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arXiv 2303.09574astro-ph.GA
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Taurus Molecular Cloud B10 区域无星核的 3D 辐射转移建模与维里分析

3D Radiative Transfer Modelling and Virial Analysis of Starless Cores in the B10 Region of the Taurus Molecular Cloud

Samantha Scibelli, Yancy Shirley, Anika Schmiedeke, Brian Svoboda, Ayushi Singh, James Lilly, Paola Caselli

AI总结:

本文利用 NIKA2 仪器对 Taurus Molecular Cloud B10 区域的 14 个无星核进行高分辨率尘埃连续谱观测,结合 3D 辐射转移建模与维里分析,揭示了其内部密度结构、尘埃发射率指数及稳定性,发现约 64% 的核在引力或外部压力下处于维里平衡或束缚状态。

摘要:

像我们太阳这样的低质量恒星在冷(10 K)且致密($\sim 10^5$ cm$^{-3}$)的气体和尘埃核内开始其演化。无星核的物理结构最好通过尘埃颗粒的热发射来探测。我们展示了对 Taurus Molecular Cloud B10 区域无星核的高分辨率尘埃连续谱研究。利用 IRAM 30m 上的 NIKA2 仪器在 1.2mm 和 2.0mm($12^{

英文摘要:

Low-mass stars like our Sun begin their evolution within cold (10 K) and dense ($\sim 10^5$ cm$^{-3}$) cores of gas and dust. The physical structure of starless cores is best probed by thermal emission of dust grains. We present a high resolution dust continuum study of the starless cores in the B10 region of the Taurus Molecular Cloud. New observations at 1.2mm and 2.0mm ($12^{"}$ and $18^{"}$ resolution) with the NIKA2 instrument on the IRAM 30m have probed the inner regions of 14 low-mass starless cores. We perform sophisticated 3D radiative transfer modelling for each of these cores through the radiative transfer framework $\textit{pandora}$, which utilizes RADMC-3D. Model best-fits constrain each cores' central density, density slope, aspect ratio, opacity, and interstellar radiation field strength. These `typical' cores in B10 span central densities from $5 \times 10^4 - 1 \times 10^6$ cm$^{-3}$, with a mean value of $2.6 \times 10^5$ cm$^{-3}$. We find the dust opacity laws assumed in the 3D modelling, as well as the estimates from $\textit{Herschel}$, have dust emissivity indices, $β$'s, on the lower end of the distribution constrained directly from the NIKA2 maps, which averages to $β= 2.01\pm0.48$. From our 3D density structures and archival NH$_3$ data, we perform a self-consistent virial analysis to assess each core's stability. Ignoring magnetic field contributions, we find 9 out of the 14 cores ($64\%$) are either in virial equilibrium or are bound by gravity and external pressure. To push the bounded cores back to equilibrium, an effective magnetic field difference of only $\sim 15 μ$G is needed.

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