Abstract

We report on investigations of the critical magnetic behaviour of GdMg. In this intermetallic ferromagnet the sum of all fourth-order interactions (i.e. biquadratic, three-spin and four-spin interactions) is 50 K and antiferromagnetic at the Curie temperature of T ‖ C=110 K. This has been shown with measurements of the third-order susceptibility χ 3. Although the Curie temperature can be assumed to be defined mainly by bilinear (Heisenberg) interactions, the critical indices for the linear susceptibility χ 1 and the spontaneous magnetization are molecular field like γ= γ′=1, β=0.5. The third-order susceptibility χ 3 is discontinuous at T ‖ C: for T> T ‖ C, χ 3 is finite but for T< T ‖ C it diverges with a critical exponent of one. The ferromagnetic order–disorder transition is therefore weakly first order. At a second critical temperature of T ⊥ N=91 K the rise of an ordered antiferromagnetic component oriented perpendicular to the ferromagnetic one has been reported two decades ago based on neutron scattering investigations. Here we will show that the third order susceptibility χ 3 diverges at T ⊥ N but that the linear susceptibility χ 1 stays finite. This is characteristic for a phase transition driven by the fourth-order interactions. We must therefore assume that the transverse components of the ferromagnetically ordered moments order antiferromagnetically at T ⊥ N. This view is in accordance with measurements of the susceptibility χ ⊥ perpendicular to an applied static magnetic field. As a result, a second-order parameter perpendicular to the spontaneous magnetization is generated by the fourth-order interactions. As a further consequence of the perpendicular moment configuration, the spontaneous longitudinal magnetization reaches only 0.75 of the theoretical saturation value for T→0 and decreases like T 2 with temperature as has been observed for other ferromagnets with fourth-order interactions, such as EuS and CrBr 3.

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