A Haxpes Study on Solid Electrolyte Interphase Formed on a Carbon Negative Electrode
Authors: Matsumoto Masashi , Kamiguchi Kazuhiro , Sanada Takashi , Imamura Daichi , Imai Hideto 
Published: February 2020

Solid electrolyte interphase (SEI) formed on a carbon negative electrode plays an important role in supporting the reversible Li ion intercalation phenomena during charge and discharge treatments. Since the chemical and electrochemical conditions of the electro-lyte/electrode interface change during electrochemical lithiation and delithiation reactions, the structure of the SEI might change even after the formation of the SEI by the initial charge and discharge treatments, although details of the reaction mechanism remain unknown. We, therefore, investigated the behavior of the SEI of a carbon negative electrode during electrochemical lithiation and delithiation reactions by using Hard X-ray photoelectron spectroscopy (HAX-PES) technique.

Lithiated and delithiated carbon anodes were prepared by using a coin-type cell with Li metal. The carbon anode was a composite graphite (active agents, carbon black, PVDF) coated on Cu foil. The electrolyte was 1 M LiPF6 in ethylene carbonate / diethyl carbonate (EC / DEC) in a 1:1 volume ratio. After charge and discharge, the cell was disassembled and the anode was then retrieved, washed with dimethyl carbonate repeatedly in an argon-filled glovebox (<1 ppm H2O, <1 ppm O2). The anodes were transferred from the glovebox to UHV measurement chamber without exposing to the air by using special transfer systems. The HAXPES measurements were carried out at the BL46XU beamline at SPring-8. The photon energy of incident x-rays was 8 keV.

Figure 1 shows C 1s HAXPES spectra for the lithiated graphite anodes with the state of charge (SOC) 0%, 50%, 100% after twice charge and discharge cycles. The spectra were fitted with six singlets centered at 283.5eV (Peak 1), 284.6 eV (Peak 2), 285.5 eV (Peak 3), 287 eV(Peak 4), 289 eV(Peak 5) and 290.5 eV(Peak 6). Peak 1 can be assigned to lithiated carbon LixC. Peak 2 can be assigned to hydrocarbons for lithium alkyl carbonate (LAC), the organic materials of SEI and PVDF binder. The carbonyl components for the LAC are observed as Peak 3, Peak 4, and Peak 5. Peak 6 can be associated with a organofluorine component for the PVDF binder and a carbonate component for the Li2CO3, a inorganic material of SEI. LixC was observed in the C 1s HAXPES spectra with all SOC conditions, whereas this peak wasn’t observed in the C 1s XPS spectra with Al K-α incident x-rays for the lithiated graphite anodes with SOC 50%, 100% after twice charge and discharge cycles (the C 1s XPS spectra were not shown). This result indicates that the probing depth of HAXPES (hν = 8keV) is larger than thickness of SEI, thus HAXPES detected whole SEI and a part of the LixC exists underneath SEI formed on all the lithiated graphite anodes in the depth direction. HAXPES technique allows us to analyze the variation of the chemical composition of SEI depending on electrochemical lithiation and delithiation reactions. Table 1 shows the concentration ratio of LixC, LAC, and Li2CO3 depending on SOC determined by the C 1s HAXPES spectra. The ratio of LixC decreases up to SOC 100%, while those of LAC, and Li2CO3 increases up to SOC 100%. This variation shows the structural behavior of the SEI during electrochemical lithiation reactions after the formation of the SEI by the initial charge and cycles: SEI continues growth and dissolution even after stable state is established.

Acknowledgement

The synchrotron experiments were carried out on beamline BL46XU at Spring-8 with approvals from Japan synchrotron radiation institute (JASRI) (Proposal nos. 2013A1234)

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