“…More significantly, when the current density reaches a maximum value of 2.0 A g −1 , the corresponding capacity still maintains approximately 454 mAh g −1 , exhibiting fast reaction kinetics and excellent reversibility of the ZMO‐NRs. Notably, the achieved reversible capacities are superior to those of reported Mn‐based anodes for LIBs (Table S1, Supporting Information), especially at a much higher rate, such as bare MnO x (≈180 mAh g −1 at 2 A g −1 ), graphene oxide/Mn 3 O 4 (≈174 mAh g −1 at 1 A g −1 ), ZnMnO 3 NT arrays (≈364 mAh g −1 at 2 A g −1 ), porous ZnMn 2 O 4 rugby‐balls (≈200 mAh g −1 at 2 A g −1 ), ZnMn 2 O 4 nanoparticles (≈173 mAh g −1 at 1 A g −1 ), and hollow ZnMn 2 O 4 NTs (≈272 mAh g −1 at 2 A g −1 ), as comparatively collected in Figure c. Meanwhile, the high diffusion coefficients ( D ) of approximately 1.3×10 −9 and 5.2×10 −9 cm 2 s −1 for anodic and cathodic processes can also be obtained for the 1D ZMO‐NRs, respectively, on the basis of i p versus v 1/2 plots and using Equation , further revealing the fast Li + diffusion rate (Figure d, Figure S2, Supporting Information). …”