Theoretical interpretation of the Ξ(1620)\Xi(1620) and Ξ(1690)\Xi(1690) resonances seen in Ξc+β†’Ξžβˆ’Ο€+Ο€+\Xi_c^+ \to \Xi^- \pi^+ \pi^+ decay

Abstract

We study the Belle reaction Ξc+β†’Ξžβˆ’Ο€+Ο€+\Xi_c^+ \to \Xi^- \pi^+ \pi^+ looking at the mass distribution of Ο€+Ξ\pi^+ \Xi, where clear signals for the Ξ(1620)\Xi(1620) and Ξ(1690)\Xi(1690) resonances are seen. These two resonances are generated dynamically from the interaction in coupled channels of Ο€Ξž,KΛ‰Ξ›,KΛ‰Ξ£\pi \Xi, \bar K \Lambda, \bar K \Sigma and ηΞ\eta \Xi within the chiral unitary approach. Yet, the weak decay process at the quark level, together with the hadronization to produce pairs of mesons, does not produce the Ο€Ο€Ξž\pi \pi \Xi final state. In order to produce this state one must make transitions from the KΛ‰Ξ›,KΛ‰Ξ£\bar K \Lambda, \bar K \Sigma and ηΞ\eta \Xi components to Ο€Ξž\pi \Xi, and this interaction is what produces the resonances. So, the reaction offers a good test for the molecular picture of these resonances. Adding the contribution of the Ξžβˆ—(1530)\Xi^*(1530) and some background we are able to get a good reproduction of the mass distribution showing the signatures of the two resonances as found in the experiment.Comment: 15 pages, 8 figures, 2 tables; v2: discussion added, references added, version to appear in Eur.Phys.J.

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