4.7 Article

Gas kinematics and excitation in the filamentary IRDC G035.39-00.33

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 439, Issue 2, Pages 1996-2013

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stu078

Keywords

stars: formation; ISM: individual objects: G035.39-00.33; ISM: molecules

Funding

  1. European Union [PIIF-GA-2011-301538]
  2. UK Science and Technology Funding Council
  3. European Research Council (ERC) [PALs 320620]
  4. Deutsche Forschungsgemeinschaft [1573]
  5. INSU/CNRS (France)
  6. MPG (Germany)
  7. IGN (Spain)
  8. STFC [ST/L000628/1, ST/I505772/1] Funding Source: UKRI
  9. Science and Technology Facilities Council [ST/I505772/1] Funding Source: researchfish

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Some theories of dense molecular cloud formation involve dynamical environments driven by converging atomic flows or collisions between preexisting molecular clouds. The determination of the dynamics and physical conditions of the gas in clouds at the early stages of their evolution is essential to establish the dynamical imprints of such collisions, and to infer the processes involved in their formation. We present multitransition (CO)-C-13 and (CO)-O-18 maps towards the IRDC G035.39-00.33, believed to be at the earliest stages of evolution. The (CO)-C-13 and (CO)-O-18 gas is distributed in three filaments (Filaments 1, 2 and 3), where the most massive cores are preferentially found at the intersecting regions between them. The filaments have a similar kinematic structure with smooth velocity gradients of similar to 0.4-0.8 km s(-1) pc(-1). Several scenarios are proposed to explain these gradients, including cloud rotation, gas accretion along the filaments, global gravitational collapse and unresolved sub-filament structures. These results are complemented by HCO+, HNC, (HCO+)-C-13 and (HNC)-C-13 single-pointing data to search for gas infall signatures. The (CO)-C-13 and (CO)-O-18 gas motions are supersonic across G035.39-00.33, with the emission showing broader linewidths towards the edges of the infrared dark cloud (IRDC). This could be due to energy dissipation at the densest regions in the cloud. The average H-2 densities are similar to 5000-7000 cm(-3), with Filaments 2 and 3 being denser and more massive than Filament 1. The (CO)-O-18 data unveil three regions with high CO depletion factors (f(D) similar to 5-12), similar to those found in massive starless cores.

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