Next Contents Previous

2. BIRTH OF TIDAL DWARF GALAXIES: MODELS, SIMULATIONS

Observations give some clues on the formation mechanism of tidal dwarfs. In the young TDGs observed so far, the atomic hydrogen makes the bulk of their mass. Therefore gas should play a key role. On the theoretical side, several scenarios have been proposed, supported by various types of numerical simulations:

  1. Local gravitational instabilities in the stellar component. Simulations of mergers which only include the stellar component are apparently able to produce along tidal tails gravitational bound stellar objects, some reaching the mass of dwarf galaxies [1]. However it has been claimed that they might in fact be artifacts of the N-body simulations [30].

  2. Local gravitational instabilities in the gaseous component. In simulations which include the gas component, real massive gas condensations may locally grow in the tails and form objects similar to TDGs [30].

  3. Ejection of Jeans-unstable gas clouds. Due to the increased velocity dispersion induced by galaxy-galaxy interactions, the Jeans mass of the individual cloud complexes increases in the outer disks of the parent galaxies. They are then pulled out by tidal forces, become unstable and collapse when reaching large galacto-centric distances [11].

  4. A top-down kinematical scenario. The global tidal field of galaxies with extended dark matter halos can efficiently carry away from their disk a large fraction of the gas, while maintaining its surface density to a high value [9]. In fact tidal forces contribute to stretch the gas only at low galacto-centric distances, i.e. at the base of the tail. As a result, gas accumulates near the tip of tidal tail, and then collapses and fragments, through a process apparently opposite to the bottom-up one favored with the Cold Dark Matter model for the building up of classical galaxies.

  5. The fully compressive mode of tidal forces. At locations where tidal forces are compressive rather than destructive, star / cluster formation may be triggered and/or already formed stellar objects, such as TDGs, may be protected from disruption [24].

  6. Merger between Super-Star-Clusters. SSCs with a range of masses may be formed in mergers. Some of them might merge to reach the mass of dwarf galaxies [12]. The TDGs born that way would then resemble the Ultra Compact Dwarf Galaxies (UCDs) identified in nearby groups and clusters of galaxies.

The variety of proposed scenarios tells how much having ad-hoc initial conditions and all necessary ingredients in the simulations is important: if the dark matter halo is truncated in the numerical simulations (to lower their computational cost), scenario (4) will not work; scenarios (2)-(5) require proper treatment of the gaseous component, including feedback. Scenario (6) needs high resolution, so as to resolve Super Star Clusters. Fig. 2 presents one of such simulations fulfilling most of these criteria. The numerical model used a total of 36 million particles, including 12 million "sticky" particles for the gas component, and minimal grid cell size of 32 pc [6]. The production of star clusters with masses down to 105 Modot was directly resolved in these simulations. The mass spectrum of objects produced during the merger seems to be bimodal. Two distinct families arise: (a) compact SSCs, with masses less than 108 Modot which seem pressure supported and may be the progenitors of globular clusters; (b) extended objects with masses above 108 Modot which are usually supported by rotation. The latter have the properties of observed Tidal Dwarf Galaxies. Thus TDGs are not simply the high mass end of SSCs, a conclusion that was also reached from the analysis of HST images [16]. Furthermore, analyzing snapshots of the simulation for a period of one Gyr, we found no evidence that the latter evolve into the former, via merging. The TDG progenitors are visible soon after the first encounter, in the outskirts of the colliding galaxies, at a time when the tidal tails have not yet completely unfolded. They quickly collect all their building material. After about 100 Myr, their mass is stabilized. Rotational support appears as well very early on. Only a few massive objects are formed later on within the tidal tails. Note however that star-formation and gas feedback are not properly handled with the sticky particles used in these simulations. Investigations may now be carried using fully hydrodynamical simulations [26].

Figure 2

Figure 2. Formation of tidal dwarf galaxies in high resolution numerical simulation of a major merger [6]. Two snapshots are shown, resp. after the first encounter and the merger (Belles et al., in prep).

Next Contents Previous