Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/8118
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dc.contributor.authorKim, Shinyoung-
dc.contributor.authorLee, Chang Won-
dc.contributor.authorTafalla, Mario-
dc.contributor.authorMaheswar, G-
dc.contributor.authorCaselli, Paola-
dc.contributor.authorMyers, Philip C-
dc.contributor.authorChung, Eun Jung-
dc.contributor.authorLi, Shanghuo-
dc.date.accessioned2023-01-18T06:09:51Z-
dc.date.available2023-01-18T06:09:51Z-
dc.date.issued2022-12-01-
dc.identifier.citationThe Astrophysical Journal, Vol. 940, No. 2, 112en_US
dc.identifier.issn1538-4357-
dc.identifier.urihttp://hdl.handle.net/2248/8118-
dc.descriptionOpen Accessen_US
dc.descriptionOriginal content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.-
dc.description.abstractWe present mapping results of two prestellar cores, L1544 and L694-2, embedded in filamentary clouds in C18O (3–2), 13CO (3–2), 12CO (3–2), HCO+ (4–3), and H13CO+ (4–3) lines with the James Clerk Maxwell Telescope to examine the role of the filamentary structures in the formation of dense cores in the clouds, with new distance estimates for L1544 ( - + 175 3 4 pc) and L694-2 ( - + 203 7 6 pc). From these observations, we found that the nonthermal velocity dispersion of two prestellar cores and their surrounding clouds is smaller than or comparable to the sound speed. This may indicate that the turbulence has already been dissipated for both filaments and cores during their formation time. We also found a λ/4 shift between the periodic oscillations in the velocity and the column density distributions, implying the possible presence of gravitational core-forming flow motion along the axis of the filament. The mass accretion rates due to these flow motions are estimated to be 2–3 Me Myr−1 , being comparable to that for Serpens cloud but much smaller than those for the Hub filaments, cluster, or high-mass forming filaments by 1 or 2 orders of magnitude. From this study, we suggest that the filaments in our targets might be formed from the shock compression of colliding clouds, and then the cores are formed by gravitational fragmentation of the filaments to evolve to the prestellar stage. We conclude that the filamentary structures in the clouds play an important role in the entire process of formation of dense cores and their evolution.en_US
dc.language.isoenen_US
dc.publisherAmerican Astronomical Societyen_US
dc.relation.urihttps://doi.org/10.3847/1538-4357/ac96e0-
dc.rights© 2022. The Author(s)-
dc.subjectStar formationen_US
dc.subjectStar forming regionsen_US
dc.subjectMolecular cloudsen_US
dc.subjectInterstellar filamentsen_US
dc.subjectInterstellar line emissionen_US
dc.subjectDust continuum emissionen_US
dc.titleThe Role of Filamentary Structures in the Formation of Two Dense Cores, L1544 and L694-2en_US
dc.typeArticleen_US
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