarifies how MOFs can confine and reversibly adsorb halogen species, and provides a viable route to designing ZnCl2 cathodes with high safety, reversibility, and performance.

Although single metal atom catalysts exhibit excellent activity in the zinc–halide cathodes system, they often face stability issues such as atomic aggregation and active site leaching under actual working conditions. On the other hand, they are also inherently limited by scaling relationships: enhancing the adsorption of one reactant often weakens the binding ability to another intermediate. This contradiction is particularly prominent in Zn–I2 batteries, where multiple intermediate species such as I, I3, I5, and I2 have significantly different affinities for catalytic sites, making it difficult for a single metal center to simultaneously achieve optimal regulation of each reaction step. Based on this, bimetallic catalysts exhibit greater design freedom and outstanding comprehensive catalytic performance in multi-step halogen conversion reactions due to their adjustable bimetallic synergistic effect and richer charge interaction modes. Mai and co-workers developed honeycomb-like Zn–Zn dual-metal sites anchored on N-doped carbon nanosheets via a novel co-pyrolysis strategy to serve as iodine host centers, as confirmed by microscopic and spectroscopic characterization (Fig. 9e).135 Electrochemical tests combined with theoretical calculations reveal that these Zn2 sites not only strengthen I2 adsorption but also accelerate multi-iodide redox kinetics (Fig. 9f). Consequently, the I2@Zn2NC cathode delivers high capacity and ultralong cycling durability, sustaining 100[thin space (1/6-em)]000 cycles at 50C.

In order to further improve the interfacial charge transfer ability and catalytic performance of host materials, metal compounds have been introduced to create structures for rapid electron transfer. Chen group abandoned traditional carbon hosts and instead employed a low-cost MnO2 redox adsorbent to regulate Cl2 electrochemistry (Fig. 9g and h).136 DFT calculations and kinetic analysis reveal that the intermediate Clads@MnO2 acts as an electron donor, accelerating electrode kinetics and Cl2 reduction while contributing to capacity enhancement (Fig. 9i). Benefiting from the synergistic interaction of Mn2+/MnO2 with chlorine during both dis(charge), the Zn–Cl2@MnO2 battery shows improved reaction dynamics, coulombic efficiency, and cycling stability. This Cl2 cathode regulation strategy provides a methodological approach for the research of aqueous Zn–Cl2 batteries.

To further expand the application scope of limited catalytic strategies in halogen hosts, Liang group developed a Co9S8@nitrogen-doped carbon catalyst with an anti-perovskite structure.137 This design allows Co9S8 nanoparticles to be uniformly confined within a porous honeycomb-like N-doped carbon framework. Besides, the Co9S8 phase features an electron-deficient character, which induces strong electrostatic attraction and robust anchoring toward iodine species. As a result, the Co9S8@NC catalyst delivers a high energy density of 554 Wh kg−1 and maintains stable cycling performance over 5000 cycles.

Although the current design strategy for halogen materials has made progress, it still faces several challenges: (i) insufficient regulation of the pore structure in carbon materials makes it difficult to simultaneously achieve sufficient electrolyte infiltration, charge transfer, and full exposure of storage sites; (ii) although surface functionalization can improve halogen anchoring, precise control of functional group sites remain difficult, which may result in uneven electrode surface reactions; (iii) many carbon-based materials are difficult to achieve precise control over the electronic structure and conversion pathways of halogen species due to physical limitations. In the future, electron rich regions should be introduced by doping heteroatoms, optimizing interface polarity, ion distribution, and creating ordered hierarchical pore structures to effectively improve ion transport efficiency. Meanwhile, metal atom doping can enhance the adsorption and catalytic performance of halogen substances, suppress shuttle effects, and accelerate redox reactions. The doping of heteroatoms still faces problems such as unclear regulatory mechanisms and decreased conductivity. In the future, in situ characterization and theoretical calculations should be strengthened, and multi-component co-doping schemes should be explored to enhance the confinement, catalytic, and conductive capabilities of iodine species, and promote the development of Zn–halogen batteries.

7 Summary and outlook

This article reviews the latest developments in versatile inorganic cathodes for AZIBs, covering major categories such as Mn-based materials, V-based materials, PBAs, transition metal sulfides, and emerging halogen cathodes. There are three charge-storage mechanisms in inorganic cathodes for AZIBs: Zn2+ storage, H+ storage, and H+/Zn2+ co-storage, resulting in different electrochemical performances. Zn2+ ion (or hydrated structures) is a typical charge carrier, but its large hydrated size and high desolvation energy trigger slow interfacial reaction. In contrast, the smallest-radius H+ can transfer along the H-bonding network of water, and enter the interlayer of inorganic cathodes to achieve fast charge storage, but is prone to corrode inorganics, resulting in inferior cycling stability of AZIBs. Significantly, H+/Zn2+ co-storage enables fast charge compensation to mitigate polarization, and contributes to superior reversible (de)insertion energy storage, thereby synergistically enhancing the capacity and rate performance of AZIBs.

The key performance indicators of these materials in battery systems, such as discharge capacity, rate capability, energy density, and cycling stability, are compared. Table 1 summarizes the key performance characteristics of versatile inorganic cathode materials based on the semi-quantitative rationale. The electrochemical performances of various inorganic cathode materials were compared by prioritizing literature results tested under identical conditions for AZIBs (electrolyte: ZnSO4/H2O and Zn(OTF)2/H2O solution; voltage window: 0∼1.8 V; mass load: 1∼2 mg cm−2; current density: 0.1∼0.5 A g−1). Mn-based cathodes often exhibit large interlayer spacing to achieve high Zn2+ diffusion coefficient (DZn2+, 10−15∼10−4 cm2 s−1). In contrast, the interaction between Zn2+ and V–O in V-based cathodes are stronger, resulting in a decrease in DZn2+ (10−11∼10−6 cm2 s−1). Although PBAs have open 3D channels, the transport of Zn2+ is limited by the influence of structural water, resulting in relatively low DZn2+ (10−15∼10−9 cm2 s−1). Compared with layered Mn/V-based cathodes, layered TMDs often show low DZn2+ (10−10∼10−8 cm2 s−1) due to narrower ion channels.

