Pentaquark Symmetries, Selection Rules and another potentially Narrow State

Abstract

We identify essential differences between the pentaquark and chiral soliton models of \10bar$_5$ and {\bf 8}$_5$ pentaquarks and conventional {\bf 8}$_3$ states, which are experimentally measurable. We show how the decays of $Ξ_5$ states in particular can test models of the pentaquarks, recommend study of the relative branching ratios of e.g. $Ξ^{-}_5 \to Ξ^-π^0:Ξ^0π^-$, and predict that the decay amplitude $Ξ_5 \to Ξ^*π$ is zero at leading order in pentaquark models for any mixture of \10bar and the associated {\bf 8}$_5$. We also include a pedagogic discussion of wavefunctions in the pentaquark picture and show that pentaquark models have this {\bf 8}$_5$ with $F/D=1/3$, in leading order forbidding $Ξ_5 \to ΛK$. The role of Fermi-Dirac symmetry in the $qqqq$ wavefunction and its implications for the width of pentaquarks are briefly discussed. The relative couplings $g^2(Θ_Q N K_Q^*)/g^2(Θ_Q N K_Q) = 3$ for $Q \equiv s,c,b$. A further potentially narrow state $Λ$ in {\bf 8}$_5$ with $J^P = 3/2^+$ is predicted around 1650 MeV.