  The mass modifications of the light vector mesons ($\omega$, $\rho$ and
$\phi$) are investigated in asymmetric nuclear matter in the presence of strong
magnetic fields, using a QCD sum rule approach. These are computed from the
medium modifications of the non-strange and strange light quark condensates as
well as scalar gluon condensate. The quark and gluon condensates are calculated
from the medium changes of the scalar fields (non-strange and strange) and a
scalar dilaton field in the magnetized nuclear matter, within a chiral SU(3)
model. The scalar dilaton field within the model breaks the scale invariance of
QCD and simulates the gluon condensate. The anomalous magnetic moments for the
nucleons are taken into account in the present study.
