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Materials Data on SrYb by Materials Project

SrYb crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Sr is bonded to six equivalent Sr and six equivalent Yb atoms to form SrSr6Yb6 cuboctahedra that share corners with eighteen equivalent SrSr6Yb6 cuboctahedra, edges with six equivalent SrSr6Yb6 cuboctahedra, edges with twelve equivalent YbSr6Yb6 cuboctahedra, faces with eight equivalent SrSr6Yb6 cuboctahedra, and faces with twelve equivalent YbSr6Yb6 cuboctahedra. All Sr–Sr bond lengths are 4.14 Å. All Sr–Yb bond lengths are 4.05 Å. Yb is bonded to six equivalent Sr and six equivalent Yb atoms to form YbSr6Yb6 cuboctahedra that share corners with eighteen equivalent YbSr6Yb6 cuboctahedra, edges with six equivalent YbSr6Yb6 cuboctahedra, edges with twelve equivalent SrSr6Yb6 cuboctahedra, faces with eight equivalent YbSr6Yb6 cuboctahedra, and faces with twelve equivalent SrSr6Yb6 cuboctahedra. All Yb–Yb bond lengths are 4.14 Å.

36 MATERIALS SCIENCE↗

Impact of Erbium Doping in the Structural and Magnetic Properties of the Anisotropic and Frustrated SrYb 2 O 4 Antiferromagnet

We present a systematic study of the structural and magnetic properties of a series of powder samples of SrYb 2-x Er x O 4 with different Yb/Er concentrations. Magnetometry and neutron diffraction have been used to study the magnetic ground states of the compound series, while inelastic neutron scattering was used to investigate the crystal field excitations for a chosen concentration. These results show that the crystal structure remains the same for all compositions, while the lattice parameters increase linearly with the Er content. All compounds showed some type of magnetic transition below 1 K, however, both the magnetic structure and nature of the phase transition vary throughout the series. The samples present a non-collinear magnetic structure with the moments lying on the ab plane for low Er content. For high Er content, the magnetic structure is collinear with the moments aligned along the c-axis. A critical concentration is found where there is a bifurcation between zero-field and field-cooled magnetic susceptibility. This irreversible process could be due to the random mixture of single-ion magnetic anisotropies.

36 MATERIALS SCIENCE↗