TY - JOUR
T1 - An ALMA study of hub-filament systems - I. On the clump mass concentration within the most massive cores
AU - Anderson, Michael
AU - Peretto, Nicolas
AU - Ragan, Sarah E.
AU - Rigby, Andrew J.
AU - Avison, Adam
AU - Duarte-Cabral, Ana
AU - Fuller, Gary A.
AU - Shirley, Yancy L.
AU - Traficante, Alessio
AU - Williams, Gwenllian M.
N1 - Funding Information:
MA is supported by the Science and Technology Facilities Council (STFC). NP and AJR acknowledge the support of the STFC consolidated grant number ST/S00033X/1. ADC acknowledges the support from the Royal Society University Research Fellowship (URF/R1/191609). GMW acknowledges support from STFC under grant number ST/R000905/1. This paper makes use of the following ALMA data: ADS/JAO.ALMA#2011.0.00474.S, ADS/JAO.ALMA#2015.1.01014.S, ADS/JAO.ALMA#2016.1.00810.S, and ADS/JAO.ALMA#2013.1.00960.S. ALMA is a partnership of ESO (representing its member states), NSF (USA) and NINS (Japan), together with NRC (Canada), MOST and ASIAA (Taiwan), and KASI (Republic of Korea), in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated by ESO, AUI/NRAO, and NAOJ. We would like to thank Timea Csengeri for supplying us with the additional ALMA data. This research made use of the PYTHON packages ASTROPY6 (Astropy Collaboration 2013, 2018), ASTRODENDRO,7 IPYTHON8 (Ṕerez & Granger 2007), NUMPY9 (Harris et al. 2020), SCIPY10 (Virtanen et al. 2020), MATPLOTLIB11 (Hunter 2007), and SCIKIT-IMAGE12 (van der Walt et al. 2014). This research also made use of NASA's Astrophysics Data System Bibliographic Services, TOPCAT13 (Taylor 2005), and SAOImageDS914 (Joye & Mandel 2003).
Publisher Copyright:
© 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society.
PY - 2021/12/1
Y1 - 2021/12/1
N2 - The physical processes behind the transfer of mass from parsec-scale clumps to massive star-forming cores remain elusive. We investigate the relation between the clump morphology and the mass fraction that ends up in its most massive core (MMC) as a function of infrared brightness, i.e. a clump evolutionary tracer. Using Atacama Large Millimeter/submillimeter Array (ALMA) 12 m and Atacama Compact Array, we surveyed six infrared dark hubs in 2.9 mm continuum at ∼3 arcsec resolution. To put our sample into context, we also re-analysed published ALMA data from a sample of 29 high-mass surface density ATLASGAL sources. We characterize the size, mass, morphology, and infrared brightness of the clumps using Herschel and Spitzer data. Within the six newly observed hubs, we identify 67 cores, and find that the MMCs have masses between 15 and 911 M⊙ within a radius of 0.018-0.156 pc. The MMC of each hub contains 3-24 per cent of the clump mass (fMMC), becoming 5-36 per cent once core masses are normalized to the median core radius. Across the 35 clumps, we find no significant difference in the median fMMC values of hub and non-hub systems, likely the consequence of a sample bias. However, we find that fMMC is ∼7.9 times larger for infrared dark clumps compared to infrared bright ones. This factor increases up to ∼14.5 when comparing our sample of six infrared dark hubs to infrared bright clumps. We speculate that hub-filament systems efficiently concentrate mass within their MMC early on during its evolution. As clumps evolve, they grow in mass, but such growth does not lead to the formation of more massive MMCs.
AB - The physical processes behind the transfer of mass from parsec-scale clumps to massive star-forming cores remain elusive. We investigate the relation between the clump morphology and the mass fraction that ends up in its most massive core (MMC) as a function of infrared brightness, i.e. a clump evolutionary tracer. Using Atacama Large Millimeter/submillimeter Array (ALMA) 12 m and Atacama Compact Array, we surveyed six infrared dark hubs in 2.9 mm continuum at ∼3 arcsec resolution. To put our sample into context, we also re-analysed published ALMA data from a sample of 29 high-mass surface density ATLASGAL sources. We characterize the size, mass, morphology, and infrared brightness of the clumps using Herschel and Spitzer data. Within the six newly observed hubs, we identify 67 cores, and find that the MMCs have masses between 15 and 911 M⊙ within a radius of 0.018-0.156 pc. The MMC of each hub contains 3-24 per cent of the clump mass (fMMC), becoming 5-36 per cent once core masses are normalized to the median core radius. Across the 35 clumps, we find no significant difference in the median fMMC values of hub and non-hub systems, likely the consequence of a sample bias. However, we find that fMMC is ∼7.9 times larger for infrared dark clumps compared to infrared bright ones. This factor increases up to ∼14.5 when comparing our sample of six infrared dark hubs to infrared bright clumps. We speculate that hub-filament systems efficiently concentrate mass within their MMC early on during its evolution. As clumps evolve, they grow in mass, but such growth does not lead to the formation of more massive MMCs.
KW - ISM: clouds
KW - methods: observational
KW - stars: formation
KW - stars: massive
KW - submillimetre: ISM
KW - techniques: interferometric
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U2 - 10.1093/mnras/stab2674
DO - 10.1093/mnras/stab2674
M3 - Article
AN - SCOPUS:85119086289
SN - 0035-8711
VL - 508
SP - 2964
EP - 2978
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 2
ER -