  We study the magnetic properties of a superconductor in a crystal without $z
\to -z$ symmetry, in particular how the lack of this symmetry exhibits itself.
We show that, though the penetration depth itself shows no such effect, for
suitable orientation of magnetic field, there is a magnetic field discontinuity
at the interface which shows this absence of symmetry. The magnetic field
profile of a vortex in the $x-y$ plane is shown to be identical to that of an
ordinary anisotropic superconductor except for a shift in the $-z$ direction by
${\tilde \kappa} \lambda_x$ (see errata). For a vortex along $z$, there is an
induced magnetization along the radial direction.
