Abstract
The impurity contribution to the resistivity in zero field Δρ(T) of dilute hexagonal single crystals of ZnMn, CdMn and MgMn has been studied in the mK range on samples cut parallel (‖) and perpendicular (⊥) to thec-axis, using a SQUID technique for the measurements. Typical spin glass behavior is found in Δρ⊥(T) as well as Δρ‖(T) for all alloys, with Kondo like logarithmic increases at higher temperatures and maxima atT m at lower temperatures, indicating the influence of impurity interactions. The differences in the corresponding isotropic resistivity Δρpoly(T) between the three systems can qualitatively be understood within the framework of a theoretical model by Larsen, describing Δρ(T) as a function of universal quantitiesT/T K and ΔRKKY/T K , where ΔRKKY is the RKKY-interaction strength andT K the Kondo temperature. With respect to the two lattice directions studied, the behavior of Δρ⊥(T and Δρ‖(T is anisotropic in the Kondo regime as well as in the range where ordering becomes important. While the anisotropy in the Kondo slope can be understood by an anisotropic unitarity limit, the understanding of the anisotropy in region where impurity interactions are important remains problematic.
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For a valence difference of ΔZ=2 of the present system a value δv=π/2 cannot be achieved
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Dedicated to Prof. Dr. S. Methfessel on the occasion of his 60th birthday
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Albrecht, H., Meierling, H., Wassermann, E.F. et al. Anisotropy of the low temperature resistivity of hexagonal single crystalline spin glass systems. Z. Physik B - Condensed Matter 49, 213–220 (1982). https://doi.org/10.1007/BF01313029
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DOI: https://doi.org/10.1007/BF01313029