Confinement with Perturbation Theory, after All?

I call attention to the possibility that QCD bound states (hadrons) could be derived using rigorous Hamiltonian, perturbative methods. Solving Gauss’ law for $A^0$ with a non-vanishing boundary condition at spatial infinity gives an \order{\alpha_s^0} linear potential for color singlet $q\bar{q}$ and $qqq$ states. These states are Poincar'e and gauge covariant and thus can serve as initial states of a perturbative expansion, replacing the conventional free $in$ and $out$ states. The coupling freezes at ${\alpha }_s(0)\simeq 0.5$, allowing reasonable convergence. The \order{\alpha_s^0} bound states have a sea of $q\bar{q}$ pairs, while transverse gluons contribute only at \order{\alpha_s}. Pair creation in the linear $A^0$ potential leads to string breaking and hadron loop corrections. These corrections give finite widths to excited states, as required by unitarity. Several of these features have been verified analytically in $D=1+1$ dimensions, and some in $D=3+1$.