A particular initial state for the construction of the perturbative expansi
on of QCD is investigated. It is formed as a coherent superposition of zero
momentum gluon pairs and shows Lorentz as well as global SU(3) symmetries.
It follows that the gluon and ghost propagators determined by it coincide
with the ones used in an alternative of the usual perturbation theory propo
sed in a previous work. Therefore, the ability of such a procedure to produ
ce a finite gluon condensation parameter already in the first orders of per
turbation theory is naturally explained. It also follows that this state sa
tisfies the physicality condition of the Becchi-Rouet-Stora-Tyutin (BRST) p
rocedure in its Kugo-Ojima formulation. The ERST quantization is done for t
he value alpha = 1 of the gauge parameter where the procedure is greatly si
mplified. Therefore. after assuming that the adiabatic connection of the in
teraction does not take out the state from the interacting physical space,
the predictions of the perturbation expansion, at the value alpha = 1, for
the physical quantities should have meaning. The validity of this conclusio
n solves the gauge dependence indeterminacy remaining in the proposed pertu
rbation expansion.