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arXiv 2403.14751astro-ph.GA
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GOALS-JWST:合并星暴星系 NGC 3256 的暖分子外流

GOALS-JWST: The Warm Molecular Outflows of the Merging Starburst Galaxy NGC 3256

Thomas Bohn, Hanae Inami, Aditya Togi, Lee Armus, Thomas S. -Y. Lai, Loreto Barcos-Munoz, Yiqing Song, Sean T. Linden, Jason Surace, Marina Bianchin, Vivian U, … 展开作者

Thomas Bohn, Hanae Inami, Aditya Togi, Lee Armus, Thomas S. -Y. Lai, Loreto Barcos-Munoz, Yiqing Song, Sean T. Linden, Jason Surace, Marina Bianchin, Vivian U, Aaron S. Evans, Torsten Böker, Matthew A. Malkan, Kirsten L. Larson, Sabrina Stierwalt, Victorine A. Buiten, Vassilis Charmandaris, Tanio Diaz-Santos, Justin H. Howell, George C. Privon, Claudio Ricci, Paul P. van der Werf, Susanne Aalto, Christopher C. Hayward, Justin A. Kader, Joseph M. Mazzarella, Francisco Muller-Sanchez, David B. Sanders

AI总结:

本文利用 JWST/NIRSpec 和 MIRI 观测数据研究了合并星系 NGC 3256 核区的暖分子 H2 外流,测得南核外流速度约 1000 km/s,质量外流率为 2.0±0.8 太阳质量/年,并发现外流引发了机械加热但未显著改变 PAH 特征。

摘要:

我们展示了 James Webb Space Telescope (JWST) 积分场光谱仪对 NGC 3256 的观测结果,这是一个本地红外亮度的晚期合并系统,具有两个相距约 1 kpc 的核,两者均有冷分子外流的证据。使用 JWST/NIRSpec 和 MIRI 数据集,我们在 <100 pc 的空间尺度上研究这个形态复杂的系统,重点关注核周围的暖分子 H2 气体。我们检测到源自南核的准直外流暖 H2 气体,尽管我们没有发现北核周围有显著的外流 H2 气体。我们测得的最大本征外流速度约为 1,000 km s^-1,延伸至 0.7 kpc 的距离。基于 H2 S(7)/S(1) 比率,我们在南核附近发现更大比例的较暖气体,该比例随距核距离增加而降低,表明南核是 H2 加热的主要来源。暖 H2 外流分量的气体质量估计为 M_warm,out=(1.4±0.2)×10^6 M_sun,高达使用 ALMA CO 数据估计的冷 H2 质量的 6%。外流时间尺度约为 7×10^5 年,导致质量外流率 M_dot_warm,out=2.0±0.8 M_sun yr^-1 和动能功率 P_warm,out ~ 4×10^41 erg s^-1。最后,在我们 3.0"x3.0" NIRSpec 数据内外流气体所在的区域显示出高 [Fe II]/Paβ 和 H2/Brγ 谱线比率,表明外流引起了增强的机械加热。这些区域中多环芳烃 (PAH) 的通量和比率与盘上其他区域相比没有显著差异,表明外流可能不会显著改变 PAH 的电离状态或晶粒尺寸。

英文摘要:

We present James Webb Space Telescope (JWST) Integral Field Spectrograph observations of NGC 3256, a local infrared-luminous late-stage merging system with two nuclei roughly 1$\;\rm{kpc}$ apart, both of which have evidence of cold molecular outflows. Using JWST/NIRSpec and MIRI datasets, we investigate this morphologically complex system on spatial scales of $<$100$\;\rm{pc}$, where we focus on the warm molecular H$_2$ gas surrounding the nuclei. We detect collimated outflowing warm H$_2$ gas originating from the southern nucleus, though we do not find significant outflowing H$_2$ gas surrounding the northern nucleus. We measure maximum intrinsic outflow velocities of $\sim$1,000$\;\rm{km}\;\rm{s}^{-1}$, which extend out to a distance of 0.7$\;\rm{kpc}$. Based on H$_2$ S(7)/S(1) ratios, we find a larger fraction of warmer gas near the S nucleus, which decreases with increasing distance from the nucleus, signifying the southern nucleus as a primary source of H$_2$ heating. The gas mass of the warm H$_2$ outflow component is estimated to be $M\rm{_{warm,out}}=(1.4\pm0.2)\times10^6\;\rm{M}_{\odot}$, as much as 6$\%$ of the cold H$_2$ mass estimated using ALMA CO data. The outflow time scale is about $7\times10^5\;\rm{yr}$, resulting in a mass outflow rate $\dot{M}\rm{_{warm,out}}=2.0\pm0.8\;\rm{M}_{\odot}\;\rm{yr}^{-1}$ and kinetic power $P\rm{_{warm,out}}\;\sim\;4\times10^{41}\;\rm{erg}\;\rm{s}^{-1}$. Lastly, regions within our 3.0"x3.0" NIRSpec data where the outflowing gas reside show high [Fe II]/Pa$β$ and H$_2$/Br$γ$ line ratios, indicate enhanced mechanical heating caused by the outflows. The fluxes and ratios of Polycyclic Aromatic Hydrocarbons (PAH) in these regions are not significantly different compared to those elsewhere in the disk, suggesting the outflows may not significantly alter the PAH ionization state or grain size.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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