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2024vjm 暗弱 Iax 型超新星在爆发后 200 天的 JWST 全波段观测与模型

Panchromatic JWST Observations and Models of the Dim Type Iax Supernova 2024vjm at 200 days

E Baron, J. M. DerKacy, C. Ashall, M. Shahbandeh, Peter H. Hauschildt, T. Barman, J. P. Aufdenberg, C. R. Burns, N. Morrell, M. D. Stritzinger, P. Hoeflich, K. Medler, E. Fereidouni, C. M. Pfeffer, T. Mera, W. B. Hoogendam, S. Shiber, P. J. Brown, Divya Mishra, Inma Dominguez, L. Galbany, Paolo Mazzali, E. Y. Hsiao, Huangfei Xiao, T. de Jaeger, S. Kumar

arXiv 2608.15040首次发表:更新:

AI 中文总结

本研究基于 JWST 观测 2024vjm 暗弱 Iax 型超新星爆发后 200 天的光谱与测光,用 PHOENIX/1D 模型开展研究,揭示了其尘埃、元素组成等特性,为 Iax 型超新星前身系统参数提供了严格约束。

AI 中文摘要

我们报告了在爆发后 202.8 静止帧天获得的暗弱 Iax 型超新星(SN Iax)2024vjm 的 JWST 光谱和测光数据。该光谱呈现出丰富的禁线,来自低电离、中等质量和铁族元素,其中值得注意的是[Ni II] 6.64 微米共振线,它是稳定镍的直接指标。在温暖尘埃连续谱中探测到强 CO 和 SiO 发射;这些光谱特性与预先存在的而非新形成的尘埃一致。我们使用通用恒星大气代码 PHOENIX/1D 结合简化的抛射体模型计算合成光谱。这些模型能够合理地重现整体光谱能量分布和分子发射特征,但大幅低估了中红外原子禁线的强度,导致合成光谱以分子发射为主。抑制分子不透明度的实验未能恢复禁线;相反,发射峰迁移到 2 微米附近的 Co 和 Fe 跃迁。我们将这种差异归因于碰撞速率约束不佳,以及当前抛射体模型中铁族物质可能过量。12.8 微米处的显著特征无法用[Ne II] 12.81 微米线很好地解释,表明该 12.8 微米特征可能主要源于[Fe III]。CO、SiO 和稳定镍的存在,加上未探测到氖,对 SN Iax 前身系统的总抛射体质量和核合成产额施加了严格约束。

英文摘要

We report JWST spectra and photometry of the underluminous SN Iax 2024vjm obtained 202.8 restframe days post-explosion. The spectrum exhibits a rich set of forbidden lines from low-ionization, intermediate-mass, and iron-group elements, notably the [Ni II] 6.64 micron resonance line, which is a direct indicator of stable nickel. Strong CO and SiO emission is detected alongside a warm dust continuum; the spectral properties are consistent with pre-existing rather than newly formed dust. Synthetic spectra were computed with the generalized stellar atmospheres code PHOENIX/1D using simplified ejecta models. The models reproduce the overall spectral energy distribution and the molecular emission features reasonably well, but substantially underestimate the strength of the mid-infrared atomic forbidden lines, leaving the synthetic spectrum dominated by molecular emission. Experiments in which the molecular opacity is suppressed do not recover the forbidden lines; instead, the emission peak migrates to Co and Fe transitions near 2 microns. We attribute this discrepancy to poorly constrained collisional rates and possibly to an excess of iron-group material in the current ejecta models. A prominent feature at 12.8 microns is not well accounted for by the [Ne II] 12.81 micron line, indicating that the 12.8 micron feature may be largely due to [Fe III]. The presence of CO, SiO, and stable nickel together with the non-detection of neon places tight constraints on the total ejecta mass and the nucleosynthetic yields of SNe Iax progenitor systems.

Comments19 pages, 10 figures, to appear in ApJ (Letters)

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