论文标题
行星星云的共同包膜塑造。 iv。从原始星际到行星星云
Common Envelope Shaping of Planetary Nebulae. IV. From Proto-planetary to Planetary Nebula
论文作者
论文摘要
我们提出了对经历了常见包膜事件的二元系统中的二元系统中二元系统中的中央恒星的2D流体动力学模拟,向中央恒星的行星星云过渡。在1,000年的磁驱动动力学(原始星云阶段)后,将线驱动的恒星风引入计算域中,并为另外10,000年的年度模拟了星云的膨胀,包括恒星照片的影响。在这项研究中,我们考虑了1(0.569)和2.5(0.677)\ mo的主要序列(最终)质量的中心恒星,以及序列伴侣的0.6 \ mo mA。极度双极的,狭窄的原始星际星云导致双极行星星云,而其余形状主要演变为椭圆形的行星星云。在大多数情况下,最初的磁场对准直结构(例如喷气机)的影响往往会消失,仅在少数情况下留下了这些特征的残留物。赤道区域主要由光电离(1 \ mo祖细胞)碎片,导致``项链''结构由与辐射场对齐的彗星团制成。另一方面,通过光电离和震动的风(2.5 \ mo祖细胞)的碎裂导致在纬度方向上形成多个团块,这些团块留在裂片内,靠近叶片,靠近中心,并被热震动的气体浸入并包围,被热的气体包围,不一定与辐射场保持一致。这些结果表明,碎裂过程对恒星质量祖细胞有依赖性。通过由喷气机的作用雕刻的先前常见的包膜原始星云中,气体的分布使这种碎片成为可能。
We present 2D hydrodynamical simulations of the transition of a proto-planetary nebula to a planetary nebula for central stars in binary systems that have undergone a common envelope event. After 1,000 yr of magnetically driven dynamics (proto-planetary nebula phase), a line-driven stellar wind is introduced into the computational domain and the expansion of the nebula is simulated for another 10,000 yr, including the effects of stellar photoionization. In this study we consider central stars with main sequence (final) masses of 1 (0.569) and 2.5 (0.677) \Mo, together with a 0.6 \Mo ma in sequence companion. Extremely bipolar, narrow-waisted proto-planetary nebulae result in bipolar planetary nebulae, while the rest of the shapes mainly evolve into elliptical planetary nebulae. The initial magnetic field's effects on the collimated structures, such as jets, tend to disappear in most of the cases, leaving behind the remnants of those features in only a few cases. Equatorial zones fragmented mainly by photoionization ( 1 \Mo progenitors), result in ``necklace'' structures made of cometary clumps aligned with the radiation field. On the other hand, fragmentation by photoionization and shocked wind ( 2.5 \Mo progenitors) give rise to the formation of multiple clumps in the latitudinal direction, which remain within the lobes, close to the center, which are immersed and surrounded by hot shocked gas, not necessarily aligned with the radiation field. These results reveal that the fragmentation process has a dependence on the stellar mass progenitor. This fragmentation is made possible by the distribution of gas in the previous post-common envelope proto-planetary nebula as sculpted by the action of the jets.