The radial distribution of radio emission from SN 1993J: Magnetic field amplification due to the Rayleigh-Taylor instability

IF 5.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Astronomy & Astrophysics Pub Date : 2024-11-08 DOI:10.1051/0004-6361/202450329
I. Martí-Vidal, C.-I. Björnsson, M. A. Pérez-Torres, P. Lundqvist, J. M. Marcaide
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Abstract

Context. Observations of radio emission from young core-collapse supernovae (CCSNe) allow one to study the history of the pre-supernova stellar wind, trace the density structure of the ejected material, and probe the magnetohydrodynamics that describe the interaction between the two, as the forward shock expands into the circumstellar medium. The radio shell of supernova SN 1993J has been observed with very long baseline interferometry (VLBI) for ∼20 years, giving one of the most complete pictures of the evolution of a CCSN shock. However, different results about the expansion curve and properties of the radio-emitting structure have been reported by different authors, likely due to systematics in the data calibration and/or model assumptions made by each team.Aims. We aim to perform an analysis of the complete set of VLBI observations of SN 1993J that accounts for different instrumental and source-intrinsic effects, in order to retrieve robust conclusions about the shock expansion and physics in SN 1993J.Methods. We have explored the posterior probability distribution of a complete data model, using a technique based on Markov chains. Our model accounts for antenna calibration effects, as well as different kinds of radio-emission structures for the supernova.Results. The posterior parameter distributions strongly favor a spherical shell-like radio structure with a nonuniform radial intensity profile, with a broad brightness distribution that peaks close to or just above the region where the contact discontinuity is expected to be located. Regarding the shell expansion, the full dataset can be well described using one single deceleration parameter, β ∼ 0.80, being the shell outer radius R ∝ tβ. There is clear evidence of a relative widening of the shell width beyond day 2600−3300 after the explosion, which is due to an increased deceleration of the inner shell boundary. This is similar to findings previously reported by other authors.Conclusions. The radial intensity profile and the late evolution of the shell suggest a scenario in which the magnetic field is amplified mainly by the Rayleigh-Taylor instability, which emanates from the contact discontinuity. Furthermore, the increased deceleration of the inner boundary indicates that the reverse shock enters a region of the ejecta at around 3000 days, where the density distribution is substantially flatter. Such a weakening of the reverse shock can also explain the achromatic break in the radio light curves, which occurs at the same time. The deduced radial intensity distribution for SN 1993J is quite similar to that observed in the spatially well-resolved supernova remnant Cassiopeia A.
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SN 1993J 射电辐射的径向分布:瑞利-泰勒不稳定性导致的磁场放大
背景通过对年轻的核坍缩超新星(CCSNe)射电辐射的观测,我们可以研究超新星前恒星风的历史,追踪抛射物质的密度结构,并探测描述前向冲击向周星际介质膨胀时两者相互作用的磁流体动力学。超新星 SN 1993J 的射电壳体已经被超长基线干涉测量法(VLBI)观测了 20 年之久,这是最完整的 CCSN 冲击演化图之一。然而,不同的作者对射电发射结构的膨胀曲线和特性有不同的报道,这可能是由于每个团队在数据校准和/或模型假设方面的系统性造成的。我们的目的是对 SN 1993J 的整套 VLBI 观测数据进行分析,以考虑不同的仪器效应和源内在效应,从而获得有关 SN 1993J 的冲击膨胀和物理特性的可靠结论。我们利用基于马尔可夫链的技术,探索了完整数据模型的后验概率分布。我们的模型考虑了天线校准效应以及超新星的不同射电发射结构。后验参数分布强烈倾向于一个具有非均匀径向强度剖面的球壳状射电结构,其亮度分布宽广,峰值接近或刚好高于预计的接触不连续性所在区域。关于壳的扩展,整个数据集可以用一个单一的减速参数β∼0.80(即壳的外半径R∝tβ)来很好地描述。有明显的证据表明,爆炸后第 2600-3300 天以后,壳体宽度相对增宽,这是由于壳体内边界的减速效应增强所致。这与其他作者之前报告的结果类似。壳体的径向强度分布和后期演变表明,磁场主要是由接触不连续性产生的瑞利-泰勒不稳定性放大的。此外,内部边界的减速增加表明,反向冲击在 3000 天左右进入了喷出物的一个区域,在这个区域,密度分布要平坦得多。反向冲击的减弱也可以解释同时出现的射电光曲线消色差断裂。推导出的SN 1993J的径向强度分布与在空间分辨率较高的超新星残余仙后座A中观测到的非常相似。
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来源期刊
Astronomy & Astrophysics
Astronomy & Astrophysics 地学天文-天文与天体物理
CiteScore
10.20
自引率
27.70%
发文量
2105
审稿时长
1-2 weeks
期刊介绍: Astronomy & Astrophysics is an international Journal that publishes papers on all aspects of astronomy and astrophysics (theoretical, observational, and instrumental) independently of the techniques used to obtain the results.
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