have been considered as an alternative to lithium-ion batteries (LIBs) for largescale applications like smart grid energy storage. [1][2][3][4][5][6] Significant progress has been made in developing cathode materials for high-performance SIBs, such as layered transition metal oxides (Na x MeO 2 , Me = 3d transition metals), [7] polyanionic compounds, [8] and miscellaneous Na insertion materials. [9] The progress of designing efficient anode materials, however, has been relatively slow and finding proper ones is exigent because the commercial graphite anode for LIBs cannot be used to host the Na + ions whose diameter is ≈34% larger than Li + ions in the commonly used carbonate-based electrolytes. [10][11][12][13] Further, graphite has negligible capacities of 30-35 mA h g −1 in SIBs. [14,15] Although Si has been considered the most promising anode for LIBs, it holds very limited Na storage capacities at ambient temperature due to the unfavorable kinetics. [16][17][18] In view of the abovementioned reasons, it is crucial to identify anode materials that possess high capacities and long cyclic stability in SIBs. Benefiting from the high theoretical capacity of 2596 mA h g −1[19-23] by forming a highly reactive Na 3 P phase [24] and a safe working potential of ≈0.45 V versus Na/Na + , [25] phosphorus (P) has been considered a promising anode candidate for SIBs among many proposed materials. [26,27] Red P presents better chemical stability at room temperature and is commercially available at lower cost than other phosphorus allotropes, like white P, black P, [28] and violet P. [29] Nevertheless, most electrodes made from red P suffered low rate capacities, severe capacity reduction, and poor electrochemical reversibility, [19,21,30] which hindered the wide application of red P-based anodes. The following unfavorable reaction mechanisms are responsible for the poor electrochemical performance. (i) The extremely large volume expansion over 300% occurring when red P is transformed to Na 3 P phase causes pulverization of the active material and separation of red P from the current collectors, leading to rapid capacity deterioration. [23,[31][32][33] (ii) The electrically insulating amorphous red P whose electrical conductivity is ≈10 −14 S cm −1 results in large polarization and poor utilization of active material, [20,21,23,25,34] limiting the high-rate performance. (iii) The unstable, electronically insulating solid electrolyte This paper reports the rational assembly of novel hollow porous carbon nanospheres (HPCNSs) as the hosts of phosphorous (P) active materials for high-performance sodium-ion batteries (SIBs). The vaporization-condensation process is employed to synthesize P/C composites, which is elucidated by both theories and experiments to achieve optimized designs. The combined molecular dynamics simulations and density functional theory calculations indicate that the morphologies of polymeric P 4 and the P loading in the P/C composites depend mainly on the pore size and surface condition of carbon supports. M...