  The semi-Dirac semi-Weyl semi-metal has been of interest in recent years due
to its naturally occurring point Fermi surface and the associated exotic
band-structure near the Fermi surface, which is linear (graphene-like) in one
direction of the Brillouin zone, but quadratic in a direction perpendicular to
it. In this paper the effect of a magnetic adatom impurity in a semi-Dirac
system is studied. As in a metal, the magnetic impurity in a semi-Dirac system
interacts with the sea of conduction electrons and gives rise to magnetism. The
transition of the semi-Dirac system from the non-magnetic to the magnetic phase
is studied as a function of the impurity energy, the strength of hybridization
between the impurity and the bath as well as that of the electron electron
interaction at the impurity atom. The results are compared and contrasted with
those of graphene and ordinary metal. Since the semi-Dirac and the Dirac
dispersion share similar features,e.g, both are particle hole symmetric and
linear in one direction, the two systems share resemblances in their
characteristics in the presence of a magnetic impurity. But some features are
unique to the semi-Dirac dispersion.