Table 1 Comparison of electrochemical properties of AZIBs with different cathodes
Materials Mass loading (mg cm−2) Electrolyte Voltage (V) Capacity (mAh g−1) Current (A g−1) Cycles Retention rate (%) Current (A g−1) Ref.
Mn-based compounds
α-MnO2 N/A 1 M ZnSO4 1–1.8 197 0.13 75 50 0.084 62
NS-MnO2 1.5 2 M ZnSO4 + 0.1 M MnSO4 0.8–1.8 284 0.2 1500 94 1 69
Cein/inter-MnO2 1–2 2 M ZnSO4 + 0.1 M MnSO4 0.9–1.8 270.9 0.3 2000 100 3 70
Al0.1–MnO2 1.5 2 M ZnSO4 + 0.1 M MnSO4 0.8–1.8 347.6 0.1 1000 87 1 71
HE-MnO/C 1–1.5 2 M ZnSO4 + 0.2 M MnSO4 0.2–1.8 230.2 0.3 10[thin space (1/6-em)]000 92.3 10 72
KMO-NAPD 2 2 M ZnSO4 + 0.4 M MnSO4 0.8–1.9 233 1 1000 85 4 73
DP-MnO2 1.5 2 M ZnSO4 + 0.1 M MnSO4 1–1.8 357 0.1 1000 N/A 1 74
3DP MnO2 2.7 1 M ZnSO4 + 0.1 M MnSO4 1–1.8 288.8 N/A N/A N/A N/A 75
C-MnO2 1.5 2 M ZnSO4 + 0.2 M MnSO4 0.6–1.8 302 0.2 10[thin space (1/6-em)]000 78 5 76
γ-MnO2@CP 2 2 M ZnSO4 + 0.1 M MnSO4 0.8–1.8 391.2 0.1 3000 92.1 5 77
VMn-Mn3O4@C 1.5 2 M ZnSO4 + 0.2 M MnSO4 1–1.8 280.9 0.1 5000 100 1 83
Zn0.17MnO2−n·0.52H2O 1.5 2 M ZnSO4 + 0.2 M MnSO4 0.8–1.9 558 0.1 5000 95.8 5 84
NC@VN/MnO 1.5 2 M ZnSO4 + 0.2 M MnSO4 0.7–1.8 550 0.2 12[thin space (1/6-em)]000 83 10 85
Zn0.5Mn2O4 1 3 M ZnSO4 + 0.2 M MnSO4 1–1.8 299 0.1 3200 92 10 86
[thin space (1/6-em)]
V-based compounds
V2O5 N/A 3 M ZnSO4 0.4–1.4 224 0.1 400 54 2 91
MxV2O5·nH2O 1.5 2 M Zn(OTF)2 0.2–1.6 N/A N/A 1000 88.4 0.2 89
IO-V2O5 1.5 3 M Zn(OTF)2 0.2–1.6 549.5 0.2 20[thin space (1/6-em)]000 80.1 30 98
PEDOT-SO3-ZnVO 1.5 2 M ZnSO4 0.2–1.6 310 0.2 5000 90.3 5 99
VSSe/VO2/V2O5 1–1.2 3 M Zn(OTF)2 0.1–1.7 432 1 12[thin space (1/6-em)]000 60 10 100
Sn-V3O7·H2O 1.5 3 M Zn(OTF)2 0.4–1.5 408 0.1 6000 89.3 5 101
Cu-HHTP 2 3 M Zn(OTF)2 0.2–1.6 518 0.2 5000 81 10 102
VO2(B) 1 3 M Zn(OTF)2 0.2–1.5 420.8 0.1 5000 84.3 10 32
H-NVO 1.5 3 M Zn(OTF)2 0.2–1.6 352 0.05 6000 90 5 103
HNVO-Glu 1.5 3 M Zn(OTF)2 0.2–1.6 354.6 1 12[thin space (1/6-em)]000 87.2 10 104
HE-NVPF@C 10 1.7 M Zn(OTF)2 0.8–1.9 74.1 0.5 6000 81 20 105
[thin space (1/6-em)]
Prussian blue analogues
CuHCF N/A 2 M ZnSO4 0.45–1.4 53 0.06 100 96.3 N/A 108
CuMn-PBA DSNBs 1 2 M Zn(OTF)2 0.5–1.8 116.8 0.1 2000 96.8 1  
CuMn PBA-2 1.2 2 M ZnSO4 + 0.2 M MnSO4 0.7–1.9 175 0.5 2000 N/A 3  
CoHCF/M-1% 1.2–1.5 15 M ZnCl2 0.7–2.0 197 0.1 3000 95.3 2  
V-PBA 1 3 M Zn(OTF)2 0.2–2.0 120.7 0.5 10[thin space (1/6-em)]000 55 10  
AgHCF-3 2 1 M ZnSO4 0.5–2.0 79.6 0.02 100 90.3 0.2  
[thin space (1/6-em)]
Transition metal sulfides
MoS2 N/A 3 M Zn(OTF)2 0.2–1.4 21 0.1 N/A N/A N/A 118
MoS2-β-CD 10 2 M ZnSO4 0–1.4 228 4 5000 85.3 20 119
MoS2/rGO 1.5–2.0 3 M Zn(OTF)2 0.2–1.5 294.6 0.2 1600 96.8 3 120
MoS2/rGQDs 2–3 1 M ZnSO4 + 0.5 M (NH4)2SO4 0.2–1.5 439.5 0.1 8000 89.7 10 121
VSSe/V2CTx 3 3 M Zn(OTF)2 0.3–1.6 355 0.2 10[thin space (1/6-em)]000 51 10 123
[thin space (1/6-em)]
Halogens
PTCC900@I2 N/A 2 M ZnSO4 0.8–1.6 242 0.1 50[thin space (1/6-em)]000 45 5 126
I2@S3-1000 N/A 2 M ZnSO4 0.6–1.6 208.5 0.05 10[thin space (1/6-em)]000 81 2 132
I2/PPCMK 1.5–2.5 2 M ZnSO4 0.5–1.6 236 0.21 20[thin space (1/6-em)]000 85 4.4 129
F-COF N/A 3 M ZnSO4 0.8–1.9 275 0.5 1000 83 2 133
FeSAC-CMK 1 2 M ZnSO4 + 0.1M Br2 1–1.9 344 0.2 2000 76 2 134
I2@Zn2NC N/A 2 M ZnSO4 0.6–1.8 212 0.5C 100[thin space (1/6-em)]000 N/A 50C 135
I/Co9S8@NC N/A 7.5 m ZnCl2 0.6–1.8 458 1 5000 N/A 5 137


