Theoretical study on Ξ›c+β†’Ξ›K+KΛ‰0\Lambda_c^+ \to \Lambda K^+\bar{K}^0 decay and Ξžβˆ—(1690)\Xi^*(1690) resonance

Abstract

We present a theoretical study of Ξžβˆ—(1690)\Xi^*(1690) resonance in the Ξ›c+β†’Ξ›K+KΛ‰0\Lambda_c^+ \to \Lambda K^+ \bar{K}^0 decay, where the weak interaction part proceeds through the Cabibbo-favored process cβ†’s+udΛ‰c \to s + u\bar{d}. Next, the intermediate two mesons and one baryon state can be constructed with a pair of qqΛ‰q\bar{q} with the vacuum quantum numbers. Finally, the Ξžβˆ—(1690)\Xi^*(1690) is mainly produced from the final state interactions of KΛ‰Ξ›\bar{K}\Lambda in coupled channels, and it is shown in the KΛ‰Ξ›\bar{K}\Lambda invariant mass distribution. Besides, the scalar meson a0(980)a_0(980) and nucleon excited state Nβˆ—(1535)N^*(1535) are also taken into account in the decaying channels K+KΛ‰0K^+\bar{K}^0 and K+Ξ›K^+\Lambda, respectively. Within model parameters, the K+KΛ‰0K^+ \bar{K}^0, KΛ‰0Ξ›\bar{K}^0 \Lambda and K+Ξ›K^+ \Lambda invariant mass distributions are calculated, and it is found that our theoretical results can reproduce well the experimental measurements, especially for the clear peak around 16901690 MeV in the KΛ‰Ξ›\bar{K}\Lambda spectrum. The proposed weak decay process Ξ›c+β†’Ξ›K+KΛ‰0\Lambda_c^+ \to \Lambda K^+ \bar{K}^0 and the interaction mechanism can provide valuable information on the nature of the Ξžβˆ—(1690)\Xi^*(1690) resonance.Comment: 9 pages, 5 figure

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