Neutron diffraction, polarized neutron transmission, and small angle neutron scattering have been used to investigate the crystal structure and nature of the magnetic order in a polycrystalline sample of $\mathrm{Ru}{\mathrm{Sr}}_2{\mathrm{Eu}}_{1.2}{\mathrm{Ce}}_{0.8}{\mathrm{Cu}}_2{\mathrm{O}}_{10}$. The sample was made with the Eu-153 (98.8%) isotope to reduce the high neutron absorption for the naturally occurring element. Full refinements of the crystal structure, space group $I4∕mmm$, are reported. At low temperatures only a single magnetic peak is clearly observed in a relatively wide angular range. A sharp spin reorientation transition (SRT) is observed around $35\mathrm{K}$, close to the superconducting transition temperature $(T_c\sim 40\mathrm{K})$. Between the spin reorientation temperature and the Neel temperature of $59\mathrm{K}$, additional magnetic reflections are observed. However, none of these can be simply indexed on the chemical unit cell, either as commensurate peaks or simple incommensurate magnetism, and the paucity of reflections at low $T$ compels the conclusion that these magnetic Bragg peaks arise from an impurity phase. X-ray and neutron diffraction on the pressed pellet both show that the sample does not appear to contain substantial impurity phases, but it turns out that the magnetic impurity peaks exhibit strong preferred orientation with respect to the pellet orientation, while the primary phase does not. We have been unable to observe any magnetic order that can be identified with the ruthenate-cuprate system.

• Received 13 December 2006

DOI:https://doi.org/10.1103/PhysRevB.76.014519