Magnetic monolayer LiN: Density Functional Theory Calculations
arXiv:1710.04440 · doi:10.1209/0295-5075/119/57002
Abstract
Density functional theory (DFT) calculations are used to investigate the electronic and magnetic structures of a two-dimensional (2D) monolayer LiN. It is shown that bulk LiN is a non-magnetic semiconductor. The non-spinpolarized DFT calculations show that electrons of N in 2D LiN form a narrow band at the Fermi energy due to a low coordination number, and the density of states at the Fermi energy ()) is increased as compared with bulk LiN. The large ) shows instability towards magnetism in Stoner's mean field model. The spin-polarized calculations reveal that 2D LiN is magnetic without intrinsic or impurity defects. The magnetic moment of 1.0\, in 2D LiN is mainly contributed by the electrons of N, and the band structure shows half-metallic behavior. {Dynamic instability in planar LiN monolayer is observed, but a buckled LiN monolayer is found to be dynamically stable.} The ferromagnetic (FM) and antiferromagnetic (AFM) coupling between the N atoms is also investigated to access the exchange field strength. {We found that planar (buckled) 2D LiN is a ferromagnetic material with Curie temperature of 161 (572) K.}
arXiv commentEuro Phys. Lett. 2017 (Accepted)
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