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arXiv 2403.20118astro-ph.GA
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JWST观测发现的z~6星系中的Balmer减量异常:密度有界星云还是激发态H I云?

Balmer Decrement Anomalies in Galaxies at z ~ 6 Found by JWST Observations: Density-Bounded Nebulae or Excited H I Clouds?

Hiroto Yanagisawa, Masami Ouchi, Kimihiko Nakajima, Hidenobu Yajima, Hiroya Umeda, Shunsuke Baba, Takao Nakagawa, Minami Nakane, Akinori Matsumoto, Yoshiaki Ono… 展开作者

Hiroto Yanagisawa, Masami Ouchi, Kimihiko Nakajima, Hidenobu Yajima, Hiroya Umeda, Shunsuke Baba, Takao Nakagawa, Minami Nakane, Akinori Matsumoto, Yoshiaki Ono, Yuichi Harikane, Yuki Isobe, Yi Xu, Yechi Zhang

AI总结:

通过物理建模研究z~6星系中Balmer减量异常的物理起源,发现密度有界星云和被光学厚激发H I云包围的电离有界星云两种机制可定量解释该异常,后者与高红移星系中由吸积和超新星引起的过度碰撞激发有关。

摘要:

我们研究了红移z~6处GS-NDG-9422(Cameron等 2023)和RXCJ2248-ID(Topping等 2024)星系中Balmer减量异常的物理起源,它们的Hα/Hβ值显著小于2.7,后者还显示出超出误差范围的异常Hγ/Hβ和Hδ/Hβ值。由于异常的Balmer减量无法在Case B复合下复现,我们通过物理建模探索了光学深度小于和大于Case B复合的星云。我们发现了两种能定量解释该异常的情况:1)仅在Lyγ-Ly8跃迁以下不透明的密度有界星云,以及2)部分/完全被光学厚激发H I云包围的电离有界星云。情况1)通过星云中的Lyγ吸收产生更多的Hβ光子,要求对光学深度值进行微调,同时该情况有助于电离光子逃逸以实现宇宙再电离。情况2)需要主量子数n=2的氢原子柱密度N2约为10^12-10^13 cm^-2的光学厚激发H I云。有趣的是,高N2值与近期关于GS-NDG-9422(需要大量2s态电子的强星云连续谱)和RXCJ2248-ID(可能存在与光学厚云共存的致密电离区)的结论在定性上一致。尽管光学厚激发H I云的物理起源尚不清楚,但这些结果可能表明高红移星系中存在由大量吸积和超新星引起的过度碰撞激发的气体云。

英文摘要:

We investigate the physical origins of the Balmer decrement anomalies in GS-NDG-9422 (Cameron et al. 2023) and RXCJ2248-ID (Topping et al. 2024) galaxies at $z\sim 6$ whose $\mathrm{H}α/\mathrm{H}β$ values are significantly smaller than $2.7$, the latter of which also shows anomalous $\mathrm{H}γ/\mathrm{H}β$ and $\mathrm{H}δ/\mathrm{H}β$ values beyond the errors. Because the anomalous Balmer decrements are not reproduced under the Case B recombination, we explore the nebulae with the optical depths smaller and larger than the Case B recombination by physical modeling. We find two cases quantitatively explaining the anomalies; 1) density-bounded nebulae that are opaque only up to around Ly$γ$-Ly8 transitions and 2) ionization-bounded nebulae partly/fully surrounded by optically-thick excited H{\sc i} clouds. The case of 1) produces more H$β$ photons via Ly$γ$ absorption in the nebulae, requiring fine tuning in optical depth values, while this case helps ionizing photon escape for cosmic reionization. The case of 2) needs the optically-thick excited H{\sc i} clouds with $N_2\simeq 10^{12}-10^{13}$ $\mathrm{cm^{-2}}$, where $N_2$ is the column density of the hydrogen atom with the principal quantum number of $n=2$. Interestingly, the high $N_2$ values qualitatively agree with the recent claims for GS-NDG-9422 with the strong nebular continuum requiring a number of $2s$-state electrons and for RXCJ2248-ID with the dense ionized regions likely coexisting with the optically-thick clouds. While the physical origin of the optically-thick excited H{\sc i} clouds is unclear, these results may suggest gas clouds with excessive collisional excitation caused by an amount of accretion and supernovae in the high-$z$ galaxies.

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