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The dynamical breaking of chiral symmetry in QCD is caused by nonperturbative interactions on a scale rho ~ 0.3 fm, much smaller than the hadronic size R ~ 1 fm.
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This approach is fundamentally different from models in which a “pion cloud” is generated by leading–order perturbation theory in the pion–quark or pion–nucleon coupling without any parametric basis. The only instance where a perturbative treatment of the pion coupling in such models is justified is in a space–time formulation at large distances (impact parameter representation), where the pions have wavelenghts ∼ 1 / M π \sim 1/M_{\pi} and the approach becomes equivalent to chiral perturbation theory; see: M. Strikman, C. Weiss, Phys. Rev. D80
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