Influence of Dy³⁺ environment on magnetic anisotropy and magnetocaloric effect in Dy₃⁢B₂⁢C₃⁢O₁₂ (B=In, Sc, Te ; C=Ga, Al, Li) garnets
F. Damay, S. Petit, D. Sheptyakov, C. V. Colin, E. Suard, S. Rols, J. Embs, U. Stuhr, D. Bounoua, O. Demortier, and C. Decorse, Phys. Rev. B 109 (2024) 014419
 

In the framework of the general phase diagram published recently for a pseudospin S = 1/2 on a hyperkagome network [Kibalin et al., Phys. Rev. Res. 2, 033509 (2020)], four Dy₃B₂C₃O₁₂ garnets with different species on the B and C sites, namely, Dy₃Sc₂Al₃O₁₂ (DyScAl), Dy₃Te₂Li₃O₁₂ (DyTeLi), Dy₃Sc₂Ga₃O₁₂ (DyScGa), and Dy₃In₂Ga₃O₁₂ (DyInGa), have been studied by neutron powder diffraction and inelastic neutron scattering, to investigate the impact of B and C substitutions on the Dy³⁺ dodecahedral oxygen environment and crystal field, and thus on the Dy³⁺ spin magnetic anisotropy. In the four compounds, the magnetic ground state is a multiaxis antiferromagnetic order similar to that of Dy₃Al₅O₁₂, characterized by an ordered moment close to the theoretical maximum, similar to 6 mu B. The gap between the ground state and the first excited crystal electric field level varies from similar to 3.2 meV (DyInGa) up to 11.2 meV (DyScAl), confirming the rather strong Ising character of the Dy³⁺ moment in those garnets. For a better understanding of the impact of the distortion of the oxygen environment on the Dy³⁺ magnetic anisotropy, point-charge calculations were then performed, mapping a magnetic anisotropy diagram versus a wide range of distortions. Results show that Ising-like behaviors mostly predominate, associated with large gx, gy, or gz Lande values, whose stable area is determined by the shape of the DyO₈ cage. Magnetic entropy calculations confirm that the magnetocaloric effect increases sharply near those boundaries and validate the use of dysprosium garnets for low temperature, low magnetic field adiabatic demagnetization refrigeration cryostats.