We use the finite temperature AdS/CFT approach to demonstrate logarithmic b
roadening of the confining QCD(3) flux tube as a function of quark separati
on. This behavior indicates that, unlike lattice QCD, there is no roughenin
g transition in the AdS/CFT formulation, which raises the interesting possi
bility of extrapolating strong coupling results to weak couplings by the us
e of resummation techniques. In the zero-temperature non-confining limit, w
e find that this logarithmic broadening of the field strength distribution
is absent. Our results are obtained numerically at strong couplings, in the
supergravity approximation.