We calculate the one-electron Green's function of the Hubbard model on
the square lattice using a spin-rotation invariant six-slave boson re
presentation. In the strong coupling regime its spectrum splits off in
to a quasi particle peak, and a lower and an upper incoherent branch,
which we focus on, using a functional integral formulation. By includi
ng Gaussian fluctuations around a paramagnetic saddle-point, we obtain
the main contributions to G as the graphs which are of lowest order i
n tile fluctuations, in the strong coupling regime. The k-dependence o
f the weight of the upper band shows tile physically expected behavior
. We also find that its total weight quickly decreases away from half-
filling under an increase of the hole doping.