论文标题

SN 2018HTI:附近的超浮肿超新星在金属贫困的星系中发现

SN 2018hti: a nearby superluminous supernova discovered in a metal-poor galaxy

论文作者

Lin, W. L., Wang, X. F., Li, W. X., Zhang, J. J., Mo, J., Sai, H. N., Zhang, X. H., Filippenko, A. V., Zheng, W. K., Brink, T. G., Baron, E., DerKacy, J. M., Ehgamberdiev, S. A., Mirzaqulov, D., Li, X., Zhang, J. C., Yan, S. Y., Xi, G. B., Hsiao, Y., Zhang, T. M., Wang, L. J., Liu, L. D., Xiang, D. F., Wu, C. Y., Rui, L. M., Chen, Z. H.

论文摘要

SN 2018HTI是I型超浮肿超新星(SLSN〜I),绝对$ g $ -b $ - 带的幅度为$ -22.2 $,最大亮度为$ -22.2 $,以0.0612的红移在金属贫困的星系中发现。我们介绍了该超新星的广泛光度和光谱观察结果,涵盖了$ \ sim -35 $的阶段,至$ r $ band最大值的+340天以上。将我们的$ bvgri $ -band光度法与{\ it swift} uvot光学/紫外线光度法相结合,我们将峰值发光度计算为$ \ sim 3.5 \ times10^{44} $ erg s $^{ - 1} $。对观察到的光曲线进行建模表明,SN 2018HTI的光度演变可以由5.8 $ M_ \ odot $的弹出质量和具有磁场为$ b = 1.8 \ times10^{13} $ 〜g的磁场的磁场产生,其初始旋转周期为$ p_0 = 1.8 $ ms。基于这种磁力供电的情况和更大的样品,可以推断出大多数SLSNE〜I的磁力旋转与射流能量之间的相关性,这表明是一种自持平的情况。像其他Slsne〜I一样,SN 2018HTI的主机Galaxy被发现相对较弱($ M_ {G} = -17.75 $ mag)和低金属性($ z = 0.3〜Z_ \ odot $),星形形成率为0.3 $ M_ \ odot $ yr $ yr $ $ yr $^{-1} $。根据单星发展的模拟结果,SN 2018HTI可能源自巨大的,贫穷的恒星,其零年龄主序列(ZAMS)质量为25--40 $ M_ \ odot $,或者来自不太庞大的旋转恒星,带有$ M_ \ mathrm {zams} \ yathrm {Zams} \ od-Mathrm {Zams} \ od-25 $ 25 $ m_ \ odot $ \ odot。对于二进制系统的情况,其祖细胞也可能是$ M_ \ Mathrm {Zams} \ Gtrsim 25 $ $ M_ \ odot $的星星。

SN 2018hti is a Type I superluminous supernova (SLSN~I) with an absolute $g$-band magnitude of $-22.2$ at maximum brightness, discovered in a metal-poor galaxy at a redshift of 0.0612. We present extensive photometric and spectroscopic observations of this supernova, covering the phases from $\sim -35$ days to more than +340 days from the $r$-band maximum. Combining our $BVgri$-band photometry with {\it Swift} UVOT optical/ultraviolet photometry, we calculated the peak luminosity as $\sim 3.5\times10^{44}$ erg s$^{-1}$. Modeling the observed light curve reveals that the luminosity evolution of SN 2018hti can be produced by an ejecta mass of 5.8 $M_\odot$ and a magnetar with a magnetic field of $B=1.8\times10^{13}$~G having an initial spin period of $P_0=1.8$ ms. Based on such a magnetar-powered scenario and a larger sample, a correlation between the spin of the magnetar and the kinetic energy of the ejecta can be inferred for most SLSNe~I, suggesting a self-consistent scenario. Like for other SLSNe~I, the host galaxy of SN 2018hti is found to be relatively faint ($M_{g} = -17.75$ mag) and of low metallicity ($Z=0.3~Z_\odot$), with a star-formation rate of 0.3 $M_\odot$ yr$^{-1}$. According to simulation results of single-star evolution, SN 2018hti could originate from a massive, metal-poor star with a zero-age main sequence (ZAMS) mass of 25--40 $M_\odot$, or from a less massive rotating star with $M_\mathrm{ZAMS} \approx 16$--25 $M_\odot$. For the case of a binary system, its progenitor could also be a star with $M_\mathrm{ZAMS} \gtrsim 25$ $M_\odot$.

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