2008
DOI: 10.1086/587732
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Effect of Rotation on the Stability of a Stalled Cylindrical Shock and Its Consequences for Core‐Collapse Supernovae

Abstract: A perturbative analysis is used to investigate the effect of rotation on the instability of a steady accretion shock (SASI) in a simple toy model, in view of better understanding supernova explosions in which the collapsing core contains angular momentum. A cylindrical geometry is chosen for the sake of simplicity. Even when the centrifugal force is very small, rotation can have a strong effect on the nonaxisymmetric modes of SASI by increasing the growth rate of the spiral modes rotating in the same direction… Show more

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Cited by 80 publications
(119 citation statements)
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“…On the other hand, differences do show up, for example, if random perturbations are added to the nonradial velocity components; this case is important in discussing the origin of pulsar spins proposed by Blondin & Mezzacappa (2007), and will be the subject of a forthcoming paper ( W. Iwakami et al 2008). We also note that the symmetry between m ¼ 1 and À1 modes is naturally removed if the unperturbed accretion flow is rotating (see Yamasaki & Foglizzo 2008). All the models presented in this paper are summarized in Table 1.…”
Section: Numerical Modelsmentioning
confidence: 93%
“…On the other hand, differences do show up, for example, if random perturbations are added to the nonradial velocity components; this case is important in discussing the origin of pulsar spins proposed by Blondin & Mezzacappa (2007), and will be the subject of a forthcoming paper ( W. Iwakami et al 2008). We also note that the symmetry between m ¼ 1 and À1 modes is naturally removed if the unperturbed accretion flow is rotating (see Yamasaki & Foglizzo 2008). All the models presented in this paper are summarized in Table 1.…”
Section: Numerical Modelsmentioning
confidence: 93%
“…It was unambiguously identified in 2D hydrodynamical simulations of idealized, adiabatic (and thus non-convective) postshock accretion flows (Blondin, Mezzacappa, & DeMarino 2003). SASI was found to possess the highest growth rates for the lowest-order (dipole and quadrupole) spherical harmonics (Blondin & Mezzacappa 2006;Foglizzo et al 2007;Iwakami et al 2008) and to give rise to spiral-mode mass motions in 3D simulations (Blondin & Mezzacappa 2007;Iwakami et al 2009;Fernández 2010;Hanke et al 2013) or in 2D setups without the constraint of axisymmetry (Blondin & Mezzacappa 2007;Yamasaki & Foglizzo 2008;Foglizzo et al 2012). The instability can be explained by an advectiveacoustic cycle of amplifying entropy and vorticity perturbations in the cavity between accretion shock and PNS surface (Foglizzo 2002;Foglizzo et al 2007;Scheck et al 2008; and has important consequences for NS kicks (Scheck et al 2004Nordhaus et al 2010bNordhaus et al , 2012Wongwathanarat, Janka, & Müller 2010, 2013 and spins (Blondin & Mezzacappa 2007;Rantsiou et al 2011;Guilet & Fernández 2013), quasi-periodic neutrino emission modulations (Marek, Janka, & Müller 2009;Lund et al 2010;Tamborra et al 2013), and SN gravitational-wave signals (Marek, Janka, & Müller 2009;Murphy, Ott, & Burrows 2009;).…”
Section: Introductionmentioning
confidence: 93%
“…It is possible that faster NS rotation requires the progenitor core to rotate (e.g., Heger et al 2005;Ott et al 2006). In a rotating environment, however, the growth of SASI spiral modes will be severely altered and potentially fostered (Blondin & Mezzacappa 2007;Yamasaki & Foglizzo 2008;Iwakami et al 2009), and three-dimensional simulations are therefore indispensable to make predictions for the connection between progenitor and NS rotation. Fryer & Kusenko (2006) pointed out that ejecta asymmetries could be used to distinguish between different theoretical suggestions for the kick mechanism.…”
Section: Neutron Star Spin-up Mechanismmentioning
confidence: 99%