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Cui et al. Energy Mater 2023;3:300023  https://dx.doi.org/10.20517/energymater.2022.90  Page 5 of 12

               increasing the contact area between ZVNW and CC, which enhanced the structural stability of the ZVNW-
                                                                                   2+
               CC electrode. And 1D nanostructure can shorten the diffusion pathway of Zn  during the charging and
               discharging process, promoting the electrochemical performance of the ZVNW-CC electrode. SEM images
               in Figure 2F and G show a higher-resolution view of the sample. ZVNW, ranging in size from 20-200 nm,
               was stacked and interlaced grown on CC, forming a multi-void network structure.

               The microstructure of ZVNW, peeled from CC through prolonged sonication, was further characterized by
               TEM. Figure 3A shows a TEM image of a single ZVO nanowire. The surface of the ZVNW was rough,
               which increased the contact area between the electrode and electrolyte. Figure 3B is its HRTEM image. The
               inter-planar distances of 2.01 and 2.31 Å were attributed to (210) and (112) planes of ZVO, respectively.
               Figure 3C shows the fast Fourier transform electron diffraction (FFT-ED) pattern of the HRTEM image,
               which suggests the single-crystal feature. Figure 3D shows the EDS analysis of a single ZVO nanowire. It
               was further confirmed that the ZVNW were composed of Zn, V, and O elements, which were uniformly
               distributed in the ZVNW.


               Electrochemical performances
               The electrochemical properties of ZVNW and ZVNW-CC electrodes were evaluated by CV and GCD.
               Figure 4A shows the CV curves of these two electrodes at 0.1 mV s . The surrounding CV curve area of the
                                                                        -1
               ZVNW-CC electrode was much larger than that of the ZVNW electrode, indicating that the ZVNW-CC
               electrode exhibited higher specific capacity. Figure 4B presents the first three cycles of the CV plot for the
                                                       -1
                                                                                             2+
               ZVNW-CC electrode at a scan rate of 0.1 mV s  in the voltage range of 0.2-1.6 V (vs. Zn/Zn ). Three pairs
               of redox peaks were observed at 0.56/0.76, 0.85/1.07, and 1.35/1.46 V, which were attributed to the three-
                                                                                    [21]
                                2+
               step reaction of Zn  insertion and extraction into the ZVO lattice structure . Among the reduction
               reactions at 0.56, 0.85, and 1.35 V showed that the vanadium element in ZVNW-CC was gradually reduced
               from +5 valence to +α (α < 5), and the oxidation reactions at 0.76, 1.07, and 1.46 V corresponded to the
               gradual oxidation of V  to V . The cyclic scanning process of the first three loops almost overlapped,
                                   α+
                                         5+
               indicating that the storage process of Zn  was highly reversible. GCD tests were conducted between 0.2 and
                                                 2+
                             2+
               1.6 V (vs. Zn/Zn ). Figure 4C and D indicates the GCD profiles of ZVNW-CC and ZVNW electrodes for
               the first five and 50th cycles at 50 mA g . In the discharge curve, there were two distinctive potential
                                                   -1
               plateaus within the range of 0.69-1.00 and 0.45-0.69 V, which corresponded to the two main oxidation peaks
               of CV. Similarly, another two potential plateaus in the charge curve within 0.88-1.15 and 0.6-0.88 V
               corresponded to the reduction peaks. The related charge-discharge curve of ZVNW-CC electrodes at
                      -1
               50 mA g  exhibited a smaller overpotential (∆V(Q/2)) than that of the ZVNW electrode (0.26 vs. 0.34 V,
               Figure 4C and D). In sharp contrast, the specific capacity of the ZVNW-CC electrode was larger than that of
               the ZVNW electrode, benefitting from the synergistic effects of morphology regulation and a self-
               supporting electrode.


               The rate performances are presented in Figure 5A, where the current density increases from 50 to
               1,000 mA g  and then returns to 50 mA g . The ZVNW-CC cathode displayed specific capacities of 361.8,
                                                   -1
                         -1
               328.2, 292.8, 251.1, and 207.6 mAh g  at 50, 100, 200, 500, and 800 mA g , respectively. Even at
                                                                                     -1
                                                  -1
               1,000 mA g , the ZVNW-CC cathode can still deliver a reversible capacity of 145.9 mAh g . And returning
                                                                                            -1
                         -1
                                                         -1
                         -1
               to 50 mA g , the specific capacity of 346.9 mAh g  and the capacity recovery of 95.8% can still be obtained.
               However, the capacities of the ZVNW electrode were evidently lower than those of ZVNW-CC at every
               corresponding current density. This indicated that the structural stability and electrochemical reversibility
               of the ZVNW-CC cathode were much superior to those of the ZVNW electrode. In order to assess the
               commercial potential of the ZVNW-CC electrode, long-cycle performance testing was necessary. The
               cycling performances of the ZVNW and ZVNW-CC electrodes were examined at current densities of 200,
               500, and 1,000 mA g , respectively, and were shown in Figure 5B-D. The discharge capacity of the ZVNW-
                                 -1
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