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Topotaxially grown composite cathodes for cobalt-free high-energy long-life Li-ion batteries

The vehicle industry’s increasing demand for electrification necessitates the removal of expensive and rare cobalt from current high-energy batteries. However, eliminating cobalt poses challenges due to its vital role in maintaining the layered structural ordering and cycling stability of commonly used Li(NiMnCo)O 2 cathodes. As an alternative to conventional layered oxide designs, we report a lithium nickelate cathode with a composite structure comprising major stoichiometric layered and minor rocksalt phases within the same oxygen lattice. This material outperforms conventional designs by maintaining stable battery operation at voltages up to 4.8 V vs. Li|Li + , with 88% capacity retention after 1000 cycles at 2C. The topotaxial-growth-enabled interlock between the two components mitigates chemo-mechanical degradation, offering a promising pathway to cobalt-free cathodes. Additionally, we reveal a miscibility gap in the Li-Ni-O system that enables kinetic adjustment of composition and structure during sintering, thereby tuning the functionality of high-energy cathodes.

25 ENERGY STORAGE↗

Materials Data on Li7(NiO2)11 by Materials Project

Li7(NiO2)11 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six NiO6 octahedra, edges with three LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 8–12°. There are a spread of Li–O bond distances ranging from 2.03–2.24 Å. In the second Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six NiO6 octahedra, edges with two equivalent LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 9–15°. There are four shorter (2.09 Å) and two longer (2.16 Å) Li–O bond lengths. In the third Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six NiO6 octahedra, edges with three LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 10–13°. There are a spread of Li–O bond distances ranging from 2.06–2.17 Å. In the fourth Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six NiO6 octahedra, edges with three LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 8–12°. There are a spread of Li–O bond distances ranging from 2.06–2.19 Å. There are six inequivalent Ni+3.36+ sites. In the first Ni+3.36+ site, Ni+3.36+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with three LiO6 octahedra, edges with four LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 10–11°. There are a spread of Ni–O bond distances ranging from 1.87–2.09 Å. In the second Ni+3.36+ site, Ni+3.36+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with five LiO6 octahedra, edges with three LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 8–15°. There are a spread of Ni–O bond distances ranging from 1.88–2.01 Å. In the third Ni+3.36+ site, Ni+3.36+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with three LiO6 octahedra, edges with four LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 8–10°. There are a spread of Ni–O bond distances ranging from 1.84–1.93 Å. In the fourth Ni+3.36+ site, Ni+3.36+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with four LiO6 octahedra, edges with four LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 9–11°. There are a spread of Ni–O bond distances ranging from 1.86–1.98 Å. In the fifth Ni+3.36+ site, Ni+3.36+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with four LiO6 octahedra, edges with four LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedral tilt angles are 12°. There are a spread of Ni–O bond distances ranging from 1.88–2.06 Å. In the sixth Ni+3.36+ site, Ni+3.36+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with four LiO6 octahedra, edges with four LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedra tilt angles range from 10–13°. There are a spread of Ni–O bond distances ranging from 1.87–2.07 Å. There are eleven inequivalent O2- sites. In the first O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the second O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the third O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Ni+3.36+ atoms. In the fourth O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the fifth O2- site, O2- is bonded to two equivalent Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the sixth O2- site, O2- is bonded to two equivalent Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the seventh O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the eighth O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the ninth O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the tenth O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids. In the eleventh O2- site, O2- is bonded to two Li1+ and three Ni+3.36+ atoms to form a mixture of edge and corner-sharing OLi2Ni3 square pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Li(NiO2)3 by Materials Project

Li(NiO2)3 is Corundum-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six NiO6 octahedra and edges with six NiO6 octahedra. The corner-sharing octahedral tilt angles are 13°. There are two shorter (2.07 Å) and four longer (2.15 Å) Li–O bond lengths. There are two inequivalent Ni+3.67+ sites. In the first Ni+3.67+ site, Ni+3.67+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with two equivalent LiO6 octahedra, edges with two equivalent LiO6 octahedra, and edges with six equivalent NiO6 octahedra. The corner-sharing octahedral tilt angles are 13°. There is four shorter (1.90 Å) and two longer (2.08 Å) Ni–O bond length. In the second Ni+3.67+ site, Ni+3.67+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with two equivalent LiO6 octahedra, edges with two equivalent LiO6 octahedra, and edges with six NiO6 octahedra. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ni–O bond distances ranging from 1.85–1.91 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Ni+3.67+ atoms. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Ni+3.67+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Li2Ni5O7 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on LiNi3O4 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on LiNiO2 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on LiNi6O7 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