Abstract
Strong disagreement between experimental hyperon magnetic moments and simple model predictions is exhibited in the function R(p,Σ+,Ξ)=3(μpμΣ+)(μΞμΞ0)=2.7±0.8, an order of magnitude larger than the broken-SU(6) prediction 0.34. This is shown to imply quenching of contributions of nonstrange quarks in strange-baryon magnetic moments, relative to contributions in the nucleon. The model-independent analysis includes SU(6)-symmetry breaking, configuration mixing, relativistic corrections, and quark-diquark correlations.