Magnetocaloric effect for the topological semimetal Co3Sn2S2 due to the antiferromagnetic coupling of the bulk and surface spin-polarized phases

Abstract

We experimentally investigate magnetocaloric effect for the topological magnetic Weyl semimetal Co${}_3$Sn${}_2$S${}_2$ in a wide temperature range. The isothermal magnetic entropy change $\Delta$S is calculated from the experimental magnetization curves by using Maxwell relation. In addition to the expected $\Delta$S peak at the Curie temperature $T_C$, we obtain another one at the temperature $T_{inv}$ of the hysteresis inversion, which is the main experimental result. The inverted hysteresis usually originates from the antiferromagnetic coupling between two magnetic phases. For Co${}_3$Sn${}_2$S${}_2$ topological magnetic Weyl semimetal these phases are the ferromagnetic bulk and the spin-polarized topological surface states. Thus, the pronounced magnetocaloric effect at $T_{inv}$ is determined by the bulk magnetization switching by the exchange bias field of the surface spin-polarizad phase, in contrast to the ferromagnetic–paramagnetic transition at the Curie temperature $T_C$. For possible applications of magnetocaloric effect, Weyl semimetals open a new way to transfer from ferromagnetically ordered systems to the two-phase ones with the antiferromagnetic coupling between the bulk and surface spin-polarized phases without loss of efficiency. As the advantage we can point the higher reversibility and smaller energy costs at $T_{inv}$.