Abstract

In this study, we measure the magnetic field and temperature variations of the magnetization \(M(H,T)\) of the cubic chiral compound EuPtSi and extensively investigate the magnetic phase transitions in a wide temperature range down to 60 mK. The incommensurate–commensurate transition at \(T_{\text{N}}^{*} \simeq 2.5\) K in the helical state, which has not been observed in transport or thermodynamic measurements, is exclusively detected in M(T) for H || 〈111〉. \(T_{\text{N}}^{*}\) shows a rapid decrease in H. For H || [100] and [111], M(H) at T < 100 mK showed that the helical q vectors are depinned from the preferred orientations at \(H \gtrsim 10\) kOe and gradually rotate toward the field directions as H increases. The skyrmion lattice phase (A-phase) field-induced in H || 〈111〉 only above 0.4 K in equilibrium conditions can be created at 60 mK under field cooling, with a sharp tilted plateau structure developing in M(H) of the A-phase. A similar metastable state is also created below 100 mK for the A′ phase induced by H || 〈100〉 at \(T \gtrsim 0.3\) K in equilibrium conditions. The magnetic phase diagrams established for the three directions [111], [110], and [100] are highly anisotropic and discussed herein on the basis of the q vectors rather strongly pinned to the lattice and transform under the lattice symmetry operations.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call