Chaotic motion and spiral structure in self-consistent models of rotating galaxies

Details Chaotic motion and spiral structure in self-consistent models of rotating galaxies Chaotic motion and spiral structure in self-consistent models of rotating galaxies

2006-06-22

arxiv.org/abs/astro-ph/0606561v2

Mon.Not.Roy.Astron.Soc.372:901-922,2006

Astronomy and Astrophysics

Astrophysics

30 pages, 17 figures (low resolution). Revised version. Accepted for publication in MNRAS. For high resolution figures please

Scientific paper

10.1111/j.1365-2966.2006.10914.x

Dissipationless N-body models of rotating galaxies, iso-energetic to a non-rotating model, are examined as regards the mass in regular and in chaotic motion. The values of their spin parameters $\lambda$ are near the value $\lambda=0.22$ of our Galaxy. We obtain the distinction between the sets of particles moving in regular and in chaotic orbits and we show that the spatial distribution of these two sets of particles is much different. The rotating models are characterized by larger fractions of mass in chaotic motion ($\thickapprox 65%$) compared with the fraction of mass in chaotic motion in the non-rotating iso-energetic model ($\thickapprox 32%$). Furthermore, the Lyapunov numbers of the chaotic orbits in the rotating models become by about one order of magnitude larger than in the non-rotating model. Chaotic orbits are concentrated preferably in values of the Jacobi integral around the value of the effective potential at the corotation radius. We find that density waves form a central rotating bar embedded in a thin and a thick disc with exponential surface density profile. A surprising new result is that long living spiral arms are exited on the disc, composed almost completely by chaotic orbits. The bar excites an $m=2$ mode of spiral waves on the surface density of the disc, emanating from the corotation radius. These spiral waves are deformed, fade, or disappear temporarily, but they grow again re-forming a well developed spiral pattern. Spiral arms are discernible up to 20 or 30 rotations of the bar (lasting for about a Hubble time).

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