A high specific energy has generated widespread scientific and technical interest in Li-ion cells for secondary batteries. This high specific energy density is derived from the high cell voltage, typically 4 V (vs. 1.3 V for a typical Ni-MH secondary battery). The Li densities in the cathode and anode materials are modest, however, and it is hoped that higher capacities of these electrodes will lead to further increases in the specific energies of Li-ion cells. Anode and cathode materials are now subjects of numerous investigations. [1][2][3] Huggins performed some early work on alloy anodes. 4,5 Recently, Ioda et al., of Fujifilm Celltec Co., Ltd., announced a new class of anode material comprising a composite Sn oxide glass. 6,7 These Sn oxide glasses have a reversible capacity of approximately twice that of carbon materials but unfortunately exhibit a large irreversible capacity and problems with capacity fade after tens of charge-discharge cycles.Early evidence was that the Li inserted in the Sn oxide glass material was ionic, 7 but Courtney et al. have provided convincing evidence for the formation of metallic Sn and Sn-Li alloys during Li insertion. [8][9][10] The general picture is that Li will reduce the Sn oxides to metallic Sn. Further studies on the mechanism of Li insertion in tin oxides and alloys have been performed by Mao et al. 11,12 with 119 Sn Mössbauer spectrometry measurements using a sealed cell. With increasing Li concentration in the anode material, a series of Li-Sn phases were observed by X-ray diffractometry, 13 including Li 22 Sn 5 , which represents an increase in volume over that of pure -Sn by a factor of 3.6. Courtney and Dahn argued that since the increase in specific volume induces large local stresses, the cycle life of the electrode is poor when the Sn-rich regions in the electrode are large. [8][9][10][11][12][13] The role of microstructure on cycle life of Sn oxide anodes remains poorly understood, however.Althought the Fujifilm Celltec material has not yet been used for products in the marketplace, its promise has prompted a number of investigations into other Sn and Sn oxide materials that can be used as anodes in Li-ion cells. [9][10][11][12][13][14][15][16][17][18] One of the present authors has studied the insertion of Li into SnO,14 showing again that the Li served to reduce the Sn, and a Li-Sn alloy was formed at higher Li concentrations. Here we report results of 119 Sn Mössbauer spectrometry measurements at 11 and 300 K on partially and fully charged Li-SnO anode materials. We present detailed measurements of the recoil-free fractions (RFF) of the anode materials, and we show that the RFFs of the Sn oxide in the anode is anomalous, indicative of atomic-scale heterogeneities in the distribution of Sn atoms. Similar results are reported for the -Sn in the anode material, although the contribution from the -Sn is not definitively resolved from the Li 22 Sn 5 . We also present results from a study on the deterioration of Li-charged anode materials and Li-Sn alloys dur...