High-voltage Li-ion batteries have been extensively studied to increase the energy density of batteries. To achieve this goal, 5 V class cathode materials have been developed, but the long-term stable operation has not been achieved. Recently, we reported that the poor cycle stability comes not only from the oxidative degradation of the electrolyte and/or cathode active material, but also from side reactions caused by the insertion of anions into the interlayer of a cathode conductive carbon [1]. However, the detailed mechanism of anion insertion into the conductive carbon is still not well understood. In this study, we theoretically investigated the anion insertion process at the interface between a graphite and EC-based electrolyte solution (1 M LiPF6 / EC).We adopted a density functional theory (DFT) in combination with the effective screening medium and reference interaction site model (ESM-RISM) method to analyze the insertion process of a PF6 - anion into the graphite [2]. The simulation cells are composed of graphite electrode (C252(PF6)9H36) and the 1 M LiPF6 / EC electrolyte, where the entire graphite electrode are treated quantum mechanically, whereas the electrolyte components are treated classically by the RISM method. The activation energy was calculated by computing the grand potential (Ω) at each point while moving a PF6 - anion from its initial position on the electrolyte side (r = 20 Å) to the electrode interior (r = 0 Å). These calculations were performed at two different electrode potentials, the potential of zero charge (PZC) and the equilibrium potential of the anion insertion reaction, respectively. All the DFT and ESM-RISM calculations were conducted using the Quantum Espresso v.6.1 code.The figure shows the profiles of Ω along the insertion process of the PF6 – anion into the graphite layer. The activation energies were estimated to be 0.49 eV (ΩPZC, black line) and 0.37 eV (Ωeq, red line) at the PZC and the equilibrium potential, respectively, considerably smaller than that of Li+ (0.6 eV) [3]. Importantly, the coordination number of EC molecules around PF6 – (N EC, blue line) decreases from about 10 Å and Ω becomes correspondingly unstable, indicating that the desolvation of PF6 – contributes significantly to the activation barrier. Furthermore, systematic calculations of the desolvation energies for different solvent species show that the calculated values tend to increase as the dipole moment of the solvent molecule decreases. Therefore, a use of solvents with smaller dipole moments would increase the desolvation energy, thus suppressing the anion insertion.1) S. Ko et al., Joule, 5, 998 (2021).2) S. Nishihara et al., Phys. Rev. B, 96, 115429 (2017).3) J. Haruyama et al., J. Phys. Chem. C, 122, 9804 (2018). Figure 1
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