Effect of Anion Mass on Conductivity and Lithium-Ion Transference Number in the Isomorphic Cocrystals (Adpn)₂LiXF₆ (Adpn = Adiponitrile, X = P, As, Sb)

Abstract

The solid lithium-ion electrolytes (Adpn) 2 LiXF 6 (Adpn = adiponitrile, X = P, As, Sb) are isomorphic salt-solvate cocrystals with slight differences in lattice spacing (<0.15 Å). The Li + cations are coordinated by Adpn molecules and separated from the anions so that the diffusion of the anions and cations is decoupled. As shown previously for the hexafluorphosphate analogue, (Adpn) 2 LiPF 6, the motion of Li + ions is through a solvate-mediated hopping mechanism, which is expected to be similar in all of the cocrystals. The crystal grains are surrounded and connected by a fluid-like grain-boundary network. Pulsed-field gradient 7 Li NMR, which measures diffusion in both the grains and the grain boundaries, indicated that the Li diffusion coefficients for the cocrystals were similar (<D Li + > = 1.77 × 10 –6 cm 2 /s). The transference numbers for Li + ions in Adpn 2 LiPF 6 measured by PFG-NMR at 80 °C, t Li +,PFG = 0.54, is in great agreement with t Li +,MD = 0.54 - predicted by molecular dynamics simulations at 27 °C using a grain-boundary atomistic model. Lithium-ion transference numbers, t Li +, calculated from steady-state impedance spectroscopy are 0.53, 0.63, and 0.83 for X = P, As, and Sb cocrystals, respectively, showing a lower contribution of anion charge carriers, with increasing mass of the anions, to the conductivity of these cocrystalline electrolytes. Diffusion coefficients for the AsF 6 – and SbF 6 – anions were calculated using measured values of σ and t Li + and decreased with increasing mass of the anion in the order D PF6 - > D AsF6 - > D SbF6 -. Conductivities of the cocrystals measured by EIS are in the order σ(Adpn 2 LiPF 6 ) > σ(Adpn 2 LiAsF 6 ) > σ(Adpn 2 LiSbF 6 ), while conductivities of 0.04 M solutions of the salts in Adpn decreased slightly in the opposite order LiSbF 6 > LiAsF 6 > LiPF 6 . The latter reflects better dissociation (and thus a greater number of free ions) of Li + from the heavier, more polarizable anions in dilute solution, attributed to hard–soft acid–base theory. In contrast, in the solid cocrystal, all ions are separated, and so conductivity is governed by the hopping ability of the ions, where the heavier anions diffuse more slowly. Since the total conductivity decreases in the opposite order, MD simulations suggest that the cations and anions in the nanoconfined regions of the grain boundaries are more concentrated and are exchangeable with the bulk phase grains.

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