  Within the context of the Abelian Projection of QCD monopole-like quantum
excitations of gauge fields are studied. We start with certain classical
solutions, of the SU(2) Yang-Mills field equations, which are not monopole-like
and whose energy density diverges as $r \to \infty$. These divergent classical
solutions are then quantized using a modified version of Heisenberg's
quantization technique for strongly interacting, nonlinear fields. The modified
Heisenberg quantization technique leads to a system of equations with mixed
quantum and classical degrees of freedom. By applying a Feynman path
integration over the quantum degrees of freedom the quantum-averaged solution
gives a nondivergent, monopole-like configuration after Abelian Projection.
