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First-principles study of the structures and redox mechanisms of Ni-rich lithium nickel manganese cobalt oxides

To reduce the cobalt (Co) content in lithium-ion batteries, Ni-rich (high-Ni) lithium nickel manganese cobalt oxides (NMC) are pursued as one of the next-generation cathode materials. However, there is still debate on the crystal and electronic structures of the baseline, LiNiO 2 . Density Functional Theory (DFT) calculations were performed to provide a theoretical understanding of Ni-rich NMC. First, it was found that the commonly used $R\bar{3}m$ structure for LiNiO 2 is metallic, contrary to the experimentally reported mix-conducting behavior. Among the four different space groups, $R\bar{3}m$, C2/m, P2 1 /c, and P2/c, P2/c with charge disproportionation of Ni 2+ and Ni 4+ is the most energetically stable and semiconducting structure of LiNiO 2 . Therefore, the atomic structures of representative Ni-rich NMC were built by partially replacing Ni with Co or Mn in the P2/c LiNiO 2 to form Li x Ni y Mn z Co 1-y-z O 2 . In the fully lithiated (x=1.0) high Ni content NMC (y>0.5), the oxidation state of all Mn ions becomes 4+, while Co ions still maintain 3+, and part of the Ni ions become 3+ to compensate for the charge. Upon delithiation, the local environment shows more variation of the charge states on the transition metal (TM) ions. The average oxidation on each TM follows a sequence of losing electrons that starts from Ni 2+ to Ni 3+ , then oxidizing Ni 3+ and Co 3+ , while Mn 4+ remains electrochemically inactive till x=0. Finally, a general relationship for the oxidation state change in each TM as a function of x is derived and shows agreement with both modeling and experimental data.

25 ENERGY STORAGE↗

Materials Data on Ta2I5 by Materials Project

Ta2I5 crystallizes in the triclinic P1 space group. The structure is two-dimensional and consists of one Ta2I5 sheet oriented in the (0, 0, 1) direction. there are two inequivalent Ta sites. In the first Ta site, Ta is bonded in a 5-coordinate geometry to five I atoms. There are a spread of Ta–I bond distances ranging from 2.73–2.99 Å. In the second Ta site, Ta is bonded in a 5-coordinate geometry to five I atoms. There are a spread of Ta–I bond distances ranging from 2.73–3.00 Å. There are five inequivalent I sites. In the first I site, I is bonded in a bent 120 degrees geometry to two Ta atoms. In the second I site, I is bonded in a bent 150 degrees geometry to two Ta atoms. In the third I site, I is bonded in a 2-coordinate geometry to two Ta atoms. In the fourth I site, I is bonded in a 2-coordinate geometry to two Ta atoms. In the fifth I site, I is bonded in a bent 150 degrees geometry to two Ta atoms.

36 MATERIALS SCIENCE↗

Materials Data on TaI4 by Materials Project

TaI4 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of one TaI4 cluster. there are two inequivalent Ta4+ sites. In the first Ta4+ site, Ta4+ is bonded to six I1- atoms to form a mixture of edge and face-sharing TaI6 octahedra. There are a spread of Ta–I bond distances ranging from 2.68–2.90 Å. In the second Ta4+ site, Ta4+ is bonded to six I1- atoms to form face-sharing TaI6 octahedra. There are a spread of Ta–I bond distances ranging from 2.67–2.92 Å. There are eight inequivalent I1- sites. In the first I1- site, I1- is bonded in a water-like geometry to two equivalent Ta4+ atoms. In the second I1- site, I1- is bonded in a 2-coordinate geometry to two Ta4+ atoms. In the third I1- site, I1- is bonded in a 2-coordinate geometry to two Ta4+ atoms. In the fourth I1- site, I1- is bonded in a single-bond geometry to one Ta4+ atom. In the fifth I1- site, I1- is bonded in a single-bond geometry to one Ta4+ atom. In the sixth I1- site, I1- is bonded in a single-bond geometry to one Ta4+ atom. In the seventh I1- site, I1- is bonded in a 2-coordinate geometry to two Ta4+ atoms. In the eighth I1- site, I1- is bonded in a single-bond geometry to one Ta4+ atom.

36 MATERIALS SCIENCE↗