Colossal anisotropy of the magnetic properties of doped lithium nitrodometalates

We present a first-principles investigation of the electronic structure and physical properties of doped lithium nitridometalates Li sub(2) (Li sub(1-x)M sub(x))N (LiMN) with M = Cr, Mn, Fe, Co, and Ni. The diverse properties include the equilibrium magnetic moments, magneto-crystalline anisotropy,...

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Veröffentlicht in:Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2014-09, Vol.90 (9), Article 094406
Hauptverfasser: Antropov, V. P., Antonov, V. N.
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Sprache:eng
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Zusammenfassung:We present a first-principles investigation of the electronic structure and physical properties of doped lithium nitridometalates Li sub(2) (Li sub(1-x)M sub(x))N (LiMN) with M = Cr, Mn, Fe, Co, and Ni. The diverse properties include the equilibrium magnetic moments, magneto-crystalline anisotropy, magneto-optical Kerr spectra, and x-ray magnetic circular dichroism. We explain the colossal magnetic anisotropy in LiFeN by its unique electronic structure which ultimately leads to a series of unusual physical properties. The most unique property is a complete suppression of relativistic effects and freezing of orbital moments for in-plane orientation of the magnetization. This leads to the colossal spatial anisotropy of many magnetic properties including energy, Kerr, and dichroism effects. LiFeN is identified as an ultimate single-ion anisotropy system where a nearly insulating state can be produced by a spin orbital coupling alone. A very nontrivial strongly fluctuating and sign changing character of the magnetic anisotropy with electronic 3d-atomic doping is predicted theoretically. A large and highly anisotropic Kerr effect due to the interband transitions between atomic-like Fe 3d bands is found for LiFeN. A giant anisotropy of the x-ray magnetic circular dichroism for the Fe K spectrum and a very weak one for the Fe L sub(2,3) spectra in LiFeN are also predicted.
ISSN:1098-0121
1550-235X
DOI:10.1103/PhysRevB.90.094406