Figure 3.
The same as in Fig. 1 for the case of constant angular momentum (κ2 = 0; n = 4) (case 3). Both the Rayleigh and MRI branches have infinite derivatives dω2/dk2 at k2 = 0.
The same as in Fig. 1 for the case of constant angular momentum (κ2 = 0; n = 4) (case 3). Both the Rayleigh and MRI branches have infinite derivatives dω2/dk2 at k2 = 0.
