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An Atomistic Study of Reactivity in Solid-State Electrolyte Interphase Formation for Li/Li7P3S11

Lithium metal batteries offer superior volumetric and gravimetric specific capacities compared to those based on traditional graphite anodes. Although advancements in solid-state electrolytes address safety concerns, challenges remain, particularly regarding interphase formation in lithium metal anodes. This work presents a computational framework based on high-throughput first-principles density functional theory and machine-learning interatomic potentials (MLIPs) including automated iterative, active learning to enable robust computational exploration of interphase formation between lithium metal anodes and an inorganic solid-state electrolyte. As a demonstration, we apply the framework to a Li/Li7P3S11 interface and find that it accurately identifies the experimentally observed, thermodynamically stable interphase products as well as their overall spatial arrangement within a heterogeneous, amorphous layered structure, with Li2S domains of nanocrystallinity. Our simulations show two stages, a fast and slow diffusion reaction regime, that corroborate the relative phase formation rate of Li x P, Li2S, and Li3P. Using the Onsager transport theory, we capture time-dependent ionic diffusion within the reacting interface, including cross-correlation effects. We found that cross-correlation effects between Li-P and P-S ionic motion significantly influence P-ion diffusion, making it highly sensitive to the local environment and potentially leading to "kinetic trapping" of Li-P phases. The passivation of the interface is shown as the ionic fluxes all approach zero, effectively halting interphase growth.

Diffusion↗

Materials Data on Li3P by Materials Project

Li3P is Sodium arsenide structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a trigonal planar geometry to three equivalent P3- atoms. All Li–P bond lengths are 2.45 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four equivalent P3- atoms. There are one shorter (2.53 Å) and three longer (2.75 Å) Li–P bond lengths. P3- is bonded in a 5-coordinate geometry to eleven Li1+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiP by Materials Project

LiP crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six P1- atoms. There are a spread of Li–P bond distances ranging from 2.58–2.79 Å. In the second Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six P1- atoms. There are a spread of Li–P bond distances ranging from 2.58–2.77 Å. There are two inequivalent P1- sites. In the first P1- site, P1- is bonded in a 8-coordinate geometry to six Li1+ and two equivalent P1- atoms. There are one shorter (2.22 Å) and one longer (2.24 Å) P–P bond lengths. In the second P1- site, P1- is bonded in a 8-coordinate geometry to six Li1+ and two equivalent P1- atoms.

36 MATERIALS SCIENCE↗