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The survey for ionization in neutral gas galaxies. III. Diffuse, warm ionized medium and escape of ionizing radiation

机译:中性气体星系中电离的调查。三,扩散,温暖的电离介质和电离辐射的逸出

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摘要

We use the first data release from the SINGG H alpha survey of H I-selected galaxies to study the quantitative behavior of the diffuse, warm ionized medium (WIM) across the range of properties represented by these 109 galaxies. The mean fraction f(WIM) of diffuse ionized gas in this sample is 0: 59 +/- 0: 19, slightly higher than found in previous samples. Since lower surface brightness galaxies tend to have higher f(WIM), we believe that most of this difference is due to selection effects favoring large, optically bright, nearby galaxies with high star formation rates. As found in previous studies, there is no appreciable correlation with Hubble type or total star formation rate. However, we find that starburst galaxies, defined here by an H alpha surface brightness > 2: 5; 10(39) erg s(-1) kpc (-2) within the H alpha half-light radius, do show much lower fractions of diffuse H alpha emission. The cause apparently is not dominated by a lower fraction of field OB stars. However, it is qualitatively consistent with an expected escape of ionizing radiation above a threshold star formation rate, predicted from our model in which the ISM is shredded by pressure-driven supernova feedback. The H I gas fractions in the starburst galaxies are also lower, suggesting that the starbursts are consuming and ionizing all the gas, and thus promoting regions of density-bounded ionization. If true, these effects imply that some amount of Lyman continuum radiation is escaping from most starburst galaxies, and that WIM properties and outflows from mechanical feedback are likely to be pressure-driven. However, in view of previous studies showing that the escape fraction of ionizing radiation is generally low, it is likely that other factors also drive the low fractions of diffuse ionized gas in starbursts.
机译:我们使用来自HI选星系的SINGG H alpha调查的第一批数据来研究由这109个星系代表的性能范围内的弥散性热电离介质(WIM)的定量行为。该样品中弥散离子化气体的平均分数f(WIM)为0:59 +/- 0:19,比以前的样品中发现的稍高。由于较低表面亮度的星系倾向于具有较高的f(WIM),因此我们认为,这种差异的大部分归因于选择效应,这些选择效应有利于具有高恒星形成率的大型,光学明亮的附近星系。如先前的研究发现,与哈勃类型或总恒星形成率没有明显的相关性。但是,我们发现星爆星系在这里定义为H alpha表面亮度> 2:5; H alpha半光半径内的10(39)erg s(-1)kpc(-2)确实显示了较低的弥散H alpha发射分数。原因显然不是由较低比例的实地OB星所主导。但是,它在质量上与预期的电离辐射在阈值恒星形成速率以上的预期逃逸一致,这是根据我们的模型预测得出的,在该模型中,ISM被压力驱动的超新星反馈所压缩。星暴星系中的H I气体分数也较低,这表明星暴正在消耗并电离所有气体,从而促进了密度约束电离区域。如果为真,则这些影响意味着大多数星爆星系中逃逸了一些莱曼连续谱辐射,并且WIM属性和机械反馈的流出很可能是压力驱动的。但是,鉴于先前的研究表明电离辐射的逸散率通常较低,很可能其他因素也驱使了星爆中低比例的弥散电离气体。

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