Hostname: page-component-848d4c4894-xfwgj Total loading time: 0 Render date: 2024-06-30T20:19:59.846Z Has data issue: false hasContentIssue false

Kinematic and thermal structure at the onset of high-mass star formation - ISOSS23053

Published online by Cambridge University Press:  31 March 2017

Simon Bihr
Affiliation:
Max Planck Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany email: [email protected]
Henrik Beuther
Affiliation:
Max Planck Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany email: [email protected]
Hendrik Linz
Affiliation:
Max Planck Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany email: [email protected]
Sarah E. Ragan
Affiliation:
School of Physics & Astronomy, The University of Leeds, E.C. Stoner Building, Leeds, LS2 9JT, UK email: [email protected]
Jochen Tackenberg
Affiliation:
Max Planck Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany email: [email protected]
Rowan J. Smith
Affiliation:
Jodrell Bank Centre for Astrophysics, University of Manchester, Oxford Road, Manchester, M13 9PL, UK email: [email protected]
Thomas Henning
Affiliation:
Max Planck Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany email: [email protected]
Oliver Krause
Affiliation:
Max Planck Institute for Astronomy, Königstuhl 17, 69117 Heidelberg, Germany email: [email protected]
Rights & Permissions [Opens in a new window]

Abstract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

Within the ‘earliest phases of star formation’ (EPoS) Herschel project, we observed the NH3 inversion lines of 6 very young high-mass star-forming regions at high spatial resolution (3-5″) with the JVLA. While the Herschel data provide details about the dust continuum, the ammonia data reveal the kinematics and temperatures. Here we present the exciting star-forming clump ISOSS23053 that shows multiple velocity components. We observe a prominent velocity step within the clump, which could be a sign of colliding or converging flows that triggers star formation. Furthermore, we used the JVLA in the C-array configuration to study this source in more detail and we present the first results from the new data. They support the idea of converging flows, as we observe two components in the NH3(1,1) and (2,2) line, whereas the higher excited NH3(3,3) line shows one component that links the two lower excited lines.

Type
Contributed Papers
Copyright
Copyright © International Astronomical Union 2017 

References

Bihr, S., Beuther, H., Linz, H., et al. 2015, A&A, 579, A51 Google Scholar
Birkmann, S. M., Krause, O., Hennemann, M., et al. 2007, A&A, 474, 883 Google Scholar
Bonnell, I. A., Vine, S. G., & Bate, M. R. 2004, MNRAS, 349, 735 Google Scholar
Klessen, R. S., Ballesteros-Paredes, J., Vázquez-Semadeni, E., & Durán-Rojas, C. 2005, ApJ, 620, 786 Google Scholar
Ragan, S., Henning, T., Krause, O., et al. 2012a, A&A, 547, A49 Google Scholar
Ragan, S. E., Heitsch, F., Bergin, E. A., & Wilner, D. 2012b, ApJ, 746, 174 Google Scholar
Tan, J. C., Beltrán, M. T., Caselli, P., et al. 2014, Protostars and Planets VI, 149Google Scholar
Zinnecker, H. & Yorke, H. W. 2007, ARA&A, 45, 481 Google Scholar