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arXiv 2101.01596astro-ph.SR
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FU-Orionis型亮度爆发不同机制的判别

Distinguishing between different mechanisms of FU-Orionis-type luminosity outbursts

Eduard I. Vorobyov, Vardan G. Elbakyan, Hauyu Baobab Liu, Michihiro Takami

摘要:

目标。吸积和亮度爆发触发的三个不同的机制:磁旋转不稳定性的内部磁盘区域,在引力破碎的磁盘和近距离接触的入侵者的恒星,进行了研究,以确定磁盘的运动学特征,可以帮助区分这些突发机制。方法.在薄磁盘限制的数值流体动力学模拟的磁盘环境中,预计每一个突发机制的突发。结果我们发现,具有吸积爆发的拱星盘可以承受不同的爆发机制,这可能是有用的,当确定爆发的起源是不同的运动学特征。在恒星碰撞模型和团块撞击模型中,圆盘的特征是与开普勒自转有百分之几十的偏差,而在MRI模型中,圆盘的特征是只有百分之几的偏差,这主要是由引发MRI爆发的引力不稳定性引起的。速度通道图也显示出不同的扭结和摆动,这是由气盘流动所造成的,这是每一个所考虑的爆炸机制所特有的。在爆发托管磁盘的速度通道的偏离典型的开普勒磁盘的对称模式是最强的块下落和碰撞模型,并进行个别功能,可能是有用的识别相应的突发机制。所考虑的爆发机制产生了各种各样的光变曲线,爆发幅度在Δm=2.5-3.7的范围内变化,除了聚集-下落模型,其中Δm可以达到5.4,尽管导出的数字可能受到小样本和边界条件的影响。结论.突发触发机制与突发托管磁盘中的不同运动学特征相关联,这些特征可用于识别突发托管磁盘。节录。

英文摘要:

Aims. Accretion and luminosity bursts triggered by three distinct mechanisms: the magnetorotational instability in the inner disk regions, clump infall in gravitationally fragmented disks and close encounters with an intruder star, were studied to determine the disk kinematic characteristics that can help to distinguish between these burst mechanisms. Methods. Numerical hydrodynamics simulations in the thin-disk limit were employed to model the bursts in disk environments that are expected for each burst mechanism. Results. We found that the circumstellar disks featuring accretion bursts can bear kinematic features that are distinct for different burst mechanisms, which can be useful when identifying the burst origin. The disks in the stellar encounter and clump-infall models are characterized by tens of percent deviations from the Keplerian rotation, whie the disks in the MRI models are characterized only a few percent deviation, which is mostly caused by the gravitational instability that fuels the MRI bursts. Velocity channel maps also show distinct kinks and wiggles, which are caused by gas disk flows that are peculiar to each considered burst mechanism. The deviations of velocity channels in the burst-hosting disks from a symmetric pattern typical of Keplerian disks are strongest for the clump-infall and collision models, and carry individual features that may be useful for the identification of the corresponding burst mechanism. The considered burst mechanisms produce a variety of light curves with the burst amplitudes varying in the Δm=2.5-3.7 limits, except for the clump-infall model where Δm can reach 5.4, although the derived numbers may be affected by a small sample and boundary conditions. Conclusions. Burst triggering mechanisms are associated with distinct kinematic features in the burst-hosting disks that may be used for their identification. Abridged.

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