论文标题

2018HYZ I的潮汐破坏事件:双峰排放线和平坦的Balmer降低

The Tidal Disruption Event AT 2018hyz I: Double-peaked emission lines and a flat Balmer decrement

论文作者

Short, P., Nicholl, M., Lawrence, A., Gomez, S., Arcavi, I., Wevers, T., Leloudas, G., Schulze, S., Anderson, J. P., Berger, E., Blanchard, P. K., Burke, J., Segura, N. Castro, Charalampopoulos, P., Chornock, R., Galbany, L., Gromadzki, M., Herzog, L. J., Hiramatsu, D., Horne, Keith, Hosseinzadeh, G., Howell, D. Andrew, Ihanec, N., Inserra, C., Kankare, E., Maguire, K., McCully, C., Bravo, T. E. Müller, Onori, F., Sollerman, J., Young, D. R.

论文摘要

我们介绍了AT 2018HYZ的光谱观察结果,这是ASAS -SN调查以$ m_v \ sim -20.2 $ mag的绝对幅度发现的瞬态,并在具有强大的Balmer吸收线的静态星系的核中。在2018年,HYZ显示了蓝色光谱连续性和宽阔的发射线,与以前的TDE候选者一致。高节奏的随访光谱显示出宽阔的Balmer线条,他在早期的光谱中,我在$ \ sim70-100 $ $ $天之后出现。 Balmer线从平滑的宽轮廓演变,通过与积聚圆盘发射一致的方形,不对称的双峰相位,并在后期返回光滑。 Balmer系列与典型的AGN不同,因为它们显示出平坦的Balmer降低(H $α$/H $β\ SIM1.5 $),这表明这些线是碰撞激发的,而不是通过照相离世产生。平坦的Balmer与复合物剖面一起降低表明,发射线起源于圆盘染色体,类似于在灾难性变量中看到的发射线。由于可能的部分破坏而引起的材料的低光学深度可能使我们能够观察到这些双峰,碰撞激发的线。 HE II的晚期外观可能是由于光球或流出的扩展或碎片碰撞中的延迟冲击。

We present results from spectroscopic observations of AT 2018hyz, a transient discovered by the ASAS-SN survey at an absolute magnitude of $M_V\sim -20.2$ mag, in the nucleus of a quiescent galaxy with strong Balmer absorption lines. AT 2018hyz shows a blue spectral continuum and broad emission lines, consistent with previous TDE candidates. High cadence follow-up spectra show broad Balmer lines and He I in early spectra, with He II making an appearance after $\sim70-100$ days. The Balmer lines evolve from a smooth broad profile, through a boxy, asymmetric double-peaked phase consistent with accretion disc emission, and back to smooth at late times. The Balmer lines are unlike typical AGN in that they show a flat Balmer decrement (H$α$/H$β\sim1.5$), suggesting the lines are collisionally excited rather than being produced via photo-ionisation. The flat Balmer decrement together with the complex profiles suggest that the emission lines originate in a disc chromosphere, analogous to those seen in cataclysmic variables. The low optical depth of material due to a possible partial disruption may be what allows us to observe these double-peaked, collisionally excited lines. The late appearance of He II may be due to an expanding photosphere or outflow, or late-time shocks in debris collisions.

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