Table 1 compares various inorganic cathode materials and emphasizes their inherent trade-off between capacity and cycling durability in AZIBs. Specifically, compared with pristine MnO2, multivalent redox chemistry endows Mn-based oxides with high capacity (230–400 mAh g−1). However, the Jahn–Teller distortion results in structural pulverization of Mn-based cathodes, accelerating performance degradation during long-term cycling. In contrast, the modified V-based oxides with more open and stable layered V–O frameworks deliver better capacity (310–500 mAh g−1) compared to V2O5. In addition, modified PBAs with open 3D channels generally exhibit good cycling stability (∼10[thin space (1/6-em)]000 cycles) compared with pristine CuHCF, but face slow ion transport and low capacity (80–200 mAh g−1). Featured with good structural elasticity, compared with pristine MoS2, TMDs exhibit high capacity (200–400 mAh g−1). However, during the long cycle process, TMDs often undergo structural degradation, leading to increased polarization and subsequently a decrease in cycle life (1000–8000 cycles). Different from the abovementioned insertion-type metal compounds, conversion-type halogens activate multielectron redox pairs to deliver good capacity (200–400 mA h g−1) and long cycle life.

Overall, progress has been made in the development of inorganic cathodes, with each type of material possessing unique structural advantages and electrochemical properties. But several key challenges must be addressed to accelerate the development of versatile inorganic cathode materials for next-generation AZIBs.

(i) In practical conditions, Mn/V oxides, PBAs, TMDs and halogen materials in AZIBs typically use the mass loading of 1∼2 mg cm−2 in cathodes, excess Zn metal anodes (diameter: 14 mm; thickness: 50∼100 µm), electrolyte amount (∼120 µL), cutoff voltage window (V oxides/TMDs: 0.2–1.6 V; Mn oxides/PBAs/halogen: 0.8–1.9 V), and long-term stability metrics (3000∼10[thin space (1/6-em)]000 cycles). Under these consolidated condition, different inorganic materials show differential electrochemical performances benefiting from their respective structural features, which provide feasible and useful platforms to propel the future development of next-generation energy communities.

(ii) Cathodic optimization. In addition to existing modification methods, it is particularly urgent to develop innovative strategies to enhance the performance of versatile inorganic cathodes. Meanwhile, the diffusion of Zn2+ in the cathode is often limited by strong electrostatic interactions. Therefore, in the future, it may be considered to introduce low electronegativity materials or form a three-dimensional framework structure to alleviate the dynamic bottleneck caused by strong electrostatic interactions. In addition, exploring new stable cathode material systems, such as bismuth based or metal phosphide materials, will provide feasible high-performance solutions for large-scale AZIBs.

(iii) Electrolyte engineering design. Traditional aqueous electrolytes are limited by a narrow electrochemical stability window, making it difficult to support higher operating voltages and energy outputs. Therefore, it is necessary to expand the “available window” by regulating the solvation structure and ionic environment. For example, ultra-high concentration electrolytes, deep eutectic systems, and water/organic mixed electrolytes are expected to achieve higher potential operation while suppressing side reactions and active substance dissolution; at the same time, introducing functional additives can optimize the behavior of the electrode/electrolyte interface, weaken adverse processes such as hydrogen evolution and organic component decomposition. Further, the development of gel polymer and all solid electrolyte is expected to significantly improve flexibility and safety on the premise of ensuring ion conduction, providing new design space for zinc ion batteries for wearable energy storage devices.

(iv) Although significant efforts have been made to explore future applications of high-mass-loading inorganic cathodes, their scalable, reproducible, and cost-effective fabrication with desirable electrochemical properties are still challenging. Most reported excellent properties of inorganic cathodes are based on the low mass loading (<2 mg cm−2), which is far away from the practical level (>10 mg cm−2). It is thus of great importance to explore new techniques to extend the production scale of sustainable inorganic cathodes from the laboratory stage to the practical industrial level.

(v) The future routes of developing high-energy-density AZIBs should be focused on the collaborative enhancement of capacity and voltage in high-mass-loading inorganic cathodes: (i) increasing the redox-site density (e.g., constructing rich lattice defects, expanding interlayers) and improving electron/ion transport (e.g., introducing conductive substrates, rich porosity within inorganics) for achieving desirable capacity storage; (ii) elevating redox potentials within stable electrochemical windows (e.g., introducing polyanions within inorganic lattices, heteroatom substitution).

(vi) AI intelligence and representation. In multi-coupled inorganic electrode systems, structural evolution and reaction pathways are often highly complex, making it difficult to fully elucidate their working mechanisms within a single disciplinary framework. This calls for closer integration of materials chemistry, electrochemistry, theoretical modeling, and data science, with tight coupling between experiments and simulations. At the same time, in situ and quasi in situ characterization techniques, such as synchrotron X-ray methods, in situ Raman and infrared spectroscopy, and time-resolved electrochemical impedance analysis are essential for tracking phase transitions, interfacial reconstruction, and ion migration pathways under realistic operating conditions, thereby providing mechanistic guidance for the rational design of high-performance electrodes. Furthermore, the combination of machine learning, automated high-throughput experimentation, and intelligent optimization algorithms is expected to rapidly identify promising electrode/electrolyte pairs within a vast compositional and structural space, significantly shortening the cycle from conceptual design to device validation and accelerating the iterative development of next-generation zinc-based energy storage systems.

(vii) Sustainable development and feasibility. The synthesis of high-performance multifunctional inorganic cathode materials often relies on complex processes such as multi-step precursor design, strict atmosphere control, or high-temperature long-term annealing, which not only increases energy consumption and equipment requirements, but also weakens the repeatability of the process and the feasibility of large-scale production. Therefore, developing green, low-cost, and process scalable synthetic routes (such as aqueous/solvothermal synthesis, low-temperature solid-phase reactions, and resource reuse based on biomass or industrial by-products) is crucial for achieving a balance between electrochemical performance, preparation costs, and environmental sustainability. In the future, we should also pay attention to process compatibility and engineering feasibility, such as matching with existing battery manufacturing processes such as coating, rolling, 3D printing, and electrode roll to roll production. This is expected to promote the development of multifunctional inorganic cathodes from laboratory concepts to large-scale, low-cost practical applications.

