We consider the local stability of laminar differential rotation in a
weakly magnetized plasma to adiabatic axisymmetric disturbances. Our a
ssumptions are considerably less restrictive than those of previous an
alyses. The angular velocity need not have cylindrical isorotational s
urfaces, and a priori convective stability is not assumed. In an unmag
netized gas, stability under these circumstances would be governed by
the Hoiland criteria. These criteria change qualitatively when even a
weak magnetic field is present. In a magnetized plasma, the new criter
ia for stability have the same general form exhibited by the purely hy
drodynamical case, but with all angular momentum gradients replaced by
angular velocity gradients. Our findings are in accord with those of
Papaloizou & Szuszkiewicz, who, using very different methods, consider
ed the stability of isorotational field configurations. The results pr
esented here thus point very generally to angular velocity gradients,
not angular momentum gradients, as the fundamental stability discrimin
ants in rotating astrophysical plasmas.