论文标题

phangs-jwst首先结果:中红外发射迹线在100 pc尺度上同时使用气柱密度和加热

PHANGS-JWST First Results: Mid-infrared emission traces both gas column density and heating at 100 pc scales

论文作者

Leroy, Adam K., Sandstrom, Karin, Rosolowsky, Erik, Belfiore, Francesco, Bolatto, Alberto D., Cao, Yixian, Koch, Eric W., Schinnerer, Eva, Barnes, Ashley. T., Bešlić, Ivana, Bigiel, F., Blanc, Guillermo A., Chastenet, Jérémy, Chen, Ness Mayker, Chevance, Mélanie, Chown, Ryan, Congiu, Enrico, Dale, Daniel A., Egorov, Oleg V., Emsellem, Eric, Eibensteiner, Cosima, Faesi, Christopher M., Glover, Simon C. O., Grasha, Kathryn, Groves, Brent, Hassani, Hamid, Henshaw, Jonathan D., Hughes, Annie, Jiménez-Donaire, María J., Kim, Jaeyeon, Klessen, Ralf S., Kreckel, Kathryn, Kruijssen, J. M. Diederik, Larson, Kirsten L., Lee, Janice C., Levy, Rebecca C., Liu, Daizhong, Lopez, Laura A., Meidt, Sharon E., Murphy, Eric J., Neumann, Justus, Pessa, Ismael, Pety, Jérôme, Saito, Toshiki, Sardone, Amy, Sun, Jiayi, Thilker, David A., Usero, Antonio, Watkins, Elizabeth J., Whitcomb, Cory M., Williams, Thomas G.

论文摘要

我们比较了前四个phangs-jwst目标中的70---160 PC分辨率的中红外(MID-IR),通过灭绝校正的H $α$和CO(2-1)发射。我们报告的相关强度,强度比和功率法符合JWST的F770W,F1000W,F1130W和F2100W频段与CO和H $α$相关的发射。在这些尺度上,CO和H $α$每个都与MID-IR的发射密切相关,并且这些相关性都比与H $α$发射的CO相关的相关性强。这反映出MID-IR发射同时充当尘埃柱密度示踪剂,从而与分子气体跟踪CO和加热示踪剂相匹配,从而与H $α$相匹配。通过将MID-IR,CO和H $α$相结合,在尺度上,冷气和恒星形成之间的总体相关性开始分解,我们可以分开这两种效果。我们在F770W上对MID-IR建模高于$I_ν= 0.5 $ 〜MJY SR $^{ - 1} $,该切割旨在选择分子气体主导星际介质(ISM)质量的区域。可以通过结合共同追踪组件和H $α$跟踪组件的模型来描述这种光明发射。最合适的型号表明,MID-IR通量的$ \ sim 50 \%$是由弥漫性星际辐射场加热的分子气,其余的$ \ sim 50 \%$与明亮,尘土飞扬的恒星形成区域相关。我们讨论F770W,F1000W,F1130W频段和连续体主导的F2100W频段之间的差异,并建议将MID-IR用作ISM Tracer的下一步步骤。

We compare mid-infrared (mid-IR), extinction-corrected H$α$, and CO (2-1) emission at 70--160 pc resolution in the first four PHANGS-JWST targets. We report correlation strengths, intensity ratios, and power law fits relating emission in JWST's F770W, F1000W, F1130W, and F2100W bands to CO and H$α$. At these scales, CO and H$α$ each correlate strongly with mid-IR emission, and these correlations are each stronger than the one relating CO to H$α$ emission. This reflects that mid-IR emission simultaneously acts as a dust column density tracer, leading to the good match with the molecular gas-tracing CO, and as a heating tracer, leading to the good match with the H$α$. By combining mid-IR, CO, and H$α$ at scales where the overall correlation between cold gas and star formation begins to break down, we are able to separate these two effects. We model the mid-IR above $I_ν= 0.5$~MJy sr$^{-1}$ at F770W, a cut designed to select regions where the molecular gas dominates the interstellar medium (ISM) mass. This bright emission can be described to first order by a model that combines a CO-tracing component and an H$α$-tracing component. The best-fitting models imply that $\sim 50\%$ of the mid-IR flux arises from molecular gas heated by the diffuse interstellar radiation field, with the remaining $\sim 50\%$ associated with bright, dusty star forming regions. We discuss differences between the F770W, F1000W, F1130W bands and the continuum dominated F2100W band and suggest next steps for using the mid-IR as an ISM tracer.

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