Abstract
The hexagonal EuMX (M=Cu, Ag, Au; X=P, As, Sb, Bi) compounds host interesting electronic and magnetic properties, with seemingly intertwined topology and transport properties. One key feature of such behavior is the nature of the ordered magnetic structure. In EuCuAs, a topological Hall effect is caused by a conical spin structure that emerges when a field is applied within the easy-plane (H ⊥ c) of the helical ground state that exists below the Neel temperature of TN=14K. On the other hand, EuCuP is an easy-axis ferromagnet with a Curie temperature TC near 31 K. Here, we investigate the evolution of the magnetic properties in EuCuAs1-xPx single crystals with 0.16 ≤x≤ 0.75. Crystals grown by cooling slowly in a Sn flux possessed macroscale inhomogeneity of As/P, particularly for arsenic-rich crystals. However, growth in a Sn flux via an isothermal dwell at 600∘C produced crystals that were homogeneous within the resolution of the probes utilized to investigate these crystals. The unit cell volumes, Curie-Weiss temperatures, and magnetic transitions trend linearly with composition and the magnetic anisotropy is reduced in the alloys. The magnetization data of crystals with x=0.16 and 0.24 indicate an easy-plane antiferromagnetic ground state while behavior similar to ferromagnetism is observed for crystals with x≥ 0.41. The temperature-dependent magnetization data possess multiple transitions for compositions near EuCuAs0.75P0.25, revealing a competition of ground states in this arsenic-rich region of the phase diagram. Neutron diffraction data for EuCuP are also presented as a follow up to previous results that revealed a two-step transition at TC; the observed data were consistent with ferromagnetic order at T=5K.
Original language | English |
---|---|
Article number | 084410 |
Journal | Physical Review Materials |
Volume | 8 |
Issue number | 8 |
DOIs | |
State | Published - Aug 2024 |
Funding
This work was supported by the U. S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division. A portion of this research used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. We thank J. Yan and M. McGuire for useful discussions. ACKNOWLEDGMENTS This work was supported by the U. S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division. A portion of this research used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. We thank J. Yan and M. McGuire for useful discussions.
Funders | Funder number |
---|---|
Basic Energy Sciences | |
Division of Materials Sciences and Engineering | |
Oak Ridge National Laboratory | |
U.S. Department of Energy | |
Office of Science |