IALP   13078
INSTITUTO DE ASTROFISICA LA PLATA
Unidad Ejecutora - UE
artículos
Título:
Orbital structure of self-consistent cuspy triaxial stellar systems
Autor/es:
J.C MUZZIO; H.D. NAVONE; A.F. ZORZI
Revista:
CELESTIAL MECHANICS & DYNAMICAL ASTRONOMY
Editorial:
SPRINGER
Referencias:
Lugar: Dordrecht (Holanda); Año: 2009 vol. 105 p. 379 - 395
ISSN:
0923-2958
Resumen:
We used a multipolar code to create, through dissipationless collapses of systems of 10**6 particles, two cuspy self--consistent triaxial stellar systems with γ about 1. One of the systems has an axial ratio similar to that of an E4 galaxy and it is only mildly triaxial (T=0.914), while the other one is strongly triaxial (T=0.593) and its axial ratio lies in between those of Hubble types E5 and E6. Both models rotate although their total angular momenta are zero, i.e., they exhibit figure rotation. The angular velocity is very small for the less triaxial model and, while it is larger for the more triaxial one, it is still comparable to that found by Muzzio (2006) to affect only slightly the dynamics of a similar model. Except for minor evolution, probably caused by unavoidable relaxation effects of the N--body code, the systems are highly stable. The potential of each system was subsequently approximated with interpolating formulae yielding smooth potentials, stationary in frames that rotate with the models. The Lyapunov exponents could then be computed for randomly selected samples of the bodies that make up the two systems, allowing the recognition of regular and of partially and fully chaotic orbits. Finally, the regular orbits were Fourier analyzed and classified using their locations on the frequency map. Most of the orbits are chaotic, and by a wide margin: less than 30% of the orbits are regular in our most triaxial model. Regular orbits are dominated by tubes, long axis ones in the less triaxial model and short axis tubes in the more triaxial one. Most of the boxes are resonant (i.e., they are boxlets), as could be expected from cuspy systems.