Small regions of differently strong superconducting interaction have been detected by measuring the penetration depth Δλ(T,f,B
ac) and the losses ΔR(T,f,B
ac) as deviation from the BCS theory of homogeneous materials. For Nb two deviations are most pronounced: a step-like increase in Δλ(T) and ΔR(T) at

K and an enhanced slope λ
0= dλ/dy
![[y = 1/\\sqrt {1-(T/T_{c})^{4}}]](/images/tex/9597.gif)
for T > T*. The step Δλ
0around 7 K shows the transition of regions to the normal state, which then for T > T* yield an enhanced slope λ
0, as explained by proximity effect theory. For Nb
3Sn no such deviations from the BCS theory could be detected, showing together with λ
0= 170 nm its homogeneity. For thinned Nb
3Sn layers the underlaying Nb shows up as step at 9.2 K, which is used to evaluate the mean thickness of the Nb
3Sn layer.