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Page 26 of 64          Rehman et al. Energy Mater 2024;4:400068  https://dx.doi.org/10.20517/energymater.2024.06

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               100 mA g  while sustaining 65.6% of the capacity over 5,000 cycles at an ampere density of 2 A g . During
               (dis)charging, the strong interaction between rGO and NRP/Na P inhibited volume variations.
                                                                     3
               To better protect the RP-C composites from air exposure and the resultant capacity engulfing process, a
               protective coating of polypyrrole (PPy) has been proposed, which could enhance the conductivity and
               impart electrolyte and air stabilization . This strategy resulted in stable electrode material at ambient
                                                 [155]
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               conditions having a high RP content with a stable reversible capacity of 800 mAh g  at a current density of
               50 mA g . Jin et al. have adopted an assisted double annealing strategy to ensure highly porous conductive
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               networks interconnected inside the P host . The extra-short Na /e  diffusion pathways in the conductive
                                                   [156]
                                                                       +
               matrix supported the structure from volume variations and exhibited an astonishing longevity over 2,000
               cycles with 1,027 mAh g  of steady capacity at 4 A g  and an equally competitive rate behavior.
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               An SIB anode with a distinguished performance and real-time performance-mechanistic evaluation has
               been reported by Liu et al. . In-situ TEM and simulations detected “liquid-like” properties, metallic
                                       [157]
               character, and structural endurance in the RP CNF composite. The highly encapsulated RP inside the C
               matrix, akin to a core-shell structure, mitigated side reactions. This observation of liquidity of RP on
               sodiation was dually verified using time-lapse scanning TEM (STEM) images. The optimized capacity of
               1,019 mAh g  over 5,000 cycles at 1 A g  was a benchmark. Details are shown in Figure 12.
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               MXene-supported uniform-sized RP nanoparticles were additionally integrated with multi-walled CNTs
               (MWCNTs), leading to outstanding stability and improved mobility of Na /e  transportation . The hybrid
                                                                                -
                                                                              +
                                                                                             [158]
               showed a capacity of 371.6 mAh g  at 0.2 A g  over 100 cycles. A facile methodology for high-capacity SIB
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               anodes with high mass loadings has been reported by Zhu et al. . A composite of wood-derived carbon
                                                                      [159]
               and CNTs was coupled to RP. Multi-channeled ion and electronic pathways with a compact but porous
               framework synchronously improved the capacity retention ability at high mass loadings. Although optimal
               redox kinetics at a lower mass loading (8.2 mg cm ) was achieved even at a high mass loading of
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               ~14 mg cm , capacity preservation of 53.9% was attained. A superior gravimetric capability of 468.8 mAh g
                         -2
               and real rate capacity of 1.63 mAh g  at 106.6 mAcm  were captured. A liquid exfoliation strategy for
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               amorphous RP nanoplates synthesis and their composite with CNTs has been proposed recently by
               Kaur et al. . A superior air stability was achieved with low oxidative degradation that enabled the
                        [160]
               composite to attain higher capacities above 2,000 mAh g  over 1,000 cycles. Other composite hybrids and
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               phosphorous alloys have been extensively explored as SIB alloying anodes with many recent detailed
               reviews [161-164] . Zhang et al. have reported a composite SIB anode (Sb/P@C) that could deliver a capacity of
                                                                                                     [165]
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               350 mAh g  at 500 mA g . At 50 mA g , a capacity of above 400 mAh g  was sustained over 100 cycles .
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               Germanium-based anodes for SIBs
               Germanium (Ge) has been highlighted for its strong alloying potential with Na  and less volume expansion
                                                                                  +
               than Sn and Sb conversion-alloying anodes. However, its theoretical capacity (369 mAh g ) is limited for
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               SIBs because 1 mol of Na  in the resulting NaGe formulation showed unfavored kinetics in the crystalline
                                     +
               Ge, which rendered it below the limelight of energy storage community. Although it has 1,000 times
               superior electrical conduction than Si, the crystalline Ge has a very minor affinity for Na  that can only
                                                                                             +
                                          -1
               provide a capacity of 20 mAh g . Thus, many derivatives, especially those with amorphous Ge, have been
               proposed both theoretically and experimentally, whereby a theoretical capacity of 576 mAh  g
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               (corresponding to Na Ge) has been achieved in the amorphous phase [45,166,167] . Lu et al. have presented
                                  1.56
               detailed in-situ TEM-supported evidence of (de)sodiation changes in amorphous Ge nanowires . The
                                                                                                    [45]
               unique appearance of pores in the desodiated state and their reappearance upon sodiation in the Ge
               nanowires were due to sodiation-induced defects during in-situ HRTEM. The large volume expansion of
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