The relevance of the self-field for the ‘peak effect’ in the transportJc(H) of iron-sheathed MgB2wires

A ferromagnetic sheath around a superconducting wire results in an unusual transport J c ( H ). For the field perpendicular to the current, there is a plateau in J c ( H ) at high temperatures and intermediate fields. This plateau develops into a peak at lower temperatures—resembling a 'peak effect'. A model based on cancellation of the self-field of the current and the external field within the iron sheath was proposed for the explanation of the plateau in J c ( H ). We test this model in three key experiments. Firstly, we show that the form of J c ( H ) for round MgB 2 /Fe wires is strongly temperature dependent. This is in contradiction with the model, because the properties of the iron sheath do not change in the measured temperature range. However, the temperature dependence of J c might still account for the change of J c ( H ). Secondly, the model requires a substantial component of the self-field to be parallel to the external field. Our measurements of J c ( H ) for a field parallel to the current show a peak in J c ( H ) at high temperatures and a pronounced plateau at low temperatures. The model cannot explain this because the self-field and external field are perpendicular in this experiment. Thirdly, the iron sheath was made thinner on one side of the wire, which should produce an asymmetry in J c ( H ) in the model for two different orientations of the external field. Such asymmetry was not observed. These experiments show that the effect of the self-field is of much lower importance than an as yet unknown effect that results in the observed plateau and peak in J c ( H ). Such an effect is likely to be based on a specific interaction between the superconductor and ferromagnet, perhaps similar to the overcritical state effect.