Hostname: page-component-cd9895bd7-hc48f Total loading time: 0 Render date: 2024-12-25T05:58:07.048Z Has data issue: false hasContentIssue false

Shock structure and shock heating in the Galactic central molecular zone

Published online by Cambridge University Press:  22 May 2014

Jürgen Ott
Affiliation:
National Radio Astronomy Observatory, P. O. Box O, 1003 Lopezville Road, Socorro, NM 87801, USA; email: [email protected] Department of Physics, New Mexico Institute of Mining and Technology, Socorro, NM 87801, USA; email: [email protected]
Michael Burton
Affiliation:
School of Physics, University of New South Wales, Sydney NSW 2052, Australia; email: [email protected], [email protected]
Paul Jones
Affiliation:
School of Physics, University of New South Wales, Sydney NSW 2052, Australia; email: [email protected], [email protected]
David S. Meier
Affiliation:
National Radio Astronomy Observatory, P. O. Box O, 1003 Lopezville Road, Socorro, NM 87801, USA; email: [email protected] Department of Physics, New Mexico Institute of Mining and Technology, Socorro, NM 87801, USA; 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.

We present maps of a large number of dense molecular gas tracers across the central molecular zone of our Galaxy. The data were taken with the CSIRO/CASS Mopra telescope in Large Projects in the 1.3 cm, 7 mm, and 3 mm wavelength regimes. Here, we focus on the brightness of the shock tracers SiO and HNCO, molecules that are liberated from dust grains under strong (SiO) and weak (HNCO) shocks. The shocks may have occurred when the gas enters the bar regions and the shock differences could be due to differences in the moving cloud masses. Based on tracers of ionizing photons, it is unlikely that the morphological differences are due to selective photo-dissociation of the molecules. We also observe direct heating of molecular gas in strongly shocked zones, with high SiO/HNCO ratios, where temperatures are determined from the transitions of ammonia. Strong shocks appear to be the most efficient heating source of molecular gas, apart from high energy emission emitted by the central supermassive black hole Sgr A* and the processes within the extreme star formation region Sgr B2.

Type
Contributed Papers
Copyright
Copyright © International Astronomical Union 2014 

References

Jones, P. A., Burton, M. G., Cunningham, M. R., et al. 2012, MNRAS 419, 2961CrossRefGoogle Scholar
Martin-Pintado, J., de Vicente, P., Fuente, A., & Planesas, P. 1997, ApJ Lett. 482, L45Google Scholar
Meier, D. S. & Turner, J. L. 2005, ApJ 618, 259CrossRefGoogle Scholar
Molinari, S., Bally, J., Noriega-Crespo, A., et al. 2011, ApJ Lett. 735, L33CrossRefGoogle Scholar
Morris, M. & Serabyn, E. 1996, ARAA 34, 645Google Scholar
Oka, T., Hasegawa, T., Sato, F., Tsuboi, M., & Miyazaki, A. 1998, ApJS 118, 455CrossRefGoogle Scholar
Ott, J., Henkel, C., Burton, W. A., et al. 2008, Gas and Stars in Galaxies - A Multi-Wavelength 3D PerspectiveGoogle Scholar