The doping dependence of the superconducting state for the 2D one-band
Hubbard Hamiltonian is determined. By using an Eliashberg-type theory, we find
that the gap function Δk has a dx2−y2 symmetry in momentum
space and Tc becomes maximal for 13% doping. Since we determine the
dynamical excitations directly from real frequency axis calculations, we obtain
new structures in the angular resolved density of states related to the
occurrence of {\it shadow states} below Tc. Explaining the anomalous
behavior of photoemission and tunneling experiments in the cuprates, we find a
strong interplay between d-wave superconductivity and dynamical spin
fluctuations.Comment: 4 pages (REVTeX) with 4 figures (Postscript