Magnetic phase transitions and structures of the spin-chain compound
BaErFeO4 were investigated by measurements of magnetic properties (specific heat, magnetic susceptibility) and neutron diffraction. The lattice geometry of the orthorhombic crystal structure (space group ) of the
BaRFeO4 compounds (
R=Dy–Yb, Y) supports frustrations which lead to multiple magnetic phase transitions with complex magnetic structures.
BaErFeO4 undergoes three successive magnetic phase transitions at
TN1=49K, TN2=33.4K, and
TN3=3.4K. In contrast with the previously investigated
BaRFeO4 (
R=Y, Tm, Yb) compounds, all with incommensurate magnetic propagation vectors
k1=(0,0,kz), BaErFeO4 is the first member in this series that shows a phase transition from an incommensurate (
k1 below
TN1) to a commensurate magnetic structure with
k2=(12,0,12) below
TN2. In the crystal structure, all magnetic ions (Fe1, Fe2, Er1, and Er2) are part of chains propagating along the
b axis. Below
TN1, strong antiferromagnetic (AFM) Fe-Fe spin-exchange coupling between square pyramidal (Fe1) and octahedral (Fe2) centers generates a collinear AFM structure with a constant size of the ordered Fe moments and a constant magnetic phase inside each chain of
Fe3+ cations. Exchange coupling between the Fe chains is much weaker. At
TN2, 3d−4f exchange interactions induce an ordered moment at the
Er3+ ions, which results in a change of the direction of the ordered Fe moments from the
b direction (above
TN2) to inside the
ac plane (below
TN2) and a change from an incommensurate (
k1 above
TN2) to a commensurate (
k2 below
TN2) AFM structure. Toward lower temperature,
4f−4f exchange interactions become stronger and create at
TN3 a constant magnetic phase inside each chain of
Er3+ cations. At
TN2 and
TN3, the magnetic susceptibility shows sharp decreases that coincide with large increases of the correlation length of the magnetic structure. The unique magnetic structures of
BaErFeO4 are compared with those of other
BaRFeO4 compounds by considering experimental and theoretical aspects. ©2024 American Physical Society 2024 American Physical Society