Theoretical description of the decays $Î_b \to Î^{(\ast)}(\frac12^\pm,\frac32^\pm) + J/Ï$
arXiv:1705.07299 · doi:10.1103/PhysRevD.96.013003
Abstract
We calculate the invariant and helicity amplitudes for the transitions $Î_b~\to~Î^{(\ast)}(J^P)~+~J/Ï$ where the $Î^{(\ast)}(J^P)$ are $Î(sud)$-type ground and excited states with $J^P$ quantum numbers $J^P=\frac12^{\pm},\frac32^{\pm}$. The calculations are performed in the framework of a covariant confined quark model previously developed by us. We find that the values of the helicity amplitudes for the $Î^\ast(1520,\,\frac32^-)$ and the $Î^\ast(1890,\,\frac32^+)$ are suppressed compared with those for the ground state $Î(1116,\,\frac12^+)$ and the excited state $Î^\ast(1405,\,\frac12^-)$. This analysis is important for the identification of the hidden charm pentaquark states $P_c^+(4380)$ and $P_c^+(4450)$ which were discovered in the decay chain $Î_b^0~\to~P_c^+(~\to~p~J/Ï)~+~K^- $ because the cascade decay chain $Î_b~\to~Î^\ast(\frac32^\pm)(~\to~pK^-)~+~J/Ï$ involves the same final state.
15 pages, 4 figures. Minor corrections done