The pseudogap phenomenon in the cuprates can be explained by an intrinsic i
nhomogeneity of the samples. At temperatures above the superconducting resi
stive transition but below the temperature at which the pseudogap disappear
s, the sample contains superconducting islands embedded in a normal matrix.
As a result, the normal resistance coexists with the gap structure, and th
ere is a splitting of the resistive and Meissner traditions.