Search

Using the new polarized neutron diffraction (PND) setup at MLZ the spin reorientation transition in the magnetocaloric orthoferrite HoFeO3 was studied at different wavelength. The various experiments provided reproducible results demonstrating high reliability of the used setup. We show that during the phase transition at TSR=53 K in an external magnetic field applied along crystal c-axis, the ordered magnetic moment of the Fe sublattice rotates from the crystallographic direction b to a not just in the ab plane, but through z axis. This means that the applied field breaks the orthorhombic symmetry allowing some magnetization parallel to z within a short temperature region. Interestingly, this is the same temperature region where large magnetocaloric effect for HoFeO3 was previously reported. A general model of the magnetic structure of HoFeO3, unconstrained by the orthorhombic symmetry, would allow the magnitudes and directions of the moments on each of the 8 magnetic sublattices in the unit cell to be independent of one-another, leading to 24 independent magnetic parameters. PND measurements were used to determine the absolute sign of the Dzyaloshinskii-Moriya interaction (DMI) in the ab plane for the Fe magnetic sublattice at 65 K. DMI plays an important role in the energy balance of the system.

The anisotropy of thermal conductivity k in single crystals YBa2Cu3O7 has been studied. The temperature dependence of k in c-direction is well described by the lattice thermal conductivity ( T max =60 K ; k max =4 W / mK ; T D =140 K ) . The precise measurements reveal the hysteretic behavior of out-of-plane thermal conductivity. In ab-direction the upturn in k for temperatures below Tc is observed and temperatures of thermal conductivity peaks in ab- and c-direction coincide. Theoretical analysis suggests a model in which an observed peak below Tc in thermal conductivity for ab-direction is ascribed to a quasiparticle contribution.