A hidden-charm pentaquark state in Λb0→J/ψpπ−Λ^0_b \to J/ψp π^- decay

preprint2016arXivOpen access

Abstract

We study here the Λb0→J/ψpπ−Λ_b^0 \to J/ψp π^- reaction in analogy to the Λb0→J/ψpK−Λ^0_b \to J/ψp K^- one, and we note that in both decays there is a sharp structure (dip or peak) in the J/ψpJ/ψp mass distribution around 44504450 MeV, which is associated in the Λb0→J/ψpK−Λ^0_b \to J/ψp K^- experiment to an exotic pentaquark baryonic state, although in Λb0→J/ψpπ−Λ_b^0 \to J/ψp π^- it shows up with relatively low statistics. We analyze the Λb0→J/ψpπ−Λ^0_b \to J/ψp π^- interaction along the same lines as the Λb0→J/ψpK−Λ^0_b \to J/ψp K^- one, with the main difference stemming from the reduced Cabibbo strength in the former and the consideration of the π−pπ^-p final state interaction instead of the K−pK^-p one. We find that with a minimal input, introducing the π−pπ^-p and J/ψpJ/ψp interaction in SS-wave with realistic interactions, and the empirical PP-wave and DD-wave contributions, one can accomplish a qualitative description of the π−pπ^-p and J/ψpJ/ψp mass distributions. More importantly, the peak structure followed by a dip of the experimental J/ψpJ/ψp mass distribution is reproduced with the same input as used to describe the data of Λb0→J/ψpK−Λ^0_b\rightarrow J/ψp K^- reaction. The repercussion for the triangular singularity mechanism, invoked in some works to explain the pentaquark peak, is discussed.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.