GdxEr1−xRh4B4 exhibits superconductivity at some critical temperature Tc followed by the onset of long‐range ferromagnetic ordering at a lower temperature and a loss of superconductivity for x<xc?0.28, where xc is the critical concentration at which superconductivity is suppressed. For x above xc, the compound is no longer superconducting but is still magnetically ordered. We have made ac resistivity R, ac magnetic susceptibility χ, and dc magnetization measurements on samples with x near xc. For x?0.28, the salient features for the R and χ measurements are: (1) In zero external field a sharp maximum in the ac χ (T) and a minimum in R(T) are observed. With a small external dc magnetic field (∼102 Oe), the extrema in χ (T) and R(T) are depressed and smeared considerably with a corresponding shift in the temperature at which the extrema occur. (2) The sample is not superconducting down to 0.6 K. (3) In the presence of a dc magnetic field, a second ac χ peak appears at a slightly higher temperature. (4) The field dependence of the ac susceptibility resembles that of a spin glass. Details of the field dependence of these observations and the nature of these phenomena will be presented.

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