论文标题

磁化分子云中细丝形成机制的分类

Classification of Filament Formation Mechanisms in Magnetized Molecular Clouds

论文作者

Abe, Daisei, Inoue, Tsuyoshi, Inutsuka, Shu-ichiro, Matsumoto, Tomoaki

论文摘要

最近对分子云的观察结果表明,密集的细丝是当今恒星形成的位置。因此,有必要了解灯丝形成过程,因为这些细丝为恒星形成提供了初始条件。理论研究表明,分子云中的冲击波触发细丝形成。由于已经提出了几种不同的丝形成机制,因此观察到的恒星形成细丝的形成机制需要澄清。在本研究中,我们进行了一系列丝形成的等温磁流体动力学模拟。我们专注于冲击速度和湍流对形成机制的影响,并确定了灯丝形成的三种不同机制。结果表明,当冲击快速时,在冲击速度V_SH = 7 km/s时,弯曲冲击波驱动的气流会产生丝状丝,而与湍流和自我的存在无关。但是,在慢速冲击速度v_sh = 2.5 km/s时,与初始湍流有关的压缩流量成分会诱导细丝形成。当冲击速度和湍流都较低时,冲击压缩板中的自我对丝的形成变得很重要。此外,我们分析了细丝的线质量分布,并表明强烈的冲击波自然会产生高线质丝,例如在短时间内在巨大的恒星形成区域中观察到的丝。我们得出的结论是,主要的细丝形成模式随冲击波的速度触发细丝形成而变化。

Recent observations of molecular clouds show that dense filaments are the sites of present-day star formation. Thus, it is necessary to understand the filament formation process because these filaments provide the initial condition for star formation. Theoretical research suggests that shock waves in molecular clouds trigger filament formation. Since several different mechanisms have been proposed for filament formation, the formation mechanism of the observed star-forming filaments requires clarification. In the present study, we perform a series of isothermal magnetohydrodynamics simulations of filament formation. We focus on the influences of shock velocity and turbulence on the formation mechanism and identified three different mechanisms for the filament formation. The results indicate that when the shock is fast, at shock velocity v_sh = 7 km/s, the gas flows driven by the curved shock wave create filaments irrespective of the presence of turbulence and self-gravity. However, at a slow shock velocity v_sh = 2.5 km/s, the compressive flow component involved in the initial turbulence induces filament formation. When both the shock velocities and turbulence are low, the self-gravity in the shock-compressed sheet becomes important for filament formation. Moreover, we analyzed the line-mass distribution of the filaments and showed that strong shock waves can naturally create high-line-mass filaments such as those observed in the massive star-forming regions in a short time. We conclude that the dominant filament formation mode changes with the velocity of the shock wave triggering the filament formation.

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