Author contributions

Conceptualization, Kang Guo, Yaokang Lv, Ziyang Song, Lihua Gan, Mingxian Liu; writing – original draft preparation, Kang Guo; figure and table preparation, Kang Guo; writing – review and editing, Ziyang Song, Lihua Gan, Mingxian Liu. All authors have read and agreed to publish the version of manuscript.

Conflicts of interest

The authors declare no conflicts of interest.

Data availability

The data that support the findings of this study are available on request from the corresponding author, upon reasonable request.

Acknowledgements

This work is financially supported by the National Natural Science Foundation of China (No. 22272118, 22172111, and 22309134), the Shanghai Rising-Star Program (23YF1449200), the Zhejiang Provincial Science and Technology Project (2022C01182), and the Fundamental Research Funds for the Central Universities.

Notes and references

  1. B. Dunn, H. Kamath and J. M. Tarascon, Science, 2011, 334, 982 Search PubMed.
  2. M. Armand and J.-M. J. N. Tarascon, Nature, 2008, 451, 652–657 CrossRef CAS PubMed.
  3. S. Zhao, Y. Zhang, J. Li, L. Qi, Y. Tang, J. Zhu, J. Zhi and F. Huang, Adv. Mater., 2023, 35, 202300195 Search PubMed.
  4. P. D. Lund, Joule, 2020, 4, 2543–2545 CrossRef.
  5. J. Deng, C. Bae, A. Denlinger and T. Miller, Joule, 2020, 4, 511–515 CrossRef.
  6. A. Huang, J. Xu, Y. Huang, G. Chu, M. Wang, L. Wang, Y. Sun, Z. Jiang and X. Zhu, Acta Phys. Chim. Sin., 2025, 41, 100037 CrossRef.
  7. M. R. Palacín, Chem. Soc. Rev., 2018, 47, 4924–4933 RSC.
  8. J. Liu, Z. Zhang, M. Kamenskii, F. Volkov, S. Eliseeva and J. Ma, Acta Phys. Chim. Sin., 2025, 41, 100011 CrossRef.
  9. C. M. Costa, J. C. Barbosa, R. Gonçalves, H. Castro, F. J. D. Campo and S. Lanceros-Méndez, Energy Storage Mater., 2021, 37, 433–465 Search PubMed.
  10. M. S. Whittingham, Nano Lett., 2020, 20, 8435–8437 CrossRef CAS PubMed.
  11. H. Bajolle, M. Lagadic and N. Louvet, Energy Res. Social Sci., 2022, 93, 102850 CrossRef.
  12. L. F. Zhao, Z. Hu, W. H. Lai, Y. Tao, J. Peng, Z. C. Miao, Y. X. Wang, S. L. Chou, H. K. Liu and S. X. Dou, Adv. Energy Mater., 2020, 11, 202002704 Search PubMed.
  13. P. K. Nayak, L. Yang, W. Brehm and P. Adelhelm, Angew. Chem., Int. Ed., 2017, 57, 102–120 CrossRef.
  14. Y. Gao, Q. Yu, H. Yang, J. Zhang and W. Wang, Adv. Mater., 2024, 36, 2405989 CrossRef CAS.
  15. H. Zhang, Y. Gao, X. Liu, L. Zhou, J. Li, Y. Xiao, J. Peng, J. Wang and S. L. Chou, Adv. Energy Mater., 2023, 13, 2300149 CrossRef CAS.
  16. Y. Zheng, Y. Meng, X. Hu, H. Peng, L. Feng, Y. Wang and B. Li, Adv. Mater., 2024, 37, 2413202 CrossRef.
  17. Y. Wang, Z. Cao, Z. Du, X. Cao and S. Liang, Acta Phys. Chim. Sin., 2025, 41, 100035 CrossRef.
  18. H. Zhang, X. Liu, H. Li, I. Hasa and S. Passerini, Angew. Chem., Int. Ed., 2020, 60, 598–616 Search PubMed.
  19. Y. Liang and Y. Yao, Nat. Rev. Mater., 2022, 8, 109–122 Search PubMed.
  20. D. Chao, W. Zhou, F. Xie, C. Ye, H. Li, M. Jaroniec and S.-Z. Qiao, Sci. Adv., 2020, 6, eaba4098 Search PubMed.
  21. M. Huang, X. Wang, J. Wang, J. Meng, X. Liu, Q. He, L. Geng, Q. An, J. Yang and L. Mai, Angew. Chem., Int. Ed., 2023, 62, e202308961 CrossRef CAS PubMed.
  22. D. Xie, Y. Wang, L. Tian, H. Huang, J. Sun, D. W. Kim, J. Zhao and J. Mao, Adv. Funct. Mater., 2024, 35, 2413993 CrossRef.
  23. J. Wei, P. Zhang, J. Sun, Y. Liu, F. Li, H. Xu, R. Ye, Z. Tie, L. Sun and Z. Jin, Chem. Soc. Rev., 2024, 53, 10335–10369 RSC.
  24. K. Du, Y. Liu, Y. Zhao, H. Li, H. Liu, C. Sun, M. Han, T. Ma and Y. Hu, Adv. Mater., 2024, 36, 2404172 Search PubMed.
  25. X. Zhang, R. Wang, Z. Liu, Q. Ma, H. Li, Y. Liu, J. Hao, S. Zhang, J. Mao and C. Zhang, Adv. Energy Mater., 2024, 14, 2400314 CrossRef CAS.
  26. Y. Fu, Y. Zhang, Q. Huang, P. Liu, Y. Lv, Z. Song, L. Gan and M. Liu, Mater. Horiz., 2025, 12, 6733–6740 RSC.
