The first part of my talk is a very brief review of the Pomeron and ho
w it is described in perturbative QCD by the BFKL equation. The BFKL P
omeron differs from that observed in total cross sections, but there i
s same hope that it may be observed in perturbative high energy proces
ses. A particular application of the BFKL equation is to the evolution
of the gluon at low x and the consequences that this has on the struc
ture functions, F-2 and F-L. Finally I discuss the CCFM equation which
contains both the BFKL and more traditional DGLAP forms of gluon evol
ution.