{ "id": "hep-ph/0401192", "version": "v2", "published": "2004-01-24T13:41:07.000Z", "updated": "2004-01-30T17:14:46.000Z", "title": "Pentaquark Symmetries, Selection Rules and another potentially Narrow State", "authors": [ "F. E. Close", "J. J. Dudek" ], "comment": "Revised version, corrects PDF margin problems, minor changes to text", "journal": "Phys.Lett. B586 (2004) 75-82", "doi": "10.1016/j.physletb.2004.02.023", "categories": [ "hep-ph" ], "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 $\\Xi_5$ states in particular can test models of the pentaquarks, recommend study of the relative branching ratios of e.g. $\\Xi^{-}_5 \\to \\Xi^-\\pi^0:\\Xi^0\\pi^-$, and predict that the decay amplitude $\\Xi_5 \\to \\Xi^*\\pi$ 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 $\\Xi_5 \\to \\Lambda K$. The role of Fermi-Dirac symmetry in the $qqqq$ wavefunction and its implications for the width of pentaquarks are briefly discussed. The relative couplings $g^2(\\Theta_Q N K_Q^*)/g^2(\\Theta_Q N K_Q) = 3$ for $Q \\equiv s,c,b$. A further potentially narrow state $\\Lambda$ in {\\bf 8}$_5$ with $J^P = 3/2^+$ is predicted around 1650 MeV.", "revisions": [ { "version": "v2", "updated": "2004-01-30T17:14:46.000Z" } ], "analyses": { "keywords": [ "potentially narrow state", "selection rules", "pentaquark symmetries", "pentaquark models", "chiral soliton models" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "inspire": 643318 } } }