  27. W. Du, Q. Huang, Y. Lv, Z. Song, L. Gan and M. Liu, Energy Environ. Sci., 2026 10.1039/d5ee04802h.
  28. Y. Zhang, F. Wan, S. Huang, S. Wang, Z. Niu and J. Chen, Nat. Commun., 2020, 11, 2199 CrossRef CAS PubMed.
  29. G. Zampardi and F. La Mantia, Nat. Commun., 2022, 13, 687 CrossRef CAS PubMed.
  30. J. J. Ye, P. H. Li, Z. Hou, W. Zhang, W. Zhu, S. Jin and H. Ji, Angew. Chem., Int. Ed., 2024, 136, e202410900 CrossRef.
  31. M. Wu, Y. Sun, Z. Yang, S. Deng, H. Tong, X. Nie, Y. Su, J. Li and G. Chai, Angew. Chem., Int. Ed., 2024, 136, e202407439 CrossRef.
  32. Q. He, T. Hu, Q. Wu, C. Wang, X. Han, Z. Chen, Y. Zhu, J. Chen, Y. Zhang, L. Shi, X. Wang, Y. Ma and J. Zhao, Adv. Mater., 2024, 36, 202400888 Search PubMed.
  33. Z. Song, W. Liu, Q. Huang, Y. Lv, L. Gan and M. Liu, Chem. Sci., 2025, 16, 16542–16551 RSC.
  34. Y. Hu, P. Wang, M. Li, Z. Liu, S. Liang and G. Fang, Energy Environ. Sci., 2024, 17, 8078–8093 RSC.
  35. Y. Qin, C. Hu, Q. Huang, Y. Lv, Z. Song, L. Gan and M. Liu, Nano-Micro Lett., 2026, 18, 38 CrossRef CAS PubMed.
  36. Y. Zhang, Z. Song, Q. Huang, Y. Lv, L. Gan and M. Liu, Angew. Chem., Int. Ed., 2025, 64, e202423936 CrossRef CAS PubMed.
  37. L. E. Blanc, D. Kundu and L. F. Nazar, Joule, 2020, 4, 771–799 CrossRef CAS.
  38. S. Li, M. Li, X. Chi, X. Yin, Z. Luo and J. Yu, Acta Phys. Chim. Sin., 2025, 41, 100003 CrossRef.
  39. D. Zhao, Q. Huang, Y. Lv, Z. Song, L. Gan and M. Liu, Mater. Horiz., 2026, 13, 252–261 RSC.
  40. J. Yue, S. Chen, J. Yang, S. Li, G. Tan, R. Zhao, C. Wu and Y. Bai, Adv. Mater., 2023, 36, 202304040 Search PubMed.
  41. Y. Lu, Z. Wang, M. Li, Z. Li, X. Hu, Q. Xu, Y. Wang, H. Liu and Y. Wang, Adv. Funct. Mater., 2024, 34, 202310966 Search PubMed.
  42. P. Liu, Y. Lv, Z. Song, L. Gan and M. Liu, Small, 2025 DOI:10.1002/smll.202511967.
  43. L.-L. Zhao, Y.-H. Zhao, Y.-M. Wu, P.-F. Wang, Z.-L. Liu, Q.-Y. Zhang, J. Shu and T.-F. Yi, Energy Storage Mater., 2025, 78, 104299 CrossRef.
  44. M. Yang, J. Zhu, J. Lin, L. He, M. Chen, Y. Wang, J. Chen, S. Zhong, H. Mi, C. He, D. Ma and P. Zhang, Angew. Chem., Int. Ed., 2025, 64, e202510893 CrossRef CAS PubMed.
  45. Y. Liu, Y. Sun, J. Zhang, X. Hao, M. Zhang, P. Wei, X. Zhao and K. Cai, Nano Energy, 2024, 120, 109152 CrossRef CAS.
  46. Y. Zhang, Y. Fu, Y. Lv, Z. Song, L. Gan and M. Liu, Chem. Commun., 2025, 61, 14611–14624 RSC.
  47. Y. Ding, C. Cai, L. Ma, J. Wang, M. P. Mercer, J. Liu, D. Kramer, X. Yu, D. Xue, C. Zhi and C. Peng, Adv. Energy Mater., 2024, 15, 2402819 CrossRef.
  48. D. Zhang, Z. Song, Y. Chen, P. Liu, R. Gu, L. Miao, Y. Lv, Y. Wang, L. Gan and M. Liu, Angew. Chem., Int. Ed., 2025, 64, e21269 CrossRef CAS PubMed.
  49. F. Xiankai, X. Kaixiong, Z. Wei, D. Weina, Z. Hai, C. Liang and C. Han, Carbon Energy, 2024, 6, e536 CrossRef.
  50. X. Zhang, X. Ma, H. Bi, Y. Zhang, P. Mi, F. Liu, X. Jin, Y. Chen, K. Zhang, J. Wang and Y. Dong, Adv. Funct. Mater., 2024, 35, 2411990 CrossRef.
  51. C. Wang, B. H. Xiao, J. Huang, K. Xiao and Z. Q. Liu, Adv. Funct. Mater., 2024, 34, 2405680 CrossRef CAS.
  52. X. Shi, C. Zhou, F. Yang, L. Shan, B. Tang, J. Zhang, Q. Nan, Y. Xie, J. Li, H. Li and X. Tian, ACS Energy Lett., 2024, 9, 1063–1072 CrossRef CAS.
  53. Q. Li, Q. Jiao, Z. Li, C. Lu, H. Yang, Y. Liu, Z. Yang and C. Feng, Small, 2024, 21, 2409217 CrossRef.
  54. Y.-Z. Zhu, K. Wang, S.-S. Zheng, H.-J. Wang, J.-C. Dong and J.-F. Li, Acta Phys. Chim. Sin., 2024, 40, 2304040 CrossRef.
  55. M. Xie, X. Zhang, R. Wang, Y. Jiao, Z. Shu, S. Shan, Y. Bian, H. Lin, J. Chen and Y. Xu, Chem. Eng. J., 2024, 494, 152908 CrossRef CAS.
  56. C. Zhao, M. Wu, W. Lu, Y. Cheng, X. Zhang, I. Saadoune, R. Lian, Y. Wang and Y. Wei, Small, 2024, 20, 202401379 Search PubMed.
  57. D. Qin, J. Ding, C. Liang, Q. Liu, L. Feng, Y. Luo, G. Hu, J. Luo and X. Liu, Acta Phys. Chim. Sin., 2024, 40, 2310034 CrossRef.
