论文标题

正常型IA SN 2018AOZ的起源和演变,婴儿相红和发射过量

The origin and evolution of the normal Type Ia SN 2018aoz with infant-phase reddening and excess emission

论文作者

Ni, Yuan Qi, Moon, Dae-Sik, Drout, Maria R., Polin, Abigail, Sand, David J., GonzÁlez-GaitÁn, Santiago, Kim, Sang Chul, Lee, Youngdae, Park, Hong Soo, Howell, D. Andrew, Nugent, Peter E., Piro, Anthony L., Brown, Peter J., Galbany, LluÍs, Burke, Jamison, Hiramatsu, Daichi, Hosseinzadeh, Griffin, Valenti, Stefano, Afsariardchi, Niloufar, Andrews, Jennifer E., Antoniadis, John, Beaton, Rachael L., Bostroem, K. Azalee, Carlberg, Raymond G., Cenko, S. Bradley, Cha, Sang-Mok, Dong, Yize, Gal-Yam, Avishay, Haislip, Joshua, Holoien, Thomas W. -S., Johnson, Sean D., Kouprianov, Vladimir, Lee, Yongseok, Matzner, Christopher D., Morrell, Nidia, Mccully, Curtis, Pignata, Giuliano, Reichart, Daniel E., Rich, Jeffrey, Ryder, Stuart D., Smith, Nathan, Wyatt, Samuel, Yang, Sheng

论文摘要

SN〜2018AOZ是一种IA型SN,具有$ B $频带高原,在初次光线后1天,在婴儿期光曲线$ \ Lessim $ 1 $ $ \ Lessim中的发射过量,如我们先前的研究所示,表现出过度密度的表面铁峰元素。在这里,我们基于其演变直到变形阶段,推进了SN〜2018AOZ的性质和起源的限制。近峰光谱特征表明,SN在正常类型IA的两个亚型之间中间:核心正常和宽线。过量的发射可能会从表面铁峰元素的放射性衰减以及与二元伴侣或少量情节材料的相互作用中产生贡献。 Nebular-phase对H $α$的限制,他〜我偏爱白矮人的伴侣,这与低早期SN发光度限制的小伴侣大小一致,而没有[O〜I],而他〜我〜我散布了祖先的暴力合并。在SN〜2018AOZ中提出的两种主要爆炸机制中,不对称的Chandrasekhar-Mass爆炸与祖细胞的约束和观察到的Nebular-Phase [Fe〜II]和[Ni〜II]的蓝色蓝色的蓝光相位。氦壳的双重爆炸与观察到的缺乏C光谱特征兼容,但是当前的1-D模型与婴儿相过多的发射不兼容,$ b _ {\ rm max} -v _ {\ rm max} $ co and co ca 〜ca〜ii ii]。尽管SN〜2018AOZ的爆炸过程仍然需要更精确地了解,但相同的过程可能会产生很大一部分IA SNE,而IA型SNE的一小部分在$ \ sim $ 1 $ 1天后看起来很正常。

SN~2018aoz is a Type Ia SN with a $B$-band plateau and excess emission in the infant-phase light curves $\lesssim$ 1 day after first light, evidencing an over-density of surface iron-peak elements as shown in our previous study. Here, we advance the constraints on the nature and origin of SN~2018aoz based on its evolution until the nebular phase. Near-peak spectroscopic features show the SN is intermediate between two subtypes of normal Type Ia: Core-Normal and Broad-Line. The excess emission could have contributions from the radioactive decay of surface iron-peak elements as well as ejecta interaction with either the binary companion or a small torus of circumstellar material. Nebular-phase limits on H$α$ and He~I favour a white dwarf companion, consistent with the small companion size constrained by the low early SN luminosity, while the absence of [O~I] and He~I disfavours a violent merger of the progenitor. Of the two main explosion mechanisms proposed to explain the distribution of surface iron-peak elements in SN~2018aoz, the asymmetric Chandrasekhar-mass explosion is less consistent with the progenitor constraints and the observed blueshifts of nebular-phase [Fe~II] and [Ni~II]. The helium-shell double-detonation explosion is compatible with the observed lack of C spectral features, but current 1-D models are incompatible with the infant-phase excess emission, $B_{\rm max}-V_{\rm max}$ color, and absence of nebular-phase [Ca~II]. Although the explosion processes of SN~2018aoz still need to be more precisely understood, the same processes could produce a significant fraction of Type Ia SNe that appear normal after $\sim$ 1 day.

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