论文标题

了解分子云中的恒星形成IV。柱密度PDF从静止到巨大的分子云

Understanding star formation in molecular clouds IV. Column density PDFs from quiescent to massive molecular clouds

论文作者

Schneider, N., Ossenkopf-Okada, V., Clarke, S., Klessen, R. S., Kabanovic, S., Veltchev, T., Bontemps, S., Dib, S., Csengeri, T., Federrath, C., Di Francesco, J., Motte, F., Andre, Ph., Arzoumanian, D., Beattie, J. R., Bonne, L., Didelon, P., Elia, D., Koenyves, V., Kritsuk, A., Ladjelate, B., Myers, Ph., Pezzuto, S., Robitaille, J. F., Roy, A., Seifried, D., Simon, R., Soler, J., Ward-Thompson, D.

论文摘要

我们介绍了以高角度分辨率从Herschel成像获得的29个银河系区域的N-PDF,覆盖了弥漫性和静态云,以及显示出低,中间和高质量星形成(SF)的N-PDF,并使用Delta-Variance工具表征云结构。 N-PDF在低柱密度下是双重差异,并在较高的柱密度下显示一两个电源法尾(PLT)。对于弥漫性,静止和低质量SF云,我们提出两个对数正常函数分别来自原子和分子相。对于巨大的云层,我们建议第一个对数正态是由湍流混合的H2和第二个对数 - 通过压缩(通过恒星反馈)分子气体构建的。几乎所有的云都具有两个与自我重力一致的斜率的PLT,第二个云可以比第一个云更平坦或更陡。恒星的反馈或其他物理过程可能会引起平坦的plt,从而减慢崩溃并减少质量向更高密度的流动。如果磁场的定向垂直于LOS柱密度分布,则可能会出现较高的斜率。第一个偏差点(DP),其中n-PDF从对数正态转换为PLT,显示了2-5左右的AV(DP1)视觉灭绝值的聚类。定义两个PLT之间断裂的第二个DP差异很大。使用三角变量,我们观察到,斜率在第一和第二个PLT之间变化的AV值随方差频谱中的特征尺寸尺度而增加。我们得出的结论是,在低柱密度下,原子和分子气体被湍流混合,而在高柱密度下,气体是完全分子的,并由自重力支配。因此,分子云的最佳拟合模型N-PDF是具有对数正态低柱密度分布的一个,其次是一个或两个PLT。

We present N-PDFs of 29 Galactic regions obtained from Herschel imaging at high angular resolution, covering diffuse and quiescent clouds, and those showing low-, intermediate-, and high-mass star formation (SF), and characterize the cloud structure using the Delta-variance tool. The N-PDFs are double-log-normal at low column densities, and display one or two power law tails (PLTs) at higher column densities. For diffuse, quiescent, and low-mass SF clouds, we propose that the two log-normals arise from the atomic and molecular phase, respectively. For massive clouds, we suggest that the first log-normal is built up by turbulently mixed H2 and the second one by compressed (via stellar feedback) molecular gas. Nearly all clouds have two PLTs with slopes consistent with self-gravity, where the second one can be flatter or steeper than the first one. A flatter PLT could be caused by stellar feedback or other physical processes that slow down collapse and reduce the flow of mass toward higher densities. The steeper slope could arise if the magnetic field is oriented perpendicular to the LOS column density distribution. The first deviation point (DP), where the N-PDF turns from log-normal into a PLT, shows a clustering around values of a visual extinction of AV (DP1) around 2-5. The second DP, which defines the break between the two PLTs, varies strongly. Using the Delta-variance, we observe that the AV value, where the slope changes between the first and second PLT, increases with the characteristic size scale in the variance spectrum. We conclude that at low column densities, atomic and molecular gas is turbulently mixed, while at high column densities, the gas is fully molecular and dominated by self-gravity. The best fitting model N-PDFs of molecular clouds is thus one with log-normal low column density distributions, followed by one or two PLTs.

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