I calculate the anomalous dimension governing the Q(2) evolution of the glu
on (and structure functions) coming from the running coupling BFKL equation
. This may be expressed in an exact analytic form, up to a small ultraviole
t renormalon contribution, and hence the corresponding splitting function m
ay be determined precisely. Rather surprisingly it is most efficient to exp
and the gluon distribution in powers of alpha(s)(Q(2)) rather than use the
traditional expansion where all orders of alpha(s)ln(1/x) are kept on an eq
ual footing. The anomalous dimension is very different from that obtained f
rom the fixed coupling equation, and leads to a powerlike behaviour for the
splitting function as x --> 0 which is far weaker, i.e. similar to x(-0.2)
The NLO corrections to the anomalous dimension are rather small. unlike th
r fixed coupling case, and a stable perturbative expansion is obtained. (C)
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