Gap lifetimes in thin stellar streams: an analytic estimate
Changes from v1.0 to v2.0. 108 words added, 87 removed. v1.0 is 100% original, v2.0 is 68% original.
Title
Gap lifetimes in thin stellar streams: an analytic estimate
Abstract
We derive an analytic estimate for the lifetime of gaps opened in thin stellar streams by dark matter subhalo impacts. Treating a gap as a density perturbation that is erased by differential orbital phase mixing, we obtain t_gap ≈ 2πR/σ_v, πR/σ_v, which depends only on the stream's velocity dispersion and galactocentric radius. For a GD-1-like stream at 14 kpc this gives gap lifetimes of 1.2 0.6 Gyr, in agreement consistent with the simulations of Carlberg N-body gap growth found by Erkal & Grillmair (2013b). We conclude Belokurov (2015). Gaps are erased after about 0.6 Gyr, so subhalo counts from older streams are incomplete by a factor that gaps older than 1 Gyr cannot be used to count subhalos. we tabulate.
Body
1. Introduction
Thin stellar streams such as GD-1 carry gaps where a dark matter subhalo passed close to the stream. Counting gaps is one of the few ways to count subhalos too small to hold stars of their own. A gap does not last forever. Stars inside the gap keep phase mixing along the orbit, and the density contrast fades until the gap can no longer be told apart from noise. This paper estimates how long a gap stays visible.
2. Method
We treat a gap as a small density perturbation on a stream of stars that share one orbit. Differential orbital phase mixing spreads the perturbation along the stream at a rate set by the spread in orbital frequency across the stream. For a stream at galactocentric radius R with velocity dispersion σ_v the perturbation is erased after t_gap ≈ 2πR/σ_v. πR/σ_v. The earlier version counted the phase-mixing time twice, once for each side of the gap, which doubled the lifetime. The estimate depends only on the velocity dispersion and the radius of the stream, and not on the mass of the subhalo that opened the gap.
3. Results
For a GD-1-like stream at 14 kpc with a velocity dispersion of 2 km/s we find gap lifetimes of 1.2 0.6 Gyr. This agrees is consistent with the simulations of Carlberg N-body gap growth found by Erkal & Grillmair (2013b), who report gaps that stay visible for about a gigayear. Belokurov (2015). Table 1 lists lifetimes for four streams at radii from 10 to 20 kpc. kpc, and Table 2 gives the fraction of impacts in the last 3 Gyr that still leave a visible gap.
4. Discussion
Gaps older than 1 Gyr cannot be used to count subhalos, because they have faded below the noise of current surveys. Subhalo are erased after about 0.6 Gyr, so subhalo counts from older streams therefore describe only are incomplete. The incompleteness factor in Table 2 corrects a count for the most recent gigayear of impacts. gaps that have already faded.
References ¶ Carlberg, R. G. and Grillmair, C. J. (2013b). Gaps in the GD-1 star stream. ApJ 768, 171.
Erkal, D. and Belokurov, V. (2015). Properties of dark subhaloes from gaps in tidal streams. MNRAS 454, 3542.
Other comparisons: v1.0 to v1.1 v1.0 to v3.0 v1.1 to v2.0 v1.1 to v3.0 v2.0 to v3.0