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    Local Structure of Li<sup>+</sup> in Concentrated Ethylene Carbonate Solutions Studied by Low-Frequency Raman Scattering and Neutron Diffraction with <sup>6</sup>Li/<sup>7</sup>Li Isotopic Substitution Methods

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    Isotropic Raman scattering and time-of-flight neutron diffraction measurements were carried out for concentrated LiTFSA-EC solutions to obtain structural insight on solvated Li<sup>+</sup> as well as the structure of contact ion pair, Li<sup>+</sup>···TFSA<sup>–</sup>, formed in highly concentrated EC solutions. Symmetrical stretching vibrational mode of solvated Li<sup>+</sup> and solvated Li<sup>+</sup>···TFSA<sup>–</sup> ion pair were observed at ν = 168–177 and 202–224 cm<sup>–1</sup>, respectively. Detailed structural properties of solvated Li<sup>+</sup> and Li<sup>+</sup>···TFSA<sup>–</sup> contact ion pair were derived from the least-squares fitting analysis of first-order difference function, Δ<sub>Li</sub>(<i>Q</i>), between neutron scattering cross sections observed for <sup>6</sup>Li/<sup>7</sup>Li isotopically substituted 10 and 25 mol % *LiTFSA-EC<i>d</i><sub>4</sub> solutions. It has been revealed that Li<sup>+</sup> in the 10 mol % LiTFSA solution is fully solvated by ca. 4 EC molecules. The nearest neighbor Li<sup>+</sup>···O­(EC) distance and Li<sup>+</sup>···O­(EC)C­(EC) bond angle are determined to be 1.90 ± 0.01 Å and 141 ± 1°, respectively. In highly concentrated 25 mol % LiTFSA-EC solution, the average solvation number of Li<sup>+</sup> decreases to ca. 3 and ca. 1.5. TFSA<sup>–</sup> are directly contacted to Li<sup>+</sup>. These results agree well with the results of band decomposition analyses of isotropic Raman spectra for intramolecular vibrational modes of both EC and TFSA<sup>–</sup>
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