Structural, electronic, and magnetic properties of tetragonal Mn3-xGa: Experiments and first-principles calculations

Structural, electronic, and magnetic properties of tetragonal Mn3-xGa: Experiments and first-principles calculations
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DOI:
10.1103/physrevb.77.054406
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发表时间:
2008-02
期刊:
影响因子:
3.7
通讯作者:
Jürgen Winterlik;B. Balke;G. Fecher;C. Felser;M. Alves;F. Bernardi;J. Morais
Jürgen Winterlik;B. Balke;G. Fecher;C. Felser;M. Alves;F. Bernardi;J. Morais
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
Jürgen Winterlik;B. Balke;G. Fecher;C. Felser;M. Alves;F. Bernardi;J. Morais

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This work reports on the electronic, magnetic, and structural properties of the binary intermetallic compounds ${\mathrm{Mn}}_{3\ensuremath{-}x}\mathrm{Ga}$. The tetragonal ${\mathrm{DO}}_{22}$ phase of the ${\mathrm{Mn}}_{3\ensuremath{-}x}\mathrm{Ga}$ series, with $x$ varying from 0 to 1.0 in steps of $x=0.1$, was successfully synthesized and investigated. It was found that all these materials are hard magnetic, with energy products ranging from $10.1\phantom{\rule{0.3em}{0ex}}\mathrm{kJ}\phantom{\rule{0.2em}{0ex}}{\mathrm{m}}^{\ensuremath{-}3}$ for low Mn content $(x\ensuremath{\rightarrow}1)$ to $61.6\phantom{\rule{0.3em}{0ex}}\mathrm{kJ}\phantom{\rule{0.2em}{0ex}}{\mathrm{m}}^{\ensuremath{-}3}$ for high Mn content $(x\ensuremath{\rightarrow}0)$. With decreasing Mn content, the average saturation magnetization per atom increases from $0.26{\ensuremath{\mu}}_{B}$ for ${\mathrm{Mn}}_{3}\mathrm{Ga}$ to $0.47{\ensuremath{\mu}}_{B}$ for ${\mathrm{Mn}}_{2}\mathrm{Ga}$. The increase in the saturation magnetization as the Mn content is reduced indicates a ferrimagnetic order with partially compensating moments of the two different Mn atoms on the two crystallographically different sites of the ${\mathrm{DO}}_{22}$ structure. This type of magnetic order is supported by ab initio calculations of the electronic structure that predict a nearly half-metallic ferrimagnet with the highest spin polarization of 88% at the Fermi energy for ${\mathrm{Mn}}_{3}\mathrm{Ga}$. The Curie temperature of the compounds is restricted to approximately $770\phantom{\rule{0.3em}{0ex}}\mathrm{K}$ because of a structural phase transition to the hexagonal ${\mathrm{DO}}_{19}$ phase. Thermal irreversibilities between zero-field-cooled and field-cooled measurements suggest that the ${\mathrm{Mn}}_{3\ensuremath{-}x}\mathrm{Ga}$ series belongs to the class of magnetically frustrated ferrimagnets. The most pronounced magnetic anomaly is found for ${\mathrm{Mn}}_{3}\mathrm{Ga}$.
This work reports on the electronic, magnetic, and structural properties of the binary intermetallic compounds ${\mathrm{Mn}}_{3\ensuremath{-}x}\mathrm{Ga}$. The tetragonal ${\mathrm{DO}}_{22}$ phase of the ${\mathrm{Mn}}_{3\ensuremath{-}x}\mathrm{Ga}$ series, with $x$ varying from 0 to 1.0 in steps of $x=0.1$, was successfully synthesized and investigated. It was found that all these materials are hard magnetic, with energy products ranging from $10.1\phantom{\rule{0.3em}{0ex}}\mathrm{kJ}\phantom{\rule{0.2em}{0ex}}{\mathrm{m}}^{\ensuremath{-}3}$ for low Mn content $(x\ensuremath{\rightarrow}1)$ to $61.6\phantom{\rule{0.3em}{0ex}}\mathrm{kJ}\phantom{\rule{0.2em}{0ex}}{\mathrm{m}}^{\ensuremath{-}3}$ for high Mn content $(x\ensuremath{\rightarrow}0)$. With decreasing Mn content, the average saturation magnetization per atom increases from $0.26{\ensuremath{\mu}}_{B}$ for ${\mathrm{Mn}}_{3}\mathrm{Ga}$ to $0.47{\ensuremath{\mu}}_{B}$ for ${\mathrm{Mn}}_{2}\mathrm{Ga}$. The increase in the saturation magnetization as the Mn content is reduced indicates a ferrimagnetic order with partially compensating moments of the two different Mn atoms on the two crystallographically different sites of the ${\mathrm{DO}}_{22}$ structure. This type of magnetic order is supported by ab initio calculations of the electronic structure that predict a nearly half-metallic ferrimagnet with the highest spin polarization of 88% at the Fermi energy for ${\mathrm{Mn}}_{3}\mathrm{Ga}$. The Curie temperature of the compounds is restricted to approximately $770\phantom{\rule{0.3em}{0ex}}\mathrm{K}$ because of a structural phase transition to the hexagonal ${\mathrm{DO}}_{19}$ phase. Thermal irreversibilities between zero-field-cooled and field-cooled measurements suggest that the ${\mathrm{Mn}}_{3\ensuremath{-}x}\mathrm{Ga}$ series belongs to the class of magnetically frustrated ferrimagnets. The most pronounced magnetic anomaly is found for ${\mathrm{Mn}}_{3}\mathrm{Ga}$.