The rate of flux creep over the surface barrier in clean HTSC samples
is found. This rate proves to be significantly different for the cases
of vortex entry and escape (relaxation ''in'' and ''out'', respective
ly). Since a flat surface is topologically similar to the artificial c
olumnar defects, their comparison is useful. The vortex creep over the
surface is equivalent to that over the cylinder defect of radius r >
lambda whereas the radii of real defects obtained so far are of order
xi much-less-than lambda. We discuss the effect of the smallness of de
fect radius on the creep process, which results in very small activati
on energies U at large critical current J(c). The importance of the in
crease of the defect radius is predicted.