Ternary Metastable Nitrides ε‑Fe<sub>2</sub><i>TM</i>N (<i>TM</i> = Co, Ni): High-Pressure, High-Temperature Synthesis, Crystal Structure, Thermal Stability, and Magnetic Properties

Abstract

High-pressure, high-temperature synthesis gives access to ternary metastable nitrides ε-Fe<sub>2</sub><i>TM</i>N (<i>TM</i> = Co, Ni) as bulk materials for the first time. Both ε-Fe<sub>2</sub>CoN and ε-Fe<sub>2</sub>NiN crystallize isostructural to ε-Fe<sub>3</sub>N as evidenced by X-ray powder diffraction data. The lattice parameters of the new compounds are slightly smaller than those of ε-Fe<sub>3</sub>N owing to the reduced atomic radii of the metal atoms. Energy-dispersive X-ray spectroscopy of metallographic samples show homogeneous metal ratios corresponding to compositions Fe<sub>1.99(6)</sub>Co<sub>1.01(6)</sub>N and Fe<sub>1.97(2)</sub>Ni<sub>1.03(2)</sub>N. Extended X-ray absorption fine spectra indicate that cobalt and nickel occupy iron positions. Thermal analysis measurements reveal decomposition of both ternary nitrides above 920 K. ε-Fe<sub>2</sub>CoN disintegrates into N<sub>2</sub> and iron–cobalt alloy, while ε-Fe<sub>2</sub>NiN decays into N<sub>2</sub>, iron–nickel alloy as well as α-Fe. The replacement of iron by cobalt or nickel essentially lowers the saturation magnetization from roughly 6.0 μ<sub>B</sub>/f.u. for ε-Fe<sub>3</sub>N to nearly 4.3 μ<sub>B</sub>/f.u. for ε-Fe<sub>2</sub>CoN and 3.1 μ<sub>B</sub>/f.u. for ε-Fe<sub>2</sub>NiN. In parallel, the Curie temperature decreases from 575(3) K for ε-Fe<sub>3</sub>N to 488(5) K for ε-Fe<sub>2</sub>CoN and 234(3) K for ε-Fe<sub>2</sub>NiN. Calculations of the formation enthalpies illustrate that the phases ε-Fe<sub>2</sub><i>TM</i>N (<i>TM</i> = Co, Ni) are thermodynamically unfavorable at ambient conditions which is consistent with our experimental observations. The substitution of one Fe by Co (Ni) yields one (two) more electrons per formula unit which reduces the magnetic interactions. First-principles analysis indicate that the replacement has a negligible influence on the electron occupation numbers and spin moments of the N and unsubstituted Fe sites, but decreases the local magnetic moments on the substituted Fe positions because the extra electrons occupy the minority-spin channel formed by states of the <i>TM</i> atoms

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