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{α_s^0} linear potential for color singlet $q\bar q$ and $qqq$ states. These states are Poincaré 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 $α_s(0)\simeq 0.5$, allowing reasonable convergence. The \order{α_s^0} bound states have a sea of $q\bar q$ pairs, while transverse gluons contribute only at \order{α_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 $D=3+1$.

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