Structural characterisation of the highly deintercalated LixNi1.02O2 phases (with x <= 0.30)

The full structural characterisation of the highly deintercalated LixNi1.02 O2 (x less than or equal to 0.30) phases has been performed. The structure of the Li0.30Ni1.02O2 phase was refined by the Rietveld method. The cationi c distribution was found to be identical to that of the pristine material. A study of the Li//LixNi1.02O2 system at high potential has shown the succe ssive formation of two phases with O3 (AB CA BC) and O1 (AB) oxygen packing , respectively, near the NiO2 composition. Since slab gliding is at the ori gin of the O3 to O1 transition, layer displacement faults were observed in these two phases. For the O3 phase, as soon as all the lithium ions are rem oved from an interslab space, an O1-type fault occurs locally. In contrast, for the O1 phase, the presence of extra-nickel ions in the interslab space prevents slab gliding in the vicinity and, therefore, O3-type interslab sp aces remain in the O1-type packing. The X-ray diffraction patterns were sim ulated using the DIFFaX program. It was shown that the stabilisation of the O1-type packing at the very end of the deintercalation process is due to a minimisation of the interactions between the p orbitals of the oxygen ions through the van der Waals gap. A two-phase domain is observed between Li0. 30NiO2 and a composition close to NiO2 since, for very low lithium contents , the Ni3+/Ni4+ ordering (and the lithium/vacancy ordering) is no longer po ssible and the difference in size between the cations leads to the formatio n of constraints which destabilise the Ni3+ ions in a lattice where Ni4+ io ns prevail. At the end of the deintercalation process, the NiO2 compound ap pears to be highly covalent, therefore, the steric effects prevail over the electrostatic repulsion effects, as in chalcogenides.