Nuclear shell burning in the final stages of the lives of massive stars is accompanied by strong turbulent convection. The resulting fluctuations aid supernova explosion by amplifying the non-radial flow in the post-shock region. In this work, we investigate the physical mechanism behind this amplification using a linear perturbation theory. We model the shock wave as a one-dimensional planar discontinuity and consider its interaction with vorticity and entropy perturbations in the upstream flow. We find that, as the perturbations cross the shock, their total turbulent kinetic energy is amplified by a factor of ∼2, while the average linear size of turbulent eddies decreases by about the same factor. These values are not sensitive to the par...
Convection that develops behind the shock front during the first second of a core-collapse supernova...
We investigate prompt convection in core collapse supernovae and its consequences for the late-time ...
The neutrino-heated “gain layer ” immediately behind the stalled shock in a core-collapse supernova ...
The supernova explosion of massive stars is a complex physical event. Nuclear shell burning in the ...
Convective instabilities in the advanced stages of nuclear shell burning can play an important role ...
Convective perturbations arising from nuclear shell burning can play an important role in propelling...
In the context of core-collapse supernova explosions, the interaction of standing accretion shocks w...
The neutrino-heated "gain layer" immediately behind the stalled shock in a core-collapse supernova ...
We present results from high-resolution semiglobal simulations of neutrino-driven convection in core...
The explosion of massive stars in core-collapse supernovae may be aided by the con vective instabili...
International audienceA toy model of the post-shock region of core-collapse supernovae is used to st...
We conduct a series of numerical experiments into the nature of three-dimensional (3D) hydrodynamics...
The explosion of massive stars involves the formation of a shock wave. In stars that develop iron co...
Convection that develops behind the shock front during the first second of a core-collapse supernova...
We investigate prompt convection in core collapse supernovae and its consequences for the late-time ...
The neutrino-heated “gain layer ” immediately behind the stalled shock in a core-collapse supernova ...
The supernova explosion of massive stars is a complex physical event. Nuclear shell burning in the ...
Convective instabilities in the advanced stages of nuclear shell burning can play an important role ...
Convective perturbations arising from nuclear shell burning can play an important role in propelling...
In the context of core-collapse supernova explosions, the interaction of standing accretion shocks w...
The neutrino-heated "gain layer" immediately behind the stalled shock in a core-collapse supernova ...
We present results from high-resolution semiglobal simulations of neutrino-driven convection in core...
The explosion of massive stars in core-collapse supernovae may be aided by the con vective instabili...
International audienceA toy model of the post-shock region of core-collapse supernovae is used to st...
We conduct a series of numerical experiments into the nature of three-dimensional (3D) hydrodynamics...
The explosion of massive stars involves the formation of a shock wave. In stars that develop iron co...
Convection that develops behind the shock front during the first second of a core-collapse supernova...
We investigate prompt convection in core collapse supernovae and its consequences for the late-time ...
The neutrino-heated “gain layer ” immediately behind the stalled shock in a core-collapse supernova ...