“…Using a two-state model, Lipkin showed 41 that the mass eigenstates of two pentaquarks (e.g., mixtures of the Jaffe-Wilczek model and the diquark-triquark model) can mix, resulting in one coupling strongly to KN decay (with a wide width) and one decoupling (with a narrow width). Another approach, this time with mixing between the octet and the 10, shown by Praszalowicz 40 , can suppress the width by a correction factor that depends on the value of the pion-nucleon Σ term. From a completely different angle, using the QCD string model, Suganuma et al showed 42 that the pentaquark does not just "fall apart" as predicted by the quark model, but must overcome a sizeable potential barrier to decay into a KN final state.…”