C.D.S. - SIMBAD4 rel 1.7 - 2020.08.14CEST18:20:07

2014A&A...561A.141C - Astronomy and Astrophysics, volume 561A, 141-141 (2014/1-1)

Conditions of consistency for multicomponent axisymmetric stellar systems . Is an axisymmetric model suitable yet?


Abstract (from CDS):

Solving the Boltzmann collisionless equation under the axisymmetric hypothesis introduces serious limitations on describing the kinematics of a single stellar system according to the local Galactic observables. Instead of relaxing the hypothesis of axisymmetry, one alternative is to assume a mixture model. For a finite mixture of ellipsoidal velocity distributions, the coexistence of several stellar populations sharing a common potential introduces a set of conditions of consistency that may also constrain the population kinematics. For only a few potentials, the populations may have independent mean velocities and unconstrained velocity ellipsoids. In this paper, we determine which axisymmetric potentials are connected with a more flexible superposition of the stellar populations. The conditions of consistency are checked against recent results derived from kinematic surveys of the solar neighbourhood that include RAdial Velocity Experiment (RAVE) data. Several key observables are used to determine whether the axisymmetric mixture model is able to account for the main features of the local velocity distribution, such as the vertex deviation associated with the second central moment µ{piomega}θ, the population radial mean velocities, the radial gradient of the moment µ{piomega}z, the tilt of the velocity ellipsoids, and the existence of stars with no net rotation. In addition, the mixture moments for an arbitrary number of populations are derived in terms of the one-to-one mean velocity differences in order to study whether a more populated mixture could add any new features to the velocity distribution that remain unnoticed in a two-component mixture. According to this analysis, the quasi-stationary potential is the only potential allowing arbitrary directions of the population mean velocities. Then, the apparent vertex deviation of the total velocity distribution is due to the difference of the mean velocities of the populations whose velocity ellipsoids have no vertex deviation. For a non-separable potential, the population velocity ellipsoids have the same orientation and point towards the Galactic centre. For a potential separable in addition in cylindrical coordinates, the population velocity ellipsoids may have arbitrary tilt.

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Journal keyword(s): galaxies: kinematics and dynamics - solar neighborhood - galaxies: statistics

Simbad objects: 7

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Number of rows : 7

N Identifier Otype ICRS (J2000)
ICRS (J2000)
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2020
1 Cl Melotte 22 OpC 03 47 00 +24 07.0           ~ 2993 0
2 Cl Melotte 25 OpC 04 26 54.00 +15 52 00.0           ~ 2665 0
3 NAME Gal Anticenter reg 05 46 +28.9           ~ 726 0
4 * alf CMa SB* 06 45 08.91728 -16 42 58.0171 -1.51 -1.46 -1.46 -1.46 -1.43 A1V+DA 1399 0
5 NAME UMa Region reg 11 00 +50.0           ~ 316 0
6 NAME NGP reg 12 51 26.275 +27 07 41.70           ~ 1023 0
7 NAME Gal Center reg 17 45 40.04 -29 00 28.1           ~ 11620 0

    Equat.    Gal    SGal    Ecl

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