T. Foglizzo
During the core collapse of a rotating massive star, the standing accretion shock instability (SASI) favours the development of non-axisymmetric motions, which can imprint specific frequency signatures on the neutrino and gravitational wave signals. This study establishes analytical approximations for the eigenfrequencies of the dominant SASI modes. It also explains the physical mechanism responsible for the further destabilisation of prograde SASI modes by differential rotation. A perturbative analysis was used to calculate the eigenfrequencies of a stalled accretion shock in spherical geometry while taking into account the rotation of the collapsing stellar core. The formulation of the perturbative equations as a self-forced oscillator was extended to include the effect of differential rotation and to interpret the results physically. The oscillation frequency of the dominant mode weakly depends on the detailed formulation of neutrino emission if the shock radius exceeds ∼ 1.5 times the radius r_∇ of maximum deceleration. We obtained analytical expressions for the one- and two-armed spiral modes with a 10% accuracy in this regime. The effect of differential rotation on SASI is explained by the role of phase mixing between the advective forcing and the acoustic structure. The radial wavelength of vorticity perturbations associated with the prograde mode is increased by differential rotation, leading to a better phase match with the large radial scale of the acoustic structure. Even when rotation is too modest to involve a corotation radius, its adverse effect on phase mixing can be significant at a small radius due to the steep inwards increase of the rotation frequency ∝ 1/r^2 in the region of stationary accretion. In the regime of faster rotation involving a corotation radius, the stationary phase approximation sheds light on the dominant advective-acoustic coupling, which is located between the corotation zone and the shock.