$Ω^{-}$, $Ξ^{* -}$, $Σ^{* -}$ and $Δ^{-}$ decuplet baryon magnetic moments

Details $Ω^{-}$, $Ξ^{* -}$, $Σ^{* -}$ and $Δ^{-}$ decuplet baryon magnetic moments $Ω^{-}$, $Ξ^{* -}$, $Σ^{* -}$ and $Δ^{-}$ decuplet baryon magnetic moments

2009-11-25

arxiv.org/abs/0911.4756v5

Phys.Rev.C82:015208,2010; Erratum-ibid.C83:059901,2011

Physics

High Energy Physics

High Energy Physics - Phenomenology

11 pages.V5 "This research" column of Table I. modified as all results must be in nuclear magneton units. In Eq.~(35), factor

Scientific paper

10.1103/PhysRevC.82.015208 10.11

The properties of the ground state $U$-Spin $={3/2}$ baryon decuplet magnetic moments $\Delta^{-}$, $\Xi^{* -}$, $\Sigma^{* -}$ and $\Omega^{-}$ and their ground state spin 1/2 cousins $p$, $n$, $\Lambda$, $\Sigma^{+}$, $\Sigma^{0}$, $\Sigma^{-}$, $\Xi^{+}$, and $\Xi^{-}$ have been studied for many years with a modicum of success. The magnetic moments of many are yet to be determined. Of the decuplet baryons, only the magnetic moment of the $\Omega^{-}$ has been accurately determined. We calculate the magnetic moments of the \emph{physical} decuplet $U$-Spin $={3/2}$ quartet members without ascribing any specific form to their quark structure or intra-quark interactions.

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