Gas-driven evolution of stellar orbits in barred galaxies

被引:118
作者
Berentzen, I
Heller, CH
Shlosman, I
Fricke, KJ
机构
[1] Univ Sternwarte, D-37083 Gottingen, Germany
[2] Univ Kentucky, Dept Phys & Astron, Lexington, KY 40506 USA
关键词
galaxies : active; galaxies : evolution; galaxies : kinematics and dynamics; galaxies : starburst; galaxies : structure;
D O I
10.1046/j.1365-8711.1998.01836.x
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We carry out a detailed orbit analysis of gravitational potentials selected at different times from an evolving self-consistent model galaxy consisting of a two-component disc (stars+gas) and a live halo. The results are compared with a pure stellar model, subject to nearly identical initial conditions, which are chosen so as to make the models develop a large-scale stellar bar. The bars are also subject to hose-pipe (buckling) instability which modifies the vertical structure of the disc. The diverging morphological evolution of both models is explained in terms of gas radial inflow, the resulting change in the gravitational potential at smaller radii, and the subsequent modification of the main families of orbits, both in and out of the disc plane. We find that dynamical instabilities become milder in the presence of the gas component, and that the stability of planar and 3D stellar orbits is strongly affected by the related changes in the potential - both are destabilized, with the gas accumulation at the centre. This is reflected in the overall lower amplitude of the bar mode and in the substantial weakening of the bar, which appears to be a gradual process. The vertical buckling of the bar is much less pronounced and the characteristic peanut shape of the galactic bulge almost disappears when there is a substantial gas inflow towards the centre. Milder instability results in a smaller bulge, the basic parameters of which are in agreement with observations. We also find that the overall evolution in the model with a gas component is accelerated because of the larger central mass concentration and the resulting decrease in the characteristic dynamical time.
引用
收藏
页码:49 / 63
页数:15
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