4.7 Article

Helical spin ordering in room-temperature metallic antiferromagnet Fe3Ga4

Journal

JOURNAL OF ALLOYS AND COMPOUNDS
Volume 917, Issue -, Pages -

Publisher

ELSEVIER SCIENCE SA
DOI: 10.1016/j.jallcom.2022.165532

Keywords

Magnetically ordered materials; Transition metal alloy and compounds; Metamagnetism; Growth from vapor; Density functional theory (DFT)

Funding

  1. NSF [DMR-EPM 1904446, ONR 1400844839]
  2. U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division
  3. National Science Foundation (USA) [DMR-1905662]
  4. Air Force Office of Scientific Research (USA) [FA9550-20-1-0247]
  5. US Department of Energy (DOE) , Office of Science, Basic Energy Sciences [DE-SC0022216]
  6. National Energy Research Scientific Computing Center through DOE [DE-AC02-05CH11231]
  7. Ministry of Education and Culture (Finland)
  8. RSF-Russian Science Foundation [22-12-20032]
  9. Ministry of Science and Higher Education of the Russian Federation [075-01391-22-00]
  10. DFG (German Research Foundation) [405553726]
  11. U.S. Department of Energy (DOE) [DE-SC0022216] Funding Source: U.S. Department of Energy (DOE)

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In this study, a complex magnetic phase diagram of metallic Fe3Ga4 at room temperature was obtained, and a model for the intermediate antiferromagnetic helical spin structure state was proposed. The results showed that the antiferromagnetic state had a helically ordered spiral propagating along the c-axis, with the magnetic moments rotating in the ab-plane. Under applied magnetic field, the antiferromagnetic state exhibited a transition to conical ordering, before entering a completely field-polarized ferromagnetic state.
Metallic Fe3Ga4 displays a complex magnetic phase diagram that supports an intermediate antiferromagnetic (AFM) helical spin structure (HSS) state at room temperature which lies between two ferromagnetic (FM) phases. Magnetic measurements along the three crystallographic axes were performed in order to develop a model for the temperature and field dependence of the HSS state. These results show that the AFM state is a helically ordered spiral propagating along the c-axis with the magnetic moments rotating in the ab-plane. Under applied magnetic field, the AFM state exhibits a metamagnetic transition to conical ordering before entering a fully field-polarized FM state at high fields. The conical ordering in the AFM state is anisotropic even within the ab-plane and may gives rise to Berry phase effects in transport measurements. Metallic conductivity from density of states computations was confirmed through resistivity measurements and no anomalous behavior was observed through the various magnetic transitions. Published by Elsevier B.V.

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