both thermally and electrochemically. [2][3][4] Cathodes with high nickel content (y > 0.8) are also more difficult to synthesize, requiring oxygenrich calcination conditions, and are more prone to lithium/transition-metal siteexchange. [5][6][7][8][9] Thermal parameters play a critical role in the morphology of the final cathode, which strongly affects its rate performance and cyclability. Advanced understanding of the underlying chemistry during synthesis is necessary to enable Ni-rich cathodes to operate closer to their theoretical performance limits.Preparation of Ni-rich LiNi y Mn z Co 1−y−z O 2 cathode material is a two-stage process, first involving the co-precipitation of a Ni 0.8 Mn 0.1 Co 0.1 (OH) 2 species followed by calcination of the resultant precursor with a lithium salt, typically LiOH•H 2 O. Calcination, which requires prolonged times at temperatures up to 750-900 °C in pure oxygen condition for Ni-rich cathodes, is the most energy intensive step. [10] During this process, water is lost from Ni y Mn z Co 1−y−z (OH) 2 , and lithium and oxygen enter the structure forming the final LiNi y Mn z Co 1−y−z O 2 cathode. The details of this transformation are not fully understood. While both the hydroxide precursor and final LiNi y Mn z Co 1−y−z O 2 cathode share a layered structure, prior research has implicated an intermediate cubic structure resembling rock salt, [11] recently confirmed using in situ powder X-ray diffraction (XRD). [12,13] These phases share an oxygen sub-lattice, and so the mechanism has been ascribed to a topotactic transformation involving extensive cation ordering. [14,15] In addition, several competing processes occur at high temperatures, where cation mixing and particle growth have been shown to depend on calcination temperature and hold time. [16] The final cathode performance is closely tied to the morphology of the constituent particles. [17] LiNi 0.8 Mn 0.1 Co 0.1 O 2 often has a hierarchical structure consisting of large (≈10 μm) agglomerates of small (≈100 nm) single crystal primary particles. Secondary particle size is largely controlled by coprecipitation conditions, whereas primary particles are affected by thermal parameters during calcination.Smaller particles (<100 nm) result in higher rate capability, [18][19][20][21] attributed to increased surface area and shorter Nanoscale morphology has a direct impact on the performance of materials for electrochemical energy storage. Despite this importance, little is known about the evolution of primary particle morphology nor its effect on chemical pathways during synthesis. In this study, operando characterization is combined with atomic-scale and continuum simulations to clarify the relationship between morphology of cathode primary particles and their lithiation during calcination of LiNi 0.8 Mn 0.1 Co 0.1 O 2 (NMC-811). This combined approach reveals a key role for surface oxygen adsorption in facilitating the lithiation reaction by promoting metal diffusion and oxidation, and simultaneously providing surface sites for ...