论文标题

大量恒星形成中积聚模式的参数研究

Parameter study for the burst mode of accretion in massive star formation

论文作者

Meyer, D. M. -A., Vorobyov, E. I., Elbakyan, V. G., Eisloeffel, J., Sobolev, A. M., Stoehr, M.

论文摘要

现在,这是一种普遍认为的观点,在他们的形成和早期进化中,星星在爆发中积聚了质量。恒星形成场景的爆发模式表明,恒星是通过从重力不稳定的杂质盘迁移的碎片中的碎片中生长在质量中的,它自然地解释了从高质量质体中观察到的前序列爆发的存在。我们介绍了巨大的年轻恒星物体(迈索斯)的流体动力学模型的参数研究,该模型探讨了崩溃的云的初始质量(MC = 60-200MO)和旋转与重力能量的比率(β= 0:005-0:33)。 MC和/或Beta的增加产生了质子积聚盘,这些盘更容易发展引力不稳定并体验爆发。我们发现,即使迈索斯的固有核心都使Beta <= 0.01。因此,在我们的假设中,缺乏稳定的光盘是低质量和高质量星形成机制之间的主要区别。我们所有的圆盘质量和磁盘与明星质量比MD = M*> 1比例为具有恒星质量的幂律。我们的结果证实,在爆发模式下,大量的原始恒星增添了约40-60%的质量。两次连续爆发之间的时间段的分布是双峰的:持续时间很短(〜1-10年)峰值对应于短,最微弱的爆发和较长的持续时间峰(在〜10^3-10^4 yr),对应于长,fu-orionis-type的长时间,以后的迪斯科式爆发出现在后来的迪斯科爆发中,即在二十张二十张二十张吉尔,后来又是kyr afters afters ky afters kirl aftere。我们在大规模原始喷气机的结构中讨论了这种双峰性,这是积聚爆发历史的潜在特征。

It is now a widely held view that, in their formation and early evolution, stars build up mass in bursts. The burst mode of star formation scenario proposes that the stars grow in mass via episodic accretion of fragments migrating from their gravitationally-unstable circumstellar discs and it naturally explains the existence of observed pre-main-sequence bursts from high mass protostars. We present a parameter study of hydrodynamical models of massive young stellar objects (MYSOs) that explores the initial masses of the collapsing clouds (Mc = 60-200Mo) and ratio of rotational-to-gravitational energies (beta = 0:005-0:33). An increase in Mc and/or beta produces protostellar accretion discs that are more prone to develop gravitational instability and to experience bursts. We find that all MYSOs have bursts even if their pre-stellar core is such that beta <= 0.01. Within our assumptions, the lack of stable discs is therefore a major difference between low- and high-mass star formation mechanisms. All our disc masses and disk-to-star mass ratios Md=M* > 1 scale as a power-law with the stellar mass. Our results confirm that massive protostars accrete about 40-60% of their mass in the burst mode. The distribution of time periods between two consecutive bursts is bimodal: there is a short duration (~ 1-10 yr) peak corresponding to the short, faintest bursts and a long duration peak (at ~ 10^3-10^4 yr) corresponding to the long, FU-Orionis-type bursts appearing in later disc evolution, i.e., around 30 kyr after disc formation. We discuss this bimodality in the context of the structure of massive protostellar jets as potential signatures of accretion burst history.

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