Magnetic moment of the pentaquark $Θ^+(1540)$ as diquark-diquark-antiquark state with QCD sum rules

dc.creatorWang, Zhi-Gang
dc.creatorWan, Shao-Long
dc.creatorYang, Wei-Min
dc.date2005-03-01
dc.date2005-06-27
dc.date.accessioned2026-07-07T12:24:59Z
dc.date.available2026-07-07T12:24:59Z
dc.descriptionIn this article, we study the magnetic moment of the pentaquark state $ Θ^+(1540)$ as diquark-diquark-antiquark ($[ud][ud]\bar{s}$) state with the QCD sum rules in the external weak electromagnetic field (EFSR) and the light-cone QCD sum rules (LCSR) respectively. The numerical results indicate the magnetic moment is about $μ_{Θ^+}=-(0.11\pm 0.02)μ_N$ for the EFSR and $μ_{Θ^+}\approx-(0.1-0.5)μ_N$ for the LCSR. As the values obtained from the EFSR are more stable than the corresponding ones from the LCSR, $μ_{Θ^+}=-(0.11\pm 0.02)μ_N$ is more reliable.
dc.description17 pages, 4 figures, unifing hep-ph/0503007 with hep-ph/0503073 into one article, input parameters changed slightly, add more discussions
dc.identifierhttps://arxiv.org/abs/hep-ph/0503007
dc.identifierhttp://arxiv.org/abs/hep-ph/0503007
dc.identifierEur.Phys.J.C45:201-209,2006
dc.identifierdoi:10.1140/epjc/s2005-02400-1
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/214491
dc.subjectHigh Energy Physics - Phenomenology
dc.titleMagnetic moment of the pentaquark $Θ^+(1540)$ as diquark-diquark-antiquark state with QCD sum rules
dc.typetext

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