The authors investigated the changes in local structures and magnetic property of the Li 1.2 Mn 0.4 Fe 0.4 O 2 positive electrode material for lithium-ion batteries during the first charge-discharge cycle. Although Li 1.2 Mn 0.4 Fe 0.4 O 2 has a composite structure of the layered and disordered cubic rocksalt before the electrochemical testing, nanometer-sized grains with spinel structures are formed during the extraction of Li ions up to Li 1.2−x Mn 0.4 Fe 0.4 O 2 ͑0 Յ x Յ 0.99͒. The spinel nanograins have weak spontaneous magnetization ͑ca. 0.3 G cm 3 /g͒, which is associated with the movements of Fe ions from the octahedral to the tetrahedral sites in both the layered and disordered rocksalt structures. The fraction of spinel nanograins decreased after the subsequent insertion of Li ions.Lithiated transition-metal ͑TM͒ oxides are widely studied as positive electrodes of lithium-ion batteries. 1 LiAO 2 ͑A = Co, Ni, Mn, and combinations thereof͒ with a layered rocksalt structure, comprising alternative stacking of Li and TM layers between cubic close-packed oxygen arrays, has been most intensively studied to seek high energy and high power positive electrode materials. 2-5 A charge-discharge cycle of the battery is performed by reversible extraction/insertion of Li ions in both the positive and negative electrode materials. In practice, however, irreversible phase transitions during charge-discharge cycles which cause fatal capacity loss are an essential problem. Previous studies on LiCoO 2 and LiMnO 2 found that structural transformations from the layered rocksalt structure to the spinel structures deteriorate the battery performance. [6][7][8][9][10][11][12] It is believed that spinel phases simply accumulate and grow within an original layered rocksalt phase during charge-discharge cycling.Recently, Li 2 MnO 3 -LiAO 2 ͑A = Cr, Fe, Co, Ni, and combinations thereof͒ systems attract substantial interests as positive electrode materials due to potential high capacities ͑Ͼ200 mAh/g͒ for near-future electric vehicles. 13-20 Although one of the origins of the high capacity is abundant Li contents in the nominal formula Li 1+x A 1−x Ј O 2 ͑x Ͼ 0͒, charge-discharge mechanisms are not fully understood and an urgent issue to be addressed. A Li 2 MnO 3 -LiFeO 2 system is an attractive material because it contains cheap constituent TM elements and acts as a 3 V positive electrode, which is comparable to a Li 2 MnO 3 -LiCrO 2 system 13,14 in spite of the inactive bulk LiFeO 2 . Tabuchi et al. reported that ͑1 − x͒Li 2 MnO 3 -xLiFeO 2 shows high specific capacities for x between 0.3 and 0.5. 15 Typical charge-discharge voltage profiles of a Li 1.2 Mn 0.4 Fe 0.4 O 2 ͑calcinated at 850°C in air͒/Li cell 15 are shown in Fig. 1a. The first charge profile exhibits a specific high capacity of ca. 300 mAh/g although the large capacity fading occurs during the first cycle. After the 10th cycle, the charge-discharge profiles are basically reversible. Thus understanding the first charge-discharge mechanisms is most important for impr...