论文标题

kmos $^{\ rm 3d} $调查:调查恒星形成星系中高架电子密度的起源,$ 1 \ sillesim {z} \ sillesim {3} $

The KMOS$^{\rm 3D}$ Survey: Investigating the Origin of the Elevated Electron Densities in Star-Forming Galaxies at $1\lesssim{z}\lesssim{3}$

论文作者

Davies, Rebecca L., Schreiber, N. M. Förster, Genzel, R., Shimizu, T. T., Davies, R. I., Schruba, A., Tacconi, L. J., Übler, H., Wisnioski, E., Wuyts, S., Fossati, M., Herrera-Camus, R., Lutz, D., Mendel, J. T., Naab, T., Price, S. H., Renzini, A., Wilman, D., Beifiori, A., Belli, S., Burkert, A., Chan, J., Contursi, A., Fabricius, M., Lee, M. M., Saglia, R. P., Sternberg, A.

论文摘要

我们使用主要来自KMOS $^{\ rm 3D} $($ 0.6 \ simsim {z} \ simeSim {2.6} $)的140个星系示例,研究了典型电子密度($ n_e $)的典型电子密度($ n_e $)的红移演化的原因,该$ nsemi($ 0.6 \ simsim {z} \ sameim {2.6} $)<0.113.113。我们选择没有显示AGN活性或流出证据的星系,以限制H II区域内的平均条件。 [SII] $λ$ 6716/[SII] $λ$ 6731比例的四个红移箱的测量表明,线条发射材料中的本地$ n_e $从187 $^{+140} _ {+140} _ { - 132} $ CM $^{-132} $ CM $^{ - 3} $ 2.2 32 $^{+4} _ { - 9} $ cm $^{ - 3} $ at $ z \ sim $ 0;与以前的结果一致。我们使用h $α$光度来估计每个红移在恒星形成磁盘上平均的根平方(RMS)$ n_e $。本地和体积平均$ n_e $以相似的速度进化,暗示在$ 0 \ 0 \ sillesim {z} \ sillesim {2.6} $上,发射线发气的体积填充因子可能大约是恒定的。 The KMOS$^{\rm 3D}$ and SAMI galaxies follow a roughly monotonic trend between $n_e$ and star formation rate, but the KMOS$^{\rm 3D}$ galaxies have systematically higher $n_e$ than the SAMI galaxies at fixed offset from the star-forming main sequence, suggesting a link between the $n_e$ evolution and the evolving main sequence归一化。我们定量测试密度演化的潜在驱动因素,并发现$ n_e $(rms)$ \ simeq {n_ {h_2}} $,这表明高高的$ n_e $在高$ z $ h ii区域中可能是父母分子云中较高密度的直接结果。还有暂定的证据表明,$ n_e $可能会受到恒星反馈之间的平衡,该反馈驱动了H II地区的扩张和抵抗其扩张的环境压力。

We investigate what drives the redshift evolution of the typical electron density ($n_e$) in star-forming galaxies, using a sample of 140 galaxies drawn primarily from KMOS$^{\rm 3D}$ ($0.6\lesssim{z}\lesssim{2.6}$) and 471 galaxies from SAMI ($z<0.113$). We select galaxies that do not show evidence of AGN activity or outflows, to constrain the average conditions within H II regions. Measurements of the [SII]$λ$6716/[SII]$λ$6731 ratio in four redshift bins indicate that the local $n_e$ in the line-emitting material decreases from 187$^{+140}_{-132}$ cm$^{-3}$ at $z\sim$ 2.2 to 32$^{+4}_{-9}$ cm$^{-3}$ at $z\sim$ 0; consistent with previous results. We use the H$α$ luminosity to estimate the root-mean-square (rms) $n_e$ averaged over the volumes of star-forming disks at each redshift. The local and volume-averaged $n_e$ evolve at similar rates, hinting that the volume filling factor of the line-emitting gas may be approximately constant across $0\lesssim{z}\lesssim{2.6}$. The KMOS$^{\rm 3D}$ and SAMI galaxies follow a roughly monotonic trend between $n_e$ and star formation rate, but the KMOS$^{\rm 3D}$ galaxies have systematically higher $n_e$ than the SAMI galaxies at fixed offset from the star-forming main sequence, suggesting a link between the $n_e$ evolution and the evolving main sequence normalization. We quantitatively test potential drivers of the density evolution and find that $n_e$(rms) $\simeq{n_{H_2}}$, suggesting that the elevated $n_e$ in high-$z$ H II regions could plausibly be the direct result of higher densities in the parent molecular clouds. There is also tentative evidence that $n_e$ could be influenced by the balance between stellar feedback, which drives the expansion of H II regions, and the ambient pressure, which resists their expansion.

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