Abstract
The maximum discharge capacity in non-aqueous Li-O2 batteries has been limited to a fraction of its theoretical value, largely due to a conformal deposition of Li2O2 on the cathode surface. However, it has recently been established that additives that increase the shielding of either O2− or Li+ will activate the formation of toroidal shaped Li2O2, thereby dramatically increasing cell capacity. Here we apply porous electrode theory to electrochemical impedance measured at the Li-O2 cathode to investigate changes in the surface- and ionic resistance within the pores under conditions where either the surface-mechanism or the solution-mechanism is favored. Our experimental observations show that (i) an additional charge transfer process is observed in the impedance spectrum where the solution-based mechanism is favored; (ii) that the changes in the ionic resistance in the cathode during discharge (related to Li2O2 build up) is much greater in cells where the solution-based mechanism is activated and can qualitatively determine the extent of discharge product deposited within the pores of the cathode versus the deposition extent at the electrode/electrolyte interface; and (iii) that the observed “sudden-death” during discharge is a consequence of the increasing charge transfer resistance regardless of whether Li2O2 forms predominantly through either the surface- or solution-based mechanism.
Highlights
We argue that the two activated electrochemical cathode processes detected when applying a current, i.e. the low frequency (LF)- and high frequency (HF) semicircles, observed in Figure 6 and S5, are mainly related to the formation of Li2O2 since (i) a ∼2.0–2.1 e−/O2 reaction is observed from pressure
The cathodic impedance displayed three electrochemical processes: a linear region at high frequency related to the porous structure of the cathode, a high, and a low frequency process
The low frequency process was not detected in Ar at OCV, but could be activated by applying a current in an O2 atmosphere
Summary
The low frequency (LF) semicircle.—The LF process observed in Figure 6 and S5 contain both the cathode surface/electrolyte interfacial charge transfer (RCT), the double-layer capacitance of the same interface (Ceff), and the proxy for the extent of pore clogging with the ionic resistance (Ri) when modeled with the Rs-(R1Q1)1-PETζ=RQ2 equivalent circuit.
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