  58. T. He, L. Xiao, J. Li and Y. Zhu, J. Alloys Compd., 2025, 1015, 178890 CrossRef CAS.
  59. Y. Wang, X. Wang, A. Zhang, X. Han, J. Yang, W. Chen, R. Zhao, C. Wu and Y. Bai, Small, 2024, 20, 202403136 Search PubMed.
  60. Z. Zhou, J. Tong, X. Zou, Y. Wang, Y. Bai, Y. Yang, Y. Li, C. Wang and S. Liu, J. Mater. Chem. A, 2024, 12, 10923–10931 RSC.
  61. K. Zhu, W. Zhuang, N. Wang, K. Zhang, L. Lin, Z. Shao, C. Li, W. Wang, S. Liu, P. Yang, P. Xue, Q. Zhang, G. Hong and Y. Yao, Adv. Mater., 2025, 37, 2502366 CrossRef CAS.
  62. M. H. Alfaruqi, S. Islam, J. Gim, J. Song, S. Kim, D. T. Pham, J. Jo, Z. Xiu, V. Mathew and J. Kim, Chem. Phys. Lett., 2016, 650, 64–68 CrossRef CAS.
  63. O. Zhanadilov, H. J. Kim, A. Konarov, J. Jeong, J.-H. Park, K. Y. Chung, Z. Bakenov, H. Yashiro and S.-T. Myung, Energy Storage Mater., 2024, 67, 103283 CrossRef.
  64. H. Ding, Y. He, X. Yu, L. Chen, M. Chen, Y. Luo, J. Li and S. Wei, J. Electroanal. Chem., 2025, 986, 119101 CrossRef CAS.
  65. W. Kao-ian, P. Tangthuam, P. Kidkhunthod, W. Limphirat, J. Padchasri, N. Aubert, G. Ciatto, I. In, K. C. W. Wu and S. Kheawhom, Small Methods, 2025, 9, e00871 Search PubMed.
  66. R. Jin, Y. Fang, B. Gao, Y. Wan, Y. Zhou, G. Rui, W. Sun, P. Qiu and W. Luo, Ind. Chem. Mater., 2025, 3, 87–96 RSC.
  67. A. Zhang, T. Chen, R. Zhao, Y. Wang, J. Yang, X. Han, X. Wang, C. Wu and Y. Bai, Angew. Chem., Int. Ed., 2025, 64, e202423824 CrossRef CAS PubMed.
  68. L. Wu, Z. Li, Y. Xiang, W. Dong, H. Wu, Y. Xu, Z. Ling, M. S. Chae, D. Sharon, N. Shpigel and X. Zhang, ACS Energy Lett., 2024, 9, 5801–5809 CrossRef CAS.
  69. J. Liang, Y. Zhao, L. Ren, M. Li, Q. Zhang, Y. Wang, X. Sun, M. Chuai, X. Wang and W. Liu, Adv. Funct. Mater., 2025, 35, 202501135 Search PubMed.
  70. Y. Chen, C. Lin, X. Chen, Z. Lu, K. Zhang, Y. Liu, J. Wang, G. Han and G. Xu, Adv. Energy Mater., 2024, 14, 202304303 Search PubMed.
  71. Y. Zhao, S. Zhang, Y. Zhang, J. Liang, L. Ren, H. J. Fan, W. Liu and X. Sun, Energy Environ. Sci., 2024, 17, 1279–1290 RSC.
  72. H. Jia, Y. Li, U. Ali, B. Liu, Z. Jin, L. Li, Y. Chen, L. Zhang, T. Wang and C. Wang, Nano Energy, 2024, 122, 109348 CrossRef CAS.
  73. Y. Huang, Y. Peng, Q. Ouyang, Q. Feng, H. Wang, D. Zheng, F. Wang, X. Lu and Q. Liu, Energy Storage Mater., 2024, 70, 103476 CrossRef.
  74. J. Yang, X. Li, S. Wang, R. Liu, F. Zhang, G. Wang, J. Wang, W. Ren, J. Wu, K. Ji, Y. Ji, Z. Chen, B. J. Ni, Z. Yang, N. Wu and Y. M. Yan, Adv. Funct. Mater., 2025, 36, e13512 CrossRef.
  75. H. Yang, Y. Wan, K. Sun, M. Zhang, C. Wang, Z. He, Q. Li, N. Wang, Y. Zhang, H. Hu and M. Wu, Adv. Funct. Mater., 2023, 33, 2215076 CrossRef CAS.
  76. Y. Fan, M. Xu, Q. Li, M. Liu, X. Zhang, P. Chu, B. Zhang, H. Zhou, Y. Zhao and C. Liu, Small, 2025, 21, 202501454 Search PubMed.
  77. W. Lv, Z. Shen, X. Li, J. Meng, W. Yang, F. Ding, X. Ju, F. Ye, Y. Li, X. Lyu, M. Wang, Y. Tian and C. Xu, Nano-Micro Lett., 2024, 16, 109 CrossRef CAS.
  78. S. Jia, L. Li, Y. Shi, C. Wang, M. Cao, Y. Ji and D. Zhang, Nanoscale, 2024, 16, 1539–1576 RSC.
  79. J. Chacón-Borrero, X. Chang, Z. Min, J. Yu, G. Montaña-Mora, K. V. Mejia-Centeno, Y. Sun, X. Zhou, S. Tunmee, P. Kidkhunthod, J. Li, J. Llorca, J. Arbiol and A. Cabot, Energy Storage Mater., 2025, 81, 104486 CrossRef.
  80. Y. Pan, S. Zuo, G. Ai, J. Wei, X. Zhao and W. Mao, Small Methods, 2024, 9, 202401626 Search PubMed.
  81. X. Chen, Z. Xu, B. Sun, Q. Li, Q. Meng, F. Wei, J. Qi, Y. Sui and P. Cao, J. Alloys Compd., 2025, 1020, 179484 CrossRef CAS.
  82. Y. Liu, P. Shi, Y. Li, Y. Yang, J. Yao, J. Li, Z. Tao, Y. Gan, X. Liu, Z. Wu, C. Xia, J. Zheng, L. Lv, L. Tao, J. Zhang, H. Wang, H. Wan and H. Wang, J. Energy Storage, 2024, 96, 112730 CrossRef CAS.
