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Three-Dimensional Simulations of Standing Accretion Shock Instability in Core-Collapse Supernovae

机译:核心坍塌超新星站立吸积激波不稳定性的三维模拟

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We have studied nonaxisymmetric standing accretion shock instabilities, or SASI, using three-dimensional (3D) hydrodynamical simulations. This is an extension of our previous study of axisymmetric SASI. We have prepared a spherically symmetric and steady accretion flow through a standing shock wave onto a proto-neutron star, taking into account a realistic equation of state and neutrino heating and cooling. This unperturbed model is meant to represent approximately the typical postbounce phase of core-collapse supernovae. We then added a small perturbation (~1%) to the radial velocity and computed the ensuing evolutions. Both axisymmetric and nonaxisymmetric perturbations have been imposed. We have applied mode analysis to the nonspherical deformation of the shock surface, using spherical harmonics. We have found that (1) the growth rates of SASI are degenerate with respect to the azimuthal index m of the spherical harmonics Ylm, just as expected for a spherically symmetric background; (2) nonlinear mode couplings produce only m = 0 modes for axisymmetric perturbations, whereas m≠ 0 modes are also generated in the nonaxisymmetric cases, according to the selection rule for quadratic couplings; (3) the nonlinear saturation level of each mode is lower in general for 3D than for 2D, because a larger number of modes contribute to turbulence in 3D; (4) low-l modes are dominant in the nonlinear phase; (5) equipartition is nearly established among different m modes in the nonlinear phase; (6) spectra with respect to l obey power laws with a slope slightly steeper for 3D; and (7) although these features are common to the models with and without a shock revival at the end of the simulation, the dominance of low- l modes is more remarkable in the models with a shock revival.
机译:我们使用三维(3D)流体动力学模拟研究了非轴对称站立增生冲击不稳定性或SASI。这是我们先前对轴对称SASI研究的扩展。考虑到状态和中微子加热和冷却的现实方程,我们已经准备了通过驻波冲击到达原始中子星的球形对称稳定吸积流。这种不受干扰的模型旨在代表核心塌陷超新星的典型反弹后阶段。然后,我们向径向速度添加了一个小扰动(〜1%),并计算了随后的演化。轴对称和非轴对称扰动都已被施加。我们已经使用球形谐波将模式分析应用于冲击表面的非球形变形。我们发现(1)SASI的增长率相对于球谐函数Ylm的方位角m退化,正如对球对称背景所期望的那样; (2)根据二次耦合的选择规则,非线性模态耦合仅对轴对称扰动产生m = 0个模态,而在非轴对称情况下,也产生m≠0个模态; (3)3D的每个模式的非线性饱和度通常要比2D的低,这是因为大量的模式会导致3D的湍流。 (4)低l模式在非线性阶段占主导地位; (5)在非线性阶段,在不同的m模式之间几乎建立了均分; (6)关于3D的服从幂律的光谱,其斜率略陡; (7)尽管在仿真结束时有或没有激振恢复的模型都具有这些特征,但在激振恢复的模型中,低l模式的优势更为明显。

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