The standard phenomenology of the soft pomeron in hadron-hadron intera
ctions is recalled briefly. The model is confronted with the HERA data
for the total photoproduction cross section, deep inelastic scatterin
g, diffractive vector meson photoproduction and diffractive electropro
duction of vector mesons. Although much of the data can be explained b
y the model, there are some aspects of the HERA data which require a m
ore rapid variation with energy than can be incorporated. It is argued
that the perturbative (BFKL) pomeron cannot give a sufficiently large
contribution to explain these observations. Possible nonperturbative
solutions to this problem are indicated.