利用哈勃太空望远镜追踪数十年来 SN 1987A 赤道环中冲击波的传播情况

Christos Tegkelidis, Josefin Larsson and Claes Fransson
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摘要

邻近的 SN 1987A 为研究抛射物和周围星际介质之间复杂的冲击相互作用提供了一个独特的机会。我们通过分析 1994 年至 2022 年间哈勃太空望远镜的 33 次成像观测数据,跟踪赤道环(ER)内光学热点的演变过程。通过对赤道环进行椭圆模型拟合,我们确定其倾角为 42.°85 ± 0.°50,主轴方向为西经 -6.°24 ± 0.°31。我们在整个 ER 上发现了 26 个明显的热点,随着时间的推移,特别是在西侧,还会出现更多的热点。这些热点最初表现出 390 至 1660 km s-1 的高速度,随后在 8000 天左右进入减速阶段。随后的速度从 40 到 660 公里/秒不等。热点的光变曲线在 7000 到 9000 天之间达到最大值,这表明与减速有关。许多热点都具有空间分辨率,并显示出垂直于运动方向的伸长,表明冷却时间很短。为了解释这些结果,我们提出每个热点都由嵌入密度较小气体中的致密子结构组成。最初的速度是相位速度,当爆炸波离开ER时发生断裂,而后期的速度则反映了致密子结构中辐射冲击的传播。我们估计致密子结构的体积填充因子为 ,总质量为 。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Tracing the Propagation of Shocks in the Equatorial Ring of SN 1987A over Decades with the Hubble Space Telescope
The nearby SN 1987A offers a unique opportunity to investigate the complex shock interaction between the ejecta and circumstellar medium. We track the evolution of the optical hot spots within the equatorial ring (ER) by analyzing 33 Hubble Space Telescope imaging observations between 1994 and 2022. By fitting the ER with an elliptical model, we determine its inclination to be 42.°85 ± 0.°50 with its major axis oriented −6.°24 ± 0.°31 from the west. We identify 26 distinct hot spots across the ER, with additional ones emerging over time, particularly on the western side. The hot spots initially show high velocities ranging from 390 to 1660 km s−1, followed by a deceleration phase around day ∼ 8000. Subsequent velocities vary from 40 to 660 km s−1. The light curves of the hot spots reach maxima between 7000 and 9000 days, suggesting a connection with the deceleration. Many spots are spatially resolved and show elongation perpendicular to the direction of motion, indicative of a short cooling time. To explain these results, we propose that each hot spot comprises dense substructures embedded in less dense gas. The initial velocities are then phase velocities, where the break occurs when the blast wave leaves the ER, while the late velocities reflect the propagation of radiative shocks in the dense substructures. We estimate that the dense substructures have a volumetric filling factor of and a total mass of .
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