We discuss the Hamiltonian formulation of the Schwinger proper-time me
thod of calculating Green functions in gauge theories. Instead of calc
ulating Feynman diagrams, we solve the corresponding Dyson-Schwinger e
quations. We express the solutions in terms of vertex operators, which
consist of the zero modes of the vertex operators appearing in string
theories. We show how color decomposition arises in this formalism at
tree level. At the one-loop level, we arrive at expressions similar t
o those obtained in the background gauge. In both cases, no special ga
uge-fixing procedure is needed.