C. Yang and H. R. Byon (Byon Initiative Research Unit, RIKEN, Japan)
The structure and morphology of lithium peroxide (Li
2O
2) in a lithium-oxygen (Li-O
2) cell have been widely explored by their correlation to recharge potential. A toroidal Li
2O
2 crystal with 0.1-1 μm size is a typical and predominant product observed on various carbonaceous cathodes after the 1
st discharge (2Li + O
2 ↔ Li
2O
2)
1 while the bulk size and poor conductivity of Li
2O
2 incurs its sluggish decomposition during the recharge, which results in a rapid potential rise more than 4.2 V vs. Li/Li
+ concomitant with severe side reactions. This potential shooting can be suppressed by some conductive additives such as metal and metal oxide nanoparticles (NPs), where non-crystalline and/or thin Li
2O
2 is interestingly observed after discharge. For example, our previous work demonstrated less 4.0 V of potential for the whole recharge process in the presence of RuO
2 NPs that led to the formation of amorphous Li
2O
2 film on the carbon nanotube (CNT) cathode during discharge via its high O
2 adsorption affinity.
2 Therefore, it is considered that the physical property of Li
2O
2, arising from both the poor crystallinity having higher ionic and electronic conductivity
3 and the thin-film shape providing large contact area with the CNT cathode,
4 is beneficial to smooth decomposition of Li
2O
2 at low potential. However, the criteria for promising additives contributing to the structure and morphology engineering of Li
2O
2 and mechanistic study for the formation and decomposition of such a unique structure of Li
2O
2 have not as yet been conducted. Here we present in-depth study of nucleation, growth and decomposition process of non-crystalline Li
2O
2 in the presence of cerium oxide (CeO
2) NPs using TEM and correlate this to Li-O
2 cell performance. The small diameter of CeO
2 NP (~5 nm) has strong affinity for the oxygen species (O
2, O
2- and O
22-),
5-6 which is accordingly a good candidate to investigate the evolution of Li
2O
2 morphology during discharge and recharge. At initial discharge, the nucleation of Li
2O
2 appears on the CeO
2 NPs, but not on the CNT, from which the Li
2O
2 laterally grows and coats over the CNT surface. The CeO
2 NPs determine the height of Li
2O
2 film, thus thicker Li
2O
2 film can be observed in the area of agglomerative CeO
2 NPs. Further discharge allows a vertical growth (i.e. thicker film) once the thin Li
2O
2 film covers the entire CNT surface. There is no evidence of Li
2O
2 crystal structure, which is very distinguished from the toroidal and polycrystalline Li
2O
2 observed on a CeO
2-free CNT (Fig. 1). The decomposition of Li
2O
2 seems to emerge from the amorphous and thin Li
2O
2 surface, which results in low recharge potential at the initial stage. However, the CeO
2 NPs having strong O
2 and CO
2 affinity
7 and poor conductivity become a hurdle for the completion of Li
2O
2 decomposition at low potential unlike the RuO
2 NPs. The implication of CeO
2 role and characteristics of the unique structure of Li
2O
2 based on different discharge and recharge status will be discussed in details in the presentation.
References:
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Fig. 1 TEM images of the discharged (a) CNT and (b) CeO2/CNT electrodes. Both Li-O2 cells are discharged at 50 mV g-1-CNT to 2.2 V vs. Li+/Li, using 0.5 M LiClO4 in TEGDME as electrolyte.