Abstract
The addition of pion contributions to symmetric-quark-model predictions of baryon magnetic moments is shown to lead to considerable improvement in quantitative agreement with experiment. The added variation of the nucleon quark moment in the Ξ hyperons, interpreted as a relativistic effect, removes all salient difficulties in reconciling the quark model with accurate magnetic-moment measurements. The pion probability required in the nucleon wave function is found to be (18±7)%.