realization, to further postpone the foreseeable energy crisis in the near future. [1][2][3] Nevertheless, commercially growing demand for LIBs has triggered the cost surge coming from the limited raw materials. [4][5][6] In this regard, cost-effective sodium-ion batteries (SIBs) with bountiful supply and analogous "rocking chair" working mechanism with LIBs, [7][8][9] show promise in becoming one of the favorable alternatives to LIBs, and meet the practical demands of sustainable large-scale energy storage systems as well. [10,11] That is why, SIBs have been extensively studied and flourished over the past decade. However, the existing demerits of poor structural stability, sluggish ion diffusion kinetics, low operating voltage, and unsatisfactory energy/power density of cathode materials remain challenging for the practical application of SIBs. [12][13][14] Toward cathodic hosts for sodium-ion storage, the commonly available materials mainly include layered transition-metal oxides (TMOs) and polyanionic compounds (PACs). Layered transition-metal oxides, Na x /TM/O 2 (TM = Cr, Fe, Co, Mn, Ni, etc.), especially those with a P2 type structure, [15] exhibit better cycle stability and rate performance due to the higher sodium-ion diffusion kinetics, and have been extensively studied. [16] At present, through the use of element doping, substitution, and interface modification suppression, the reversibility of layered transition mental oxide Impossible voltage plateau regulation for the cathode materials with fixed active elemental center is a pressing issue hindering the development of Na-superionic-conductor (NASICON)-type Na 3 V 2 (PO 4 ) 2 F 3 (NVPF) cathodes in sodium-ion batteries (SIBs). Herein, a high-entropy substitution strategy, to alter the detailed crystal structure of NVPF without changing the central active V atom, is pioneeringly utilized, achieving simultaneous electronic conductivity enhancement and diffusion barrier reduction for Na + , according to theoretical calculations. The as-prepared carbon-free highentropy Na 3 V 1.9 (Ca,Mg,Al,Cr,Mn) 0.1 (PO 4 ) 2 F 3 (HE-NVPF) cathode can deliver higher mean voltage of 3.81 V and more advantageous energy density up to 445.5 Wh kg −1 , which is attributed by the diverse transition-metal elemental substitution in high-entropy crystalline. More importantly, high-entropy introduction can help realize disordered rearrangement of Na + at Na(2) active sites, thereby to refrain from unfavorable discharging behaviors at low-voltage region, further lifting up the mean working voltage to realize a full Na-ion storage at the high voltage plateau. Coupling with a hard carbon (HC) anode, HE-NVPF//HC SIB full cells can deliver high specific energy density of 326.8 Wh kg −1 at 5 C with the power density of 2178.9 W kg −1 . This route means the unlikely potential regulation in NASICON-type crystal with unchangeable active center becomes possible, inspiring new ideas on elevating the mean working voltage for SIB cathodes.