  83. S. Deng, B. Xu, X. Liu, Y. Yang, Y. Xiao, S. Wang, J. Zhao and T. Chen, Adv. Funct. Mater., 2024, 35, 202413711 Search PubMed.
  84. Y. Chen, L. Miao, Z. Song, H. Duan, Y. Lv, L. Gan and M. Liu, Adv. Funct. Mater., 2024, 34, 2409428 CrossRef CAS.
  85. T. Li, R. Guo, Y. Li, L. Meng, X. Sun, F. Li, X. Zhao, Z. Xu, J. Peng and L. An, J. Energy Chem., 2023, 83, 106–118 CrossRef CAS.
  86. R. Qin, S. Ding, C. Hou, L. Liu, Y. Wang, W. Zhao, L. Yao, Y. Shao, R. Zou, Q. Zhao, S. Li and F. Pan, Adv. Energy Mater., 2023, 13, 202203915 Search PubMed.
  87. Z. Shen, Y. Zhu, M. Zhang, T. Zhang, Z. Zhai, Y. Liu, L. Wang, Y. Wang, L. Li, G. Hong and N. Zhang, ACS Energy Lett., 2025, 10, 4491–4510 CrossRef CAS.
  88. X. Zeng, Z. Gong, C. Wang, P. J. Cullen and Z. Pei, Adv. Energy Mater., 2024, 14, 2401704 CrossRef CAS.
  89. Y. Liu, C. Lu, Y. Yang, W. Chen, F. Ye, H. Dong, Y. Wu, R. Ma and L. Hu, Adv. Mater., 2024, 36, 202312982 Search PubMed.
  90. J. Luo, M. Cao, N. Naresh, J. Borah, S. Li, T. Wang, B. K. Sarma, J. Yao, I. P. Parkin and B. D. Boruah, Adv. Funct. Mater., 2024, 35, 202417607 Search PubMed.
  91. J. Zhou, L. Shan, Z. Wu, X. Guo, G. Fang and S. Liang, Chem. Commun., 2018, 54, 4457–4460 Search PubMed.
  92. R. Sun, D. Luo, H. Zhou, Z. Zhang, Y. Gao, S. Ma, Z. Li and X. Kang, J. Energy Chem., 2025, 103, 703–713 Search PubMed.
  93. S. Deshmukh, J. V. Vaghasiya, J. Michalička, R. Langer, M. Otyepka and M. Pumera, Small, 2024, 21, 202409987 Search PubMed.
  94. Y. Zhang, Z. Li, B. Zhao, D. Xu, Z. Guo, J. Zhang and C. Gong, ACS Sustain. Chem. Eng., 2025, 13, 2553–2563 CrossRef CAS.
  95. Y. Wang, Y. Fan, X. Chen, J. H. Liu, Y. Gao, X. Lin, Y. Huang, H. Jiang, C. Zhan, H. Zhang, X. Cao and Y. Xiao, InfoMat, 2025, e70055 Search PubMed.
  96. R. Sinha, X. Xie, Y. Yang, Y. Li, Y. Xue, P. Wang and Z. Li, Adv. Energy Mater., 2025, 15, 2404815 CrossRef CAS.
  97. B. Nie, S. Yu, K. Lu, H. Zhang, C. C. Yang and Q. Jiang, Nano Lett., 2025, 25, 10935–10943 CrossRef CAS.
  98. K. Guo, Z. Song, Y. Lv, L. Gan and M. Liu, Adv. Funct. Mater., 2025, 35, 202506036 Search PubMed.
  99. M. Zhu, R. Gao, Q. Ran, S. g. Gong, Q. Li, S. P. Zeng, H. Huang, L. Hu, D. Yang, T. Dai, Y. Wang, D. Chao, M. Feng and Z. Chen, Angew. Chem., Int. Ed., 2025, 64, e202425080 CrossRef CAS.
  100. M. Yang, Y. Lin, P. Chen, M. Lai, J. Zhu, G. Li, M. Chen, Y. Wang, M. Chuai, J. Chen, G. Chai, H. Mi, L. Sun, C. He, D. Ma and P. Zhang, Angew. Chem., Int. Ed., 2025, 64, e202510907 CrossRef CAS PubMed.
  101. D. Zhang, J. Cao, C. Yang, K. Lolupiman, W. Limphirat, X. Wu, X. Zhang, J. Qin and Y. Huang, Adv. Energy Mater., 2024, 15, 2404026 CrossRef.
  102. Y. Liu, X. Wang, Z. S. Wu, Y. R. Cho and X. Wu, Adv. Funct. Mater., 2025, 35, 202505535 Search PubMed.
  103. P. Hu, T. Zhu, X. Wang, X. Wei, M. Yan, J. Li, W. Luo, W. Yang, W. Zhang, L. Zhou, Z. Zhou and L. Mai, Nano Lett., 2018, 18, 1758–1763 CrossRef CAS.
  104. P. Zhang, Y. Gong, S. Fan, Z. Luo, J. Hu, C. Peng, Q. Zhang, Y. Li and X. Ren, Adv. Energy Mater., 2024, 14, 2401493 CrossRef CAS.
  105. J. Xu, M. Galib, Z. Wu, L. Tao, Y. Shao, Y. Zhang, X. Guo, E. J. Hansen, Y. Chen, Z. Wang, C. Liu, M. Ponga and J. Liu, Nano Energy, 2024, 132, 110373 CrossRef.
  106. J. Liu, Z. Shen and C.-Z. Lu, J. Mater. Chem. A, 2024, 12, 2647–2672 RSC.
  107. H. Fu, X. Wang, L. Ye, Z. Wu, J. Yang, M. Shi and E. H. Ang, Chem. Eng. J., 2025, 506, 160308 CrossRef CAS.
  108. R. Trocoli and F. La Mantia, ChemSusChem, 2015, 8, 481–485 CrossRef CAS PubMed.
  109. Y. Zeng, J. Xu, Y. Wang, S. Li, D. Luan and X. W. Lou, Angew. Chem., Int. Ed., 2022, 61, e202212031 CrossRef CAS PubMed.
  110. W. A. Syed, A. K. Kakarla, H. Bandi, R. Shanthappa and J. S. Yu, J. Energy Storage, 2024, 99, 113325 CrossRef CAS.
  111. M. Zhang, W. Zhao, T. Yang, R. Gao, D. Luo, H. W. Park, Y. Hu and A. Yu, Adv. Energy Mater., 2024, 14, 202400543 Search PubMed.
