Abstract

There are experimental evidences for the existence of narrow states Θ+Θ^+ and ΘcΘ_c with the same quantum numbers of uuddsˉuudd\bar s and uuddcˉuudd\bar c pentaquarks and also NK(∗)NK^{(*)} and ND(∗)ND^{(*)} molecular states. Their masses deviate from many theoretical estimates of the pure pentaquark and molecular states. In this work we study the possibility that the observed Θ+Θ^+ and ΘcΘ_c are mixtures of pure pentaquark and molecular states. The mixing parameters are in general related to non-perturbative QCD which are not calculable at present. We determine them by fitting data from known states and then generalize the mechanism to ΘbΘ_b to predict its mass and width. The mixing mechanism can also naturally explain the narrow width for Θ+Θ^+ and ΘcΘ_c through destructive interferences, even if the pure pentaquark and molecular states have much larger decay widths. We also briefly discuss the properties of the partner eigenstates of Θ+Θ^+ and ΘcΘ_c and the possibility of experimentally observe them. Moreover, probable consequences of multi-state mixing are also addressed.

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