论文标题

哪些反馈机制在中央分子区的高压环境中占主导地位?

Which feedback mechanisms dominate in the high-pressure environment of the Central Molecular Zone?

论文作者

Barnes, Ashley T., Longmore, Steven N., Dale, James E., Krumholz, Mark R., Kruijssen, J. M. Diederik, Bigiel, Frank

论文摘要

Supernovae(SNE)主导了恒星反馈的能量和动量预算,但是它们将它们融合到星际介质(ISM)的效率在很大程度上取决于早期的有效,预先SN的反馈清除了星形形成区域的密集气体。在低ISM压力环境中,早期恒星反馈的幅度和时间表上存在观察性的限制,但是对于更典型的典型高ISM压力环境而言,没有这种限制。在本文中,我们确定了HII区域扩展的机制,这是高压内尺寸尺度和进化时间的函数($ p/k_ \ rm {b} $〜$〜$ 10^{7-8} $ k cm $ $^{ - 3} $在Milky Way Inner 100pc中的环境。我们计算了温暖离子化的热压($ p_ \ rm {hii} $; 10 $^{4} $ k)气体,直接辐射压力($ p_ \ rm {dir} $)和灰尘处理的辐射压力($ p_ \ p_ \ rm {ir {ir} $)。我们发现(1)$ p_ \ rm {dir} $在小尺度和早期(0.01-0.1pc; $ <$ <0.10万)上占据了扩展; (2)扩展是由$ p_ \ rm {hii} $在以后的进化阶段($> 0.1 $ pc; $> 1 $ myr)驱动的; (3)在第一个〜1myr的增长期间,但此后没有,$ p _ {\ rm ir} $或恒星风压可能会产生可比的贡献。尽管环境的狭窄压力很高,但在〜2myr内,即在第一次SNE爆炸之前,将出生恒星形成的气体有效地清除了几个PC的半径。这种“预处理”是指随后的SNE会爆炸到低密度气体中,因此它们的能量和动量将有效地与ISM搭配。我们发现HII区域扩展到3pc的半径,此时它们的内部压力与周围的外部压力相等。在较低压力环境中与HII区域的比较表明,所有HII区域的最大尺寸均由压力平衡与环境ISM设置。

Supernovae (SNe) dominate the energy and momentum budget of stellar feedback, but the efficiency with which they couple to the interstellar medium (ISM) depends strongly on how effectively early, pre-SN feedback clears dense gas from star-forming regions. There are observational constraints on the magnitudes and timescales of early stellar feedback in low ISM pressure environments, yet no such constraints exist for more cosmologically typical high ISM pressure environments. In this paper, we determine the mechanisms dominating the expansion of HII regions as a function of size-scale and evolutionary time within the high-pressure ($P/k_\rm{B}$~$10^{7-8}$K cm$^{-3}$) environment in the inner 100pc of the Milky Way. We calculate the thermal pressure from the warm ionised ($P_\rm{HII}$; 10$^{4}$K) gas, direct radiation pressure ($P_\rm{dir}$), and dust processed radiation pressure ($P_\rm{IR}$). We find that (1) $P_\rm{dir}$ dominates the expansion on small scales and at early times (0.01-0.1pc; $<$0.1Myr); (2) the expansion is driven by $P_\rm{HII}$ on large scales at later evolutionary stages ($>0.1$pc; $>1$Myr); (3) during the first ~1Myr of growth, but not thereafter, either $P_{\rm IR}$ or stellar wind pressure likely make a comparable contribution. Despite the high confining pressure of the environment, natal star-forming gas is efficiently cleared to radii of several pc within ~2Myr, i.e. before the first SNe explode. This `pre-processing' means that subsequent SNe will explode into low density gas, so their energy and momentum will efficiently couple to the ISM. We find the HII regions expand to a radius of 3pc, at which point they have internal pressures equal with the surrounding external pressure. A comparison with HII regions in lower pressure environments shows that the maximum size of all HII regions is set by pressure equilibrium with the ambient ISM.

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