Fig. 3: Sclottmann’s scaling and magnetoresistivity.
a Normalized resistivity as a function of magnetic field at different temperatures T between 2 K and 60 K. The resistivity has been measured along the ab plane and normalised to the resistivity measured for each temperature with no applied magnetic field. b Normalized magnetoresistivity as a function of \(\ln (B/{B}^{* })\) for fields between −5 T and 5 T and temperatures up to 35 K. The fit parameter B* is the scaling field, discussed in the `Magnetic field dependence of the Kondo effect: Schlottmann’s scaling' subsection of the Results. The theoretically expected curve35 is marked by a red dashed line. Inset to (b) Scaling field B*(T) obtained from the fit of the normalized resistivities to the theoretical curve for temperatures from 2 K up to 35 K. The error bars represent the values of the scaling field within which the coefficient of determination between the theoretical curve and the scaled experimental data is higher or equal than 0.95.
