scholarly journals The coalescence of invariant manifolds and the spiral structure of barred galaxies

2008 ◽  
Vol 387 (3) ◽  
pp. 1264-1280 ◽  
Author(s):  
P. Tsoutsis ◽  
C. Efthymiopoulos ◽  
N. Voglis
2020 ◽  
Vol 636 ◽  
pp. A44
Author(s):  
C. Efthymiopoulos ◽  
M. Harsoula ◽  
G. Contopoulos

In the manifold theory of spiral structure in barred galaxies, the usual assumption is that the spirals rotate with the same pattern speed as the bar. Here, we generalize the manifold theory under the assumption that the spirals rotate with a different pattern speed than the bar. More generally, we consider the case in which one or more modes, represented by the potentials V2, V3, etc., coexist in the galactic disk in addition to the bar’s mode Vbar, but the modes rotate with pattern speeds, Ω2, Ω3, etc., which are incommensurable between themselves and with Ωbar. Through a perturbative treatment (assuming that V2, V3, etc. are small with respect to Vbar), we then show that the unstable Lagrangian points L1 and L2 of the pure bar model (Vbar, Ωbar) are continued in the full model as periodic orbits, in the case of one extra pattern speed, or as epicyclic “Lissajous-like” unstable orbits, in the case of more than one extra pattern speeds. We use GL1 and GL2 to denote the continued orbits around the points L1 and L2. Furthermore, we show that the orbits GL1 and GL2 are simply unstable. As a result, these orbits admit invariant manifolds, which can be regarded as the generalization of the manifolds of the L1 and L2 points in the single pattern speed case. As an example, we computed the generalized orbits GL1, GL2, and their manifolds in a Milky-Way-like model in which bar and spiral pattern speeds were assumed to be different. We find that the manifolds produce a time-varying morphology consisting of segments of spirals or “pseudorings”. These structures are repeated after a period equal to half the relative period of the imposed spirals with respect to the bar. Along one period, the manifold-induced time-varying structures are found to continuously support at least some part of the imposed spirals, except at short intervals around specific times at which the relative phase of the imposed spirals with respect to the bar is equal to ±π/2. The connection of these effects to the phenomenon of recurrent spirals is discussed.


Author(s):  
C. Efthymiopoulos ◽  
P. Tsoutsis ◽  
C. Kalapotharakos ◽  
G. Contopoulos

2008 ◽  
Vol 495 (3) ◽  
pp. 743-758 ◽  
Author(s):  
P. Tsoutsis ◽  
C. Kalapotharakos ◽  
C. Efthymiopoulos ◽  
G. Contopoulos

1996 ◽  
Vol 157 ◽  
pp. 286-298
Author(s):  
Françoise Combes

AbstractThe dynamical mechanism to form rings at Lindblad resonances in a barred galaxy is now well-known: due to its dissipative character, the gas is forced in a spiral structure, and experiences torques from the bar potential. Angular momentum is transferred until gas accumulates in the resonant rings. Some problems remain however to account for all observations, such as the very different time-scales for nuclear, inner and outer ring formation, while the three are frequently observed in the same galaxy; the shapes, orientations and thickness of the rings, etc... The adequacy of the present gas dynamical modelizations is discussed.Lenses are secondary components of barred galaxies that could originate from bar evolution. No model until now has met the observational constraints, in particular the sharp edge of the lenses, their strong velocity anisotropy, and their small thickness. We propose here that lenses are the result of partial bar destruction, a necessary step in a feedback cycle of bar formation-destruction, a cycle driven by gas accretion.


Author(s):  
M. Romero-Gómez ◽  
E. Athanassoula ◽  
J. J. Masdemont ◽  
C. García-Gómez

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