I study the normal-to-superconducting (NS) transition within the Ginzb
urg-Landau (GL) model, taking into account the fluctuations in the m-c
omponent complex order parameter psi(alpha), and the vector potential
A in the arbitrary dimension d, for any m. I find that the transition
is of second order and that the previous conclusion of the fluctuation
-driven first-order transition is a possible artifact of the breakdown
of the epsilon-expansion and the inaccuracy of the 1/m-expansion for
physical values epsilon = 1, m = 1. I compute the anomalous ri(d, m) e
xponent at the NS transition, and find eta(3, 1) approximate to - 0.38
. In the m--> infinity limit, eta(d, m) becomes exact and agrees with
the 1/m-expansion. Near d=4 the theory is also in good agreement with
the perturbative E-expansion results for m > 183 and provides a sensib
le interpolation formula for arbitrary d and m.