In order to address the role of aluminum dopant in spinel-structured lithium manganese oxide (Li 1.08 Mn 1.84 Al 0.08 O 3.96 , Al-doped LMO) electrode, high-temperature (60 • C) charge/discharge cycling and storage experiments are carried out. The Al-doped LMO outperforms the un-doped counterpart with respect to capacity fading and Mn dissolution. However, the electrode polarization becomes substantial for the Al-doped LMO after the high-temperature storage. As the resistive component to be responsible for the electrode polarization, Al 2 O 3 and Al(OH) x F 3-x are identified on the Al-doped LMO surface from X-ray photoelectron spectroscopy study. It is very likely that the doped Al ions dissolve into the electrolyte during the high-temperature storage but re-deposit as a form of Al 2 O 3 and Al(OH) x F 3-x on the LMO surface. Due to a scavenging action of these Al species for hydrogen fluoride, Mn dissolution is suppressed to give an improved cycle and storage performance at elevated temperature.Nowadays, lithium-ion batteries (LIBs) are the most popular power sources for portable electronic devices such as mobile phones, notebook computers and power tools. The application range of LIBs is being expanded gradually to plug-in hybrid electric vehicles (PHEVs) and electric vehicles (EVs). 1,2 The spinel-structured lithium manganese oxide (LiMn 2 O 4 , LMO hereafter) is one of the most popularly used positive electrode materials for the LIBs to power electric vehicles. The use of LMO is, however, not widespread because of its intrinsic shortcoming, which is the poor cycle and storage performance at high temperature, which is in turn resulted from the dissolution of manganese ions, local structural instability, and Jahn-Teller distortion. [3][4][5][6][7][8][9] The high-temperature performances of LMO electrodes have been improved by several countermeasures, one of which is the doping of metal ions (Mg, Al, Ni, Cr, Ga, and La) into the LMO lattice. 8,10-12 The roles of dopants have been identified as to prevent Jahn-Teller distortion by increasing the average Mn valence, 13-15 and to stabilize the spinel structure to suppress the formation of locally distorted structure. [16][17][18] Aluminum is the particularly preferred dopant for several reasons. Al 3+ ions easily replace the 16d site of spinel structure because ionic radius of Al 3+ (0.057 nm) is similar to that for Mn 3+ (0.066 nm). [19][20][21] The doped Al 3+ ions can improve the structural stability due to a strong bonding between Al 3+ and O 2− ions. 13,15,22,23 Furthermore, the Al-doped LMO exhibits smaller lattice change than that for un-doped one upon charge/discharge cycling, which minimizes the structural stress. 16 Due to these favorable roles of Al dopant, Al-doped LMO is now widely adopted in practical LIBs.This work finds another important role of Al dopant in LMO electrode, which is the suppression of Mn dissolution and capacity fading due to the beneficial action of Al species that are re-deposited after dissolution from the spinel lattice. To addr...