Intercalation‐based cathodes typically rely on the cationic redox activity of transition metals to deliver capacity, but, recently, anionic redox chemistry has emerged as a way to increase the energy density of rechargeable batteries. However, the irreversible structural disorder and voltage fading accompanying oxygen release are major problems preventing commercial use. To overcome these limitations, the connection between structural stability and anionic redox activity must be understood. Here, we present a review of theoretical and experimental progress in anionic redox in sodium intercalation cathodes. First, the effects of structural factors including stacking sequences and cationic vacancies on the reversible capacity originating from anionic redox are discussed. Second, the effects on anionic redox activity of cationic substitution with alkaline earth metals (Li or Na) and the coordination environment are highlighted. Third, the progress and challenges facing materials based on 3d/4d/5d metals are reviewed. Finally, research directions for the development of anionic redox active materials are outlined.
A new paradigm based on an anionic O 2− /O n− redox reaction has been highlighted in high-energy density cathode materials for sodium-ion batteries, achieving a high voltage (∼4.2 V vs Na/Na + ) with a large anionic capacity during the first charge process. The structural variations during (de)intercalation are closely correlated with stable cyclability. To determine the rational range of the anion-based redox reaction, the structural origins of Na 1−x Ru 0.5 O 1.5 (0 ≤ x ≤ 1.0) were deduced from its vacancy (□)/Na atomic configurations, which trigger different interactions between the cations and anions. In the cation-based Ru 4+ /Ru 5+ redox reaction, the □ solubility into fully sodiated Na 2 RuO 3 predominantly depends on the crystallographic 4h site when 0.0 ≤ x ≤ 0.25, and the electrostatic repulsion of the linear O 2− −□− O 2− configuration is accompanied by the increased volumetric strain. Further Na extraction (0.25 ≤ x ≤ 0.5) induces a compensation effect, leading to Na 2/3 [Na □ Ru 2/3 ]O 2 with the □ formation of 2b and 2c sites, which drastically reduce the volumetric strain. In the O 2− /O n− anionic redox region (0.5 ≤ x ≤ 0.75), Na removal at the 4h site generates a repulsive force in O 2− −□−O 2− that increases the interlayer distance. Finally, in the 0.75 ≤ x ≤ 1.0 region, the anionic O charges are unprotected by repulsive forces, and their consumption causes severe volumetric strain in Na 1−x Ru 0.5 O 1.5 . Coupling our mechanistic understanding of the structural origin with the □and Na-site preferences and the electrostatic interaction between lattice O and vacancies in Na 1−x Ru 0.5 O 1.5 , we determined the rational range of the anionic redox reaction in layered cathode materials for rechargeable battery research.
Unlike cathodes for lithium-ion batteries, oxygen redox (OR) processes at a high voltage (�4.2 V) during the first charge in sodium-ion batteries (SIBs) employ some Li-incorporated Mn oxides that is recovered during subsequent discharge. To determine the intrinsic origin, P2-type Na 0.6 [Li 0.2 Mn 0.8 ]O 2 exhibiting a reversible OR-induced two-phase reaction was investigated using experiments and first-principle calculations. First, operando X-ray diffraction results in reversible P2-Z phase transformations and thermodynamic analysis show the twophase reaction features Li migration into the tetrahedral sites from the transition-metal layer in the latter phase. Second, Liinduced decoupling of the oxygen 2p-electron led to selective anion redox activity depending on the oxygen sites that are Li-rich (redox-active) and Mn-rich (redox-inactive) environments. Third, redox-active oxygen coordinated to the Li vacancy predominantly participates in the formation of peroxo-like dimers with distortion of the MnO 6 octahedron, as observed in the reversible extended X-ray absorption fine structure spectra during the OR reaction. Considering three physicochemical perspectives, we reveal that Li ions play a role in activating OR reactions and control OR participation in the charge-compensation process. Our findings suggest that the Li/Mn ratio is a critical factor for achieving a reversible OR reaction, and broaden the possibilities of exploiting OR to reach high-energy densities in next-generation SIBs.
An intriguing redox chemistry via oxygen has emerged to achieve high-energy-density cathodes and has been intensively studied for practical use of anion-utilization oxides in A-ion batteries (A: Li or Na). However, in general, the oxygen redox disappears in the subsequent discharge with a large voltage hysteresis after the first charge process for A-excess layered oxides exhibiting anion redox. Unlike these hysteretic oxygen redox cathodes, the two Na-excess oxide models Na2IrO3 and Na2RuO3 unambiguously exhibit nonhysteretic oxygen capacities during the first cycle, with honeycomb-ordered superstructures. In this regard, the reaction mechanism in the two cathode models is elucidated to determine the origin of nonhysteretic oxygen capacities using first-principles calculations. First, the vacancy formation energies show that the thermodynamic instability in Na2IrO3 increases at a lower rate than that in Na2RuO3 upon charging. Second, considering that the strains of Ir–O and Ru–O bonding lengths are softened after the single-cation redox of Ru4+/Ru5+ and Ir4+/Ir5+, the contribution in the oxygen redox from x = 0.5 to 0.75 is larger in Na1–x Ru0.5O1.5 than that in Na1–x Ir0.5O1.5. Third, the charge variations indicate a dominant cation redox activity via Ir(5d)–O(2p) for x above 0.5 in Na1–x Ir0.5O1.5. Its redox participation occurred with the oxygen redox, opposite to the behavior in Na1–x Ru0.5O1.5. These three considerations imply that the chemical weakness of Ir(5d)–O(2p) leads to a more redox-active environment of Ir ions and reduces the oxygen redox activity, which triggers the nonhysteretic oxygen capacity during (de)intercalation. This provides a comprehensive guideline for design of reversible oxygen redox capacities in oxide cathodes for advanced A-ion batteries.
Unlike in lithium-ion batteries (LIBs), in sodiumion batteries (SIBs), nonhysteretic oxygen redox (OR) reactions are observed in Li-excess Na-layered oxides. This necessitates an understanding of the reaction mechanism of an O3-type Li-excess Mn oxide, Na[Li 1/3 Mn 2/3 ]O 2 , a novel OR material designed for advanced SIBs. It could establish the role of Li in triggering nonhysteretic oxygen capacities during (de)sodiation. Three biphasic mechanisms were compared using first-principles calculations under the desodiation modes: (i) Na/vacancy ordering, (ii) Li migration in the NaO 2 layer, and (iii) in-plane Mn migration. The migrated Li ions generated a "physicochemical screen" effect upon electrochemical OR reactions in the oxide cathode. Thermodynamic formation energies showed different biphasic pathways upon charging in Na 1−x [Li 2/6 Mn 4/6 ]O 2 (NLMO) under the three modes. O−O bond population indicated that biphasic-reaction paths -i and -iii were derived from generating inter/ intralayer O−O dimers, and path-iii was triggered by the formation of a Mn−O 2 −Mn moiety. However, Li migration exhibited an ideal OR process (O 2− /O n− ) without forming anionic dimers. The electronic structures of Mn(3d) and O(2p) revealed that Li migration pushed lattice-based O(2p)-hole states to a high energy level, resulting in the chemical suppression of O 2 molecule formation. Selectively decoupled oxygen ordering indicated that the oxygen species coordinated with two Mn (O Mn2 ) derived from Li migration played an important role in nonhysteretic oxygen capacities during cycling. From these findings, we propose the "physicochemical screen" concept that physically suppresses interlayer O−O dimers and chemically hinders discretized O(2p)− O(2p) states formed by molecular O 2 . This could significantly impact the role of Li ions in Li-excess OR-layered oxides for SIBs.
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