The $J^P=1^+$ $ud\bar s\bar s$ Tetraquark

dc.creatorCui, Ying
dc.creatorChen, Xiao-Lin
dc.creatorDeng, Wei-Zhen
dc.creatorZhu, Shi-Lin
dc.date2005-11-11
dc.date.accessioned2026-07-07T10:29:47Z
dc.date.available2026-07-07T10:29:47Z
dc.descriptionUsing the color-magnetic interaction Hamiltonian with SU(3) flavor symmetry breaking, we perform a schematic study of the masses of the $J^P=1^+$ tetraquarks in the anti-decuplet representation. After diagonalizing the mass matrix, we find the $ud\bar s\bar s$ tetraquark lies around 1347 MeV. It decays into $K^+K^0π^0, K^+K^+π^-, K^0K^0π^+$ via P-wave. The dual suppression from the not-so-big three-body phase space and P-wave decay barrier may render this exotic state rather narrow. Future experimental exclusion of this state will cast doubt on the validity of applying the simple color-magnetic Hamiltonian to the multiquark system.
dc.identifierhttps://arxiv.org/abs/hep-ph/0511150
dc.identifierhttp://arxiv.org/abs/hep-ph/0511150
dc.identifierPhys.Rev.D73:014018,2006
dc.identifierdoi:10.1103/PhysRevD.73.014018
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/177930
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectNuclear Experiment
dc.subjectNuclear Theory
dc.titleThe $J^P=1^+$ $ud\bar s\bar s$ Tetraquark
dc.typetext

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