4.7 Article

The effects of ΛCDM dark matter substructure on the orbital evolution of star clusters

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 503, Issue 2, Pages 1932-1939

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stab461

Keywords

globular clusters: general; Galaxy: kinematics and dynamics; galaxies: kinematics and dynamics; galaxies: star clusters: general; dark matter

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This study investigates how perturbations from a distribution of Lambda CDM dark matter subhalos affect the orbits of star clusters. The findings show that subhalos with masses less than 10^8 solar masses have negligible effects on test particle orbits, while perturbations lead to orbital deviations only in environments with substructure fractions greater than or equal to 1%. Additionally, perturbations from denser subhalos produce larger orbital deviations, and subhalo perturbations that are strong relative to the background tidal field lead to larger orbital deviations.
We present a comprehensive study on how perturbations due to a distribution of Lambda cold dark matter (Lambda CDM) dark matter subhalos can lead to star clusters deviating from their orbits. Through a large suite of massless test particle simulations, we find that (i) subhalos with masses less than 10(8) M-circle dot negligibly affect test particle orbits, (ii) perturbations lead to orbital deviations only in environments with substructure fractions f(sub) >= 1 per cent, (iii) perturbations from denser subhalos produce larger orbital deviations, and (iv) subhalo perturbations that are strong relative to the background tidal field lead to larger orbital deviations. To predict how the variation in test particle orbital energy sigma(e)(t) increases with time, we test the applicability of theory derived from single-mass subhalo populations to populations where subhalos have a mass spectrum. We find sigma(e)(t) can be predicted for test particle evolution within a mass spectrum of subhalos by assuming subhalos all have masses equal to the mean subhalo mass and by using the local mean subhalo separation to estimate the change in test particle velocities due to subhalo interactions. Furthermore, the orbital distance variation at an orbital distance r can be calculated via sigma(r) = 2.98 x 10(-5) +/- 8 x 10(-8)(kpc(-1)km(-2)s(2)) x r x sigma(e) with a dispersion about the line of best-fitting equalling 0.08 kpc. Finally, we conclude that clusters that orbit within 100 kpc of Milky Way-like galaxies experience a change no greater than in their dissolution times.

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