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arXiv 2602.04474astro-ph.SRastro-ph.GAastro-ph.HE
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SN 2017ati:来自大质量前身的明亮型IIb超新星爆发

SN 2017ati: A luminous type IIb explosion from a massive progenitor

Chongqing University of Posts and Telecommunications(重庆邮电大学);INAF - Osservatorio Astronomico di Padova(意大利国家天体物理研究所帕多瓦天文台);Yunnan Observatories, Chinese Academy of Sciences(中国科学院云南天文台);International Centre of Supernovae, Yunnan Key Laboratory(国际超新星中心云南省重点实验室);South-Western Institute for Astronomy Research, Yunnan Key Laboratory of Survey Science, Yunnan University(云南大学西南天文研究所云南省测绘科学重点实验室);INAF - Osservatorio Astronomico di Brera(意大利国家天体物理研究所布雷拉天文台);School of Astronomy and Space Science, University of Chinese Academy of Sciences(中国科学院大学天文与空间科学学院);National Astronomical Observatories, Chinese Academy of Sciences(中国科学院国家天文台)
Z. -H. Peng, S. Benetti, Y. -Z. Cai, A. Pastorello, J. -W. Zhao, A. Reguitti, Z. -Y. Wang, E. Cappellaro, N. Elias-Rosa, Q. -L. Fang, M. Fraser, T. Kangas, E. K… 展开作者

Z. -H. Peng, S. Benetti, Y. -Z. Cai, A. Pastorello, J. -W. Zhao, A. Reguitti, Z. -Y. Wang, E. Cappellaro, N. Elias-Rosa, Q. -L. Fang, M. Fraser, T. Kangas, E. Kankare, Z. Kostrzewa-Rutkowska, P. Lundqvist, S. Mattila, T. M. Reynolds, M. D. Stritzinger, A. Somero, L. Tomasella, S. -P. Pei, Y. -J. Yang, J. -J. Zhang, Y. Pan

AI总结:

研究通过光度学和光谱学观测分析了SN 2017ati,发现其光变曲线在晚期仍比预期明亮,表明其能量来源可能包括中子星自转能量和放射性镍沉积,且其前身质量估计为至少17个太阳质量。

摘要:

我们提供了Ia型IIb超新星(SN)2017ati的光学光度学和光谱学观测。它在爆炸后约27天达到最大光度,光变曲线显示一个宽而明亮的峰值,绝对r波段视星等为M_r = -18.48 ± 0.16 mag。在最大光度后约50天,SN 2017ati的衰减率接近由^56Co → ^56Fe放射性衰变预期的值,即每100天0.98 mag,通常在IIb型超新星中观察到。然而,它在晚期仍比通常范围高出1-2 mag,超过了该类别的通常上限。因此,用标准^56Ni衰变模型拟合SN 2017ati的光变曲线需要高达约0.37 M_sun的镍质量,但仍无法充分再现早期光变曲线。相反,加入来自磁星的额外能量输入可显著改善SN 2017ati光变曲线的拟合,将镍质量降至约0.21 M_sun,仍接近IIb型超新星通常推断的上限。将SN 2017ati的拟合结果与已知的IIb型超新星样本进行比较,表明其光度演变最佳解释为中子星自转能量和放射性镍沉积的结合。从晚期的星云光谱中,[O I] λλ6300,6364双重线的光度暗示氧质量为约1.82-3.34 M_sun,且[Ca II]/[O I]流量比为约0.5,结合星云光谱模型比较,倾向于前身零年龄主序质量至少为17 M_sun。

英文摘要:

We present optical photometric and spectroscopic observations of the Type~IIb supernova (SN)~2017ati. It reached the maximum light at about 27~d after the explosion and the light curve shows a broad, luminous peak with an absolute $r$-band magnitude of $M_{r} = -18.48 \pm 0.16$~mag. At about 50~d after maximum light, SN~2017ati exhibits a decline rate close to that expected from the $^{56}$Co $\rightarrow$ $^{56}$Fe radioactive decay, at 0.98 mag per 100 days, as usually observed in SNe IIb. However, it remains systematically brighter at late times by about 1--2~mag, exceeding the usual upper luminosity range of this class. As a result, modelling the light curve of SN~2017ati with a standard $^{56}$Ni decay scenario requires a large nickel mass of up to $\sim0.37\,M_{\odot}$ and still fails to reproduce the early-time light curve adequately. In contrast, incorporating additional energy input from a magnetar yields a significantly improved fit to the light curve of SN~2017ati, which would reduce the nickel mass to $\sim0.21\,M_{\odot}$, still close to the upper end of the range typically inferred for SNe~IIb. Comparing the fitted results of SN~2017ati with the known sample of SNe~IIb indicates that its luminosity evolution is best explained by a combination of neutron star spin-down energy and radioactive nickel deposition. From late-time nebular spectra of SN~2017ati, the luminosity of the [\Oi]~$λ\lambda6300,6364$ doublet implies an oxygen mass of $\sim1.82-3.34\,M_{\odot}$, and the combination of a [\Caii]/[\Oi] flux ratio of $\sim0.5$ with nebular spectral model comparisons favours a progenitor zero-age main-sequence mass of $\geq17\,M_{\odot}$.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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