Hostname: page-component-cd9895bd7-dzt6s Total loading time: 0 Render date: 2024-12-25T05:24:20.900Z Has data issue: false hasContentIssue false

Ionized gas dynamics in the inner 2 pc of Sgr A West

Published online by Cambridge University Press:  22 May 2014

John H. Lacy
Affiliation:
Department of Astronomy, University of Texas, Austin, TX, USA email: [email protected]
Wesley T. Irons
Affiliation:
Dept. of Physics and Astronomy, Johns Hopkins University, Baltimore, MD, USA email: [email protected]
Matthew J. Richter
Affiliation:
Department of Physics, University of California, Davis, CA, 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 a data cube of the [NeII] (12.8 μm) emission from the inner 2 pc of Sgr A West with 1″ and 4 km s−1 resolution, and with substantially better SNR and velocity resolution than previous observations of the ionized gas. We compare the observations to two proposed models of the gas motions and distribution: flows along tidally stretched streamers, and more nearly circular motions with density wave compression. The density wave model provides a considerably better fit to the kinematics of the northern arm and western arc. Neither model fits the eastern arm and bar kinematics well.

To help understand the origin of the spiral pattern we calculated orbits in the potential of a black hole in a star cluster and find that the orbits naturally evolve to set up a one-armed spiral wave very similar to that observed, both spatially and kinematically. Magnetic or other perturbing forces may influence the formation of the spiral wave, but self gravity is not required. Because a density wave evolves on the orbit precession timescale, rather than the orbital timescale, a wave pattern should persist for several 105 yr. No net inward motion of the gas is required by the model. If there is inflow, it is much smaller than is suggested by the infalling streamer model.

Type
Contributed Papers
Copyright
Copyright © International Astronomical Union 2014 

References

Aitken, D. K., Smith, C., Moore, T. J., & Roche, P. F. 1998, MNRAS 299, 743CrossRefGoogle Scholar
Irons, W. T., Lacy, J. H., & Richter, M. J. 2012, ApJ 755, 90CrossRefGoogle Scholar
Irons, W. T., Lacy, J. H., & Richter, M. J. 2013, ApJ 771, 75CrossRefGoogle Scholar
Lacy, J. H., Townes, C. H., Geballe, T. R., & Hollenbach, D. J. 1980, ApJ 241, 132Google Scholar
Lacy, J. H., Achtermann, J. M., & Serabyn, E. 1991, ApJ 380, L71Google Scholar
Paumard, T., Maillard, J. P., & Morris, M. 2004, A&A 426, 81Google Scholar
Roberts, D. A. & Goss, W. M. 1993, ApJS 86, 133CrossRefGoogle Scholar
Serabyn, E. & Lacy, J. H. 1985, ApJ 293, 445Google Scholar
Wollman, E. R., Geballe, T. R., Lacy, J. H., Townes, C. H., & Rank, D. M. 1977, ApJ 218, 103Google Scholar
Zhao, J-H., Morris, M. R., Goss, W. M., & An, T. 2009, ApJ 699, 186CrossRefGoogle Scholar
Zhao, Jun J-H., Blundell, R., Moran, J. M., Downes, D., Schuster, K. F., & Marrone, D. P. 2010, ApJ 699, 186Google Scholar