Sodium‐deficient nickel–manganese oxides exhibit a layered structure, which is flexible enough to acquire different layer stacking. The effect of layer stacking on the intercalation properties of P 3‐Na x Ni 0.5 Mn 0.5 O 2 ( x =0.50, 0.67) and P 2‐Na 2/3 Ni 1/3 Mn 2/3 O 2 , for use as cathodes in sodium‐ and lithium‐ion batteries, is examined. For P 3‐Na 0.67 Ni 0.5 Mn 0.5 O 2 , a large trigonal superstructure with 2√3 a ×2√3 a ×2 c is observed, whereas for P 2‐Na 2/3 Ni 1/3 Mn 2/3 O 2 there is a superstructure with reduced lattice parameters. In sodium cells, P 3 and P 2 phases intercalate sodium reversibly at a well‐expressed voltage plateau. Preservation of the P 3‐type structure during sodium intercalation determines improving cycling stability of the P 3 phase within an extended potential range, in comparison with that for the P 2 phase, for which a P 2– O 2 phase transformation has been found. Between 2.0 and 4.0 V, P 3 and P 2 phases display an excellent rate capability. In lithium cells, the P 3 phase intercalates lithium, accompanied by a P 3– O 3 structural transformation. The in situ generated O 3 phase, containing lithium and sodium simultaneously, determines the specific voltage profile of P 3‐Na x Ni 0.5 Mn 0.5 O 2 . The P 2 phase does not display any reversible lithium intercalation. The P 3 phase demonstrates a higher capacity at lower rates in lithium cells, whereas in sodium cells P 3‐Na x Ni 0.5 Mn 0.5 O 2 operates better at higher rates. These findings reveal the unique ability of sodium‐deficient nickel–manganese oxides with a P 3‐type structure for application as low‐cost electrode materials in both sodium‐ and lithium‐ion batteries.
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Kalapsazova et al. (2015) studied this question.
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