2025A&A...704A.149G -
Astronomy and Astrophysics, volume 704A149 (2025/12-1)
Multi-scale view of the S-shaped high-mass star-forming filament IRAS 19074+0752 observed as part of the INFANT survey.
GUO Y.Q., LIU H.-L., LU X., CHENG Y., LIU H.B., ZHEN L.M., ZHANG Q., JIAO S.H., LIU X.C., LIU T., GALVAN-MADRID R., SANHUEZA P., YANG D.T., NAKAMURA F., CHEN L., FENG S.Y., WANG K., GU Q.L., LUO Q.Y., LIN Y., LI P.S., LI S.H., TANAKA K. and GUZMAN A.E.
Abstract (from CDS):
Context. It is generally accepted that high-mass stars form through a hierarchical, multi-scale fragmentation process that range from molecular clouds down to individual protostars, involving intermediate scales such as filaments. However, a comprehensive understanding of this process remains limited due to the lack of high-resolution, multi-scale observational studies that would simultaneously probe the physical conditions across the full hierarchy of star-forming structures. Aims. We aim to understand a coherent picture of the physical processes connecting filament formation, fragmentation, and dynamical scenario of high-mass star formation in the IRAS 19074+0752 (hereafter I19074) region. Methods. Primarily using new 1.3 mm continuum mosaicked observations, as part of the ALMA-INFANT survey, we analyzed the S-shaped filamentary cloud I19074 at a ∼6000 AU resolution. Leveraging the multi-scale information, we investigated the filament and clump fragmentation properties, such as core separations and masses. Results. ALMA 1.3 mm dust continuum emission reveals that the S-shaped filament consists of two physically connected components: a southern (Fs) and a northern (Fn) segment. Fn is associated with an infrared (IR)-bright HII region, while Fs appears IR-dark. The total filament length is ∼2.8 pc, with Fn and Fs spanning ∼1.0 pc and ∼1.8 pc, respectively. Their masses are ∼250-910 M⊙, while their line masses (∼250-360 M⊙ pc–1) exceed the critical value for turbulence support, indicating they are gravitationally bound. The S-shaped morphology likely results from the expansion of the HII region, which swept up and compressed the northern part of the pre-existing filament into an arc-like structure in Fn; meanwhile, Fs retained a more linear form due to its greater distance from the ionized gas. Accordingly, a hybrid scenario could be responsible for Fn formation, which would combine the compression of a preexisting filament by the HII region with fresh gas accumulation into the shocked-compression layer. We extracted 26 dense cores from 1.3 mm emission with masses between 1.0 and 22.9 M⊙, with most (92%) being gravitationally bound (αvir ≤ 2). The core separations lack periodicity; instead, four core groups define four clumps (clumps 1-4) with masses of 110-620 M⊙. In the Fs segment, clump 1 at its southern end could be a product of edge fragmentation, while Fn exhibits hierarchical fragmentation modes: the filamentary mode responsible for clump formation within Fn and the spherical Jeans-like mode for core formation within clumps. Hierarchical fragmentation mechanisms are identified as shocked turbulence-driven within Fn and gravity-driven inside the clumps. Most cores have high mass surface densities of Σcore ≥ 1 g cm–2, but with no robust identification of high-mass prestellar candidates. This favors dynamical clump-fed accretion-type over core-fed accretion-type models for high-mass star formation in I19074. Conclusions. The S-shaped filament in the I19074 region likely formed through the interaction with an expanding H II region, with the shocked-shell fragmentation mechanism in Fn and edge fragmentation in Fs serving as pathways for producing massive, star-forming clumps. Both mechanisms contribute to high-mass star formation via a dynamical clump-fed accretion process within their respective filamentary segments.
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