Hostname: page-component-586b7cd67f-2brh9 Total loading time: 0 Render date: 2024-11-25T10:46:41.592Z Has data issue: false hasContentIssue false

The Role of the Radial Orbit Instability in Dark Matter Halo Formation and Structure

Published online by Cambridge University Press:  01 August 2006

J. M. Meyer
Affiliation:
Department of Astronomy, University of Washington, Seattle, WA 98195, USA
J. J. Dalcanton
Affiliation:
Department of Astronomy, University of Washington, Seattle, WA 98195, USA
T. R. Quinn
Affiliation:
Department of Astronomy, University of Washington, Seattle, WA 98195, USA
L. L. R. Williams
Affiliation:
Department of Astronomy, University of Minnesota, Minneapolis, MN, 55455, USA
E. I. Barnes
Affiliation:
Department of Physics, University of Wisconsin-LaCrosse, La Crosse, WI, 54601, USA
A. Babul
Affiliation:
Department of Physics & Astronomy, University of Victoria, Victoria, BC, V8P 1A1, Canada
C. G. Austin
Affiliation:
Department of Astronomy, University of Minnesota, Minneapolis, MN, 55455, USA
R. Maas
Affiliation:
Department of Astronomy, University of Washington, Seattle, WA 98195, USA
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.

For nearly a decade, N-body simulations have revealed a nearly universal dark matter density profile. This density profile appears to be robust to changes in the overall density of the universe and the underlying power spectrum. Despite its universality, however, the physical origin of this profile has not yet been well understood. Semi-analytic models have suggested that scale lengths in dark matter halos may be determined by the onset of the radial orbit instability. We have tested this theory using N-body simulations of collapsing dark matter halos. The resulting halo structures are prolate in shape, due to the mild aspect of the instability. We find that the radial orbit instability sets a scale length at which the velocity dispersion changes rapidly from isotropic to radially anisotropic. Preliminary analysis suggests that this scale length is proportional to the radius at which the density profile changes shape, as is the case in the semi-analytic models; however, the coefficient of proportionality is different by a factor of ~2. We conclude that the radial orbit instability may be a key physical mechanism responsible for the nearly universal profiles of simulated dark matter halos.

Type
Contributed Papers
Copyright
Copyright © International Astronomical Union 2007

References

Barnes, E.I., Williams, L.L.R., Babul, A., & Dalcanton, J.J. 2005, ApJ 634, 775.CrossRefGoogle Scholar
Navarro, J.F., Frenk, C.S., & White, S.D.M. 1996, ApJ 462, 563.CrossRefGoogle Scholar
Navarro, J.F., Hayashi, E., Power, C., Jenkins, A.R., Frenk, C.S., White, S.D.M., Springel, V., Stadel, J., & Quinn, T.R. 2004, ApJ 634, 775.Google Scholar
Stadel, J. 2001, PhD. Thesis.Google Scholar