concerning active source leakage and shuttle effect should be addressed, as they result in a lack of carrier and backward loading processes. The insulating nature of elemental I 2 causes it to rely on conductive supporters (mostly porous carbon) to transport electrons and redox. However, the carbon materials currently confine I 2 solely by physical means including adsorption and impregnation, resulting in uneven loading and sluggish interactions, especially considering its electrical neutrality and large radius. [12,13] Another noticeable issue concerns the generation of polyiodides and the associated shuttle effect, which can lead to undesirable selfdischarge problems. [4] MXenes are represented with a general formula of M n+1 X n T x , where M represents the transition metal (Ti, Nb, Zr, Cr, etc.), X stands for C or N, and T x is the surficial termination. They are meant to be a more ideal new carrier for I 2 , due to their exceptional electrical conductivity, abundant surface terminations (O, F, OH, etc.), periodic layered microstructure, and arrayed interlayer gap. [14-21] Furthermore, the efficient electron transport of the MXene skeleton is believed to rescue the insulating active materials to achieve ultrafast reaction kinetics. Meanwhile, the nanoscale interlayer galleries potentially confine the reaction products to suppress the common shuttle behavior. [22-29] Besides, the ceramic nature of MXenes is capable of buffering the inevitable volume change, hence escorting the composite Weak binding and affinity between the conductive support and iodine species leads to inadequate electron transfer and the shuttle effect. Herein, redox kinetics and duration are significantly boosted by introducing a Nb 2 CT X host that is classified as a layered 2D Nb-based MXene. With a facile electrodeposition strategy, initial I − ions are electrically driven to insert in the nanosized interlayers and are electro-oxidized in situ. Linear I 2 is firmly confined inside and benefits from the rapid charge supply from the MXene. Consequently, an aqueous Zn battery based on a Zn metal anode and ZnSO 4 electrolyte delivers an ultraflat plateau at 1.3 V, which contributes to 84.5% of the capacity and 89.1% of the energy density. Record rate capability (143 mAh g −1 at 18 A g −1) and lifespan (23 000) cycles are achieved, which are far superior to those of all reported aqueous MXenes and I 2-metal batteries. Moreover, the low voltage decay rate of 5.6 mV h −1 indicates its superior anti-self-discharge properties. Physicochemical analyses and density functional theory calculations elucidate that the localized electron transfer and trapping effect of the Nb 2 CT X MXene host are responsible for enhanced kinetics and suppressed shuttle behavior. This work can be extended to the fabrication of other I 2-metal batteries with long-lifetime expectations. Aqueous halide iodine batteries, which transport electrons through the direct conversion reaction between an I 2 element and I − ions, are increasingly getting noticed for their cost-ef...