Defects-driven magnetism in bulk α-Li3N

Abstract

Ab-initio calculations based on density functional theory with local spin density approximation are used to study defects-driven magnetism in bulk α-Li3N. Our calculations show that bulk Li3N is a non-magnetic semiconductor. Two types of Li vacancies (Li-I and Li-II) are considered, and Livacancies (either Li-I or Li-II type) can induce magnetism in Li3N with a total magnetic moment of 1.0 µB which arises mainly due to partially occupied N-p-orbitals around the Li vacancies. The defect formation energies dictate that Li-II vacancy, which is in the Li2N plane, is thermodynamically more stable as compared with Li-I vacancy. The electronic structures of Li-vacancies show half-metallic behavior. On the other hand N-vacancy does not induce magnetism and has a larger formation energy than Li-vacancies. N vacancy derived bands at the Fermi energy are mainly contributed by the Li atoms. Carbon is also doped at Li-I and Li-II sites, and it is expected that doping C at Li-I site is thermodynamically more stable as compared with Li-II site. Carbon can induce metallicity with zero magnetic moment when doped at Li-I site, whereas magnetism is observed when Li-II site is occupied by the C impurity atom and C-driven magnetism is spread over the N atoms as well. Carbon can also induce half-metallic magnetism when doped at N site in Li3N, and has a smaller defect formation energy as compared with Li-II site doping. The ferromagnetic (FM) and antiferromagnetic (AFM) coupling between the C atoms is also investigated, and we conclude that FM state is more stable than the AFM state.

Behavior of NO3−-Based Electrolyte Additive in Lithium Metal Batteries

“…However, the activation energy for Li + ion diffusion is slightly Li 3 N crystals are generally a mixture of α and β phases (Figure 4a,b). Generally, the α phase appears at room temperature about 25 • C, and the β phase appears at high pressure and high temperature [69,70]. Under room temperature conditions, the β phase can transition to the α phase, with no significant difference in ionic conductivity observed between the two phases.…”