  In light of the developments of the chiral constituent quark model
($\chi$CQM) in studying low energy hadronic matrix elements of the ground-state
baryons, we have extended this model to investigate their transition
properties. The magnetic moments of transitions from the $J^P=\frac{3}{2}^+$
decuplet to $J^P=\frac{1}{2}^+$ octet baryons have been calculated with
explicit valence quark spin, sea quark spin and sea quark orbital angular
momentum contributions. Since the experimental data is available for only a few
transitions, we have compared our results with the results of other available
models. The implications of other complicated effects such as chiral symmetry
breaking and SU(3) symmetry breaking arising due to confinement of quarks have
also been discussed.