  112. Y. Shi, B. Yang, G. Song, Z. Chen, M. Shakouri, W. Zhou, X. Zhang, G. Yuan and H. Pang, Angew. Chem., Int. Ed., 2024, 63, e202411579 CrossRef CAS.
  113. L. Wang, N. Liu, Q. Li, X. Wang, J. Liu, Y. Xu, Z. Luo, N. Zhang and F. Li, Angew. Chem., Int. Ed., 2024, 64, e202416392 CrossRef.
  114. L. Zhou, C. Wu, F. Yu, Y. Li, H. Liu, C. Zheng, F. Shen, A. Wen and B. Wang, ACS Appl. Mater. Interfaces, 2024, 16, 47454–47463 CrossRef CAS PubMed.
  115. M. Gu, A. M. Rao, J. Zhou and B. Lu, Chem. Sci., 2024, 15, 2323–2350 RSC.
  116. M. Hariram, P. K. Pal, A. S. Chandran, M. R. Nair, M. Kumar, M. K. Ganesha, A. K. Singh, B. Dasgupta, S. Goel, T. Roy, P. W. Menezes and D. Sarkar, Small, 2025, 21, 202410408 CrossRef.
  117. X. Wen, Y. Zhong, S. Chen, Z. Yang, P. Dong, Y. Wang, L. Zhang, Z. Wang, Y. Jiang, G. Zhou, J. Liu and J. Gao, Adv. Sci., 2024, 11, 202309555 Search PubMed.
  118. H. Liang, Z. Cao, F. Ming, W. Zhang, D. H. Anjum, Y. Cui, L. Cavallo and H. N. Alshareef, Nano Lett., 2019, 19, 3199–3206 CrossRef CAS PubMed.
  119. Q. Liu, J. He, J. Xie, H. Zhang, H. Wu, G. Wang, X. Lu and Z. Yang, Nano Energy, 2024, 127, 109780 CrossRef CAS.
  120. D. Jia, Z. Shen, W. Zhou, Y. Lv, Z. Chen, H. Tan, W. Zhou, X. He and H. Liu, Chem. Eng. J., 2024, 500, 156945 CrossRef CAS.
  121. S. Li, X. Zhao, T. Wang, J. Wu, X. Xu, P. Li, X. Ji, H. Hou, X. Qu, L. Jiao and Y. Liu, Angew. Chem., Int. Ed., 2024, 63, e202320075 CrossRef CAS PubMed.
  122. J. Xu, Z. Dong, Y. Li, K.-J. Huang, K. Liu and C. Cao, Appl. Surf. Sci., 2023, 613, 156146 CrossRef CAS.
  123. Z. H. Sun, W. Zheng, R. Zheng, Z. Y. Gu, Y. Bao, Z. B. Liu, Z. B. Sun, L. Niu and X. L. Wu, Adv. Sci., 2025, 12, e2502745 CrossRef.
  124. Z. Yan, Q.-H. Yang and C. Yang, J. Mater. Chem. A, 2024, 12, 24746–24760 RSC.
  125. H. Zhao, L. Zhao, D. Yin, N. Gao, Y. Zhang, J. Feng, X. Chen, X. Liu, J. Wei, C. Fan, G. Gao, C. Xiao and S. Ding, Adv. Mater., 2025 DOI:10.1002/adma.202515759.
  126. Y. Wu, Y. Qian, C. Huang, Y. Zhang, Y. Yang, A. Hu, Q. Tang and X. Chen, Electrochim. Acta, 2023, 460, 142593 CrossRef CAS.
  127. M. Sun, L. Wei, J. Peng, G. Zhao, D. Yu and C. Chen, J. Colloid Interface Sci., 2025, 698, 138070 CrossRef CAS PubMed.
  128. Q. Zhang, H. Jiang, S. Liu, Q. Wang, J. Wang, Z. Zhou, K. Cai, Q. Lai and Q. Wang, J. Power Sources, 2024, 601, 234286 CrossRef CAS.
  129. S. Zeng, S. Chen, Z. Ao, X. Lin, L. Yan, C. Liu and Z. Lin, Small, 2025, 21, 2501695 CrossRef CAS PubMed.
  130. S. Chen, C. Peng, D. Zhu and C. Zhi, Adv. Mater., 2024, 36, 2409810 CrossRef CAS.
  131. L. Tang, C. Yuan, W. Lu and X. Li, Adv. Funct. Mater., 2025, 35, 2502455 CrossRef CAS.
  132. Y. Li, X. Guo, S. Wang, W. Sun, D. Yu, N. Li, H. Zhou, X. Zhang and H. Pang, Adv. Sci., 2025, 12, 2502563 CrossRef CAS PubMed.
  133. Y. Zhang, C. Wei, M.-X. Wu, Y. Wang, H. Jiang, G. Zhou, X. Tang and X. Liu, Chem. Eng. J., 2023, 451, 138915 CrossRef CAS.
  134. Y. Tulchinsky, C. H. Hendon, K. A. Lomachenko, E. Borfecchia, B. C. Melot, M. R. Hudson, J. D. Tarver, M. D. Korzyński, A. W. Stubbs, J. J. Kagan, C. Lamberti, C. M. Brown and M. Dincă, J. Am. Chem. Soc., 2017, 139, 5992–5997 CrossRef CAS PubMed.
  135. C. Dong, Y. Yu, C. Ma, C. Zhou, J. Wang, J. Gu, J. Ji, S. Yang, Z. Liu, X. Xu and L. Mai, Energy Environ. Sci., 2025, 18, 3014–3025 RSC.
  136. N. Chen, W. Wang, Y. Ma, M. Chuai, X. Zheng, M. Wang, Y. Xu, Y. Yuan, J. Sun, K. Li, Y. Meng, C. Shen and W. Chen, Small Methods, 2023, 8, 2201553 CrossRef.
  137. T. Hu, Y. Zhao, Y. Yang, H. Lv, R. Zhong, F. Ding, F. Mo, H. Hu, C. Zhi and G. Liang, Adv. Mater., 2024, 36, 2312246 CrossRef CAS.

This journal is © The Royal Society of Chemistry 2026
Click here to see how this site uses Cookies. View our privacy policy here.