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16.3 SEI Formation on Carbonaceous Electrodes  505

               Li 2 SO 3 ,Li 2 S 2 O 5 , and Li 2 S). The predominating surface reactions in LiAsF 6 /MF–EC
               electrolytes contaminated withwater [85]result inthe formationof insoluble lithium
               alkylcarbonates, Li 2 O, and LiOH (Figure 16.1). EDX analysis of the surface film
               formed on mesocarbon-derived carbon fibers in LiBF 4 /EC–PC–DME solution
               [113] indicated that the film is composed of C, F, B, and O. SEM measurements
               showed that the lithiated carbon fibers cohere as a result of the formation of
               a passivating film [113]. An unstable passivating layer on petroleum coke in Li
               triflate/EC–PC–DMC, followed by interaction between the electrolyte and the
               intercalated lithium , was observed by Jean et al. [114]. The increased stability of
               lithium-carbon electrodes in EC-containing electrolytes [86] was related to inorganic
               films formed via secondary chemical decomposition of electrochemically formed
               EC–graphite-intercalation compounds. Using CV, Inaba et al. [89] found that, for
               graphite electrodes, an EC–DEC solvent mixture is preferred over EC–DME with
               respect to the formation of a stable passivating film. When graphite electrodes
               are charged in PC-based solutions, the solvent decomposes at about 1 V, and
               this makes SEI formation difficult. It was shown [76] that LiBF 4 is more reactive
               than LiPF 6 toward an Li x C 6 anode. A lithium-ion battery based on LiPF 6 /EC-DEC
               (7 : 3) electrolyte [115] underwent more than 300 stable charge–discharge cycles.
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               However an increase of cell resistance from 1.5 to 3.5k  cm was observed on
               cycling, and this was attributed to the decomposition of electrolyte.
                Lithium intercalation into graphite was studied by Morita et al. [116], who used
               XRD and electrochemical QCMB techniques. The XRD pattern of the graphite elec-
               trode after cathodic polarization in LiClO 4 /EC–DMC solution shows a spectrum
               that is more complicated than that for an electrode polarized in EC–PC mixture.
               The diffraction angles observed do not correspond exactly to the values expected
               from any idealized stage structure of Li x C 6 . Changes in the resonance frequency of
               the graphite-coated quartz crystal showed that the cathodic intercalation of lithium
               is accompanied by electrochemical decomposition of the electrolyte The mass
                                                                  +
               change per coulomb over the potential range of 0.0–0.2 V vs Li/Li was higher in
               EC–DMC than in EC–PC, indicating different surface reactions.
                Lithium carbonate and hydrocarbon were identified in XPS spectra of graphite
               electrodes after the first cycle in LiPF 6 /EC–DMC electrolyte [109]. Electrochemical
               QCMB experiments in LiAsF 6 /EC–DEC solution [102] clearly indicated the for-
               mation of a surface film at about 1.5 V vs (Li/Li ). However, the values of mass
                                                     +
               accumulation per mole of electrons transferred (m.p.e), calculated for the sur-
               face species, were smaller than those of the expected surface compounds (mainly
               (CH 2 OCO 2 Li) 2 ). This was attributed to the low stability of the SEI and its partial
               dissolution.

               16.3.5.2 HOPG
               HOPG was used as a model electrode to study separately the formation of the
               SEI on the basal and cross-section planes [103]. The cross-section planes of HOPG
               consist of both zig-zag and armchair planes. Carbon atoms on these two planes
               are considered to be much more active than carbon atoms on the basal plane
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