Globular cluster ejection, infall, and the host dark matter halo of the Pegasus dwarf galaxy

Author:

Leaman Ryan1,Ruiz-Lara Tomás23,Cole Andrew A4,Beasley Michael A23ORCID,Boecker Alina1,Fahrion Katja15,Bianchini Paolo67ORCID,Falcón-Barroso Jesus23,Webb Jeremy8,Sills Alison6ORCID,Mastrobuono-Battisti Alessandra1ORCID,Neumayer Nadine1,Sippel Anna C1

Affiliation:

1. Max-Planck Institut für Astronomie, Königstuhl 17, D-69117 Heidelberg, Germany

2. Instituto de Astrofísica de Canarias, Vía Láctea s/n, E-38205 La Laguna, Spain

3. Departamento de Astrofísica, Universidad de La Laguna, E-38206 La Laguna, Spain

4. School of Natural Sciences, University of Tasmania, Hobart, TAS 7001, Australia

5. European Southern Observatory, Karl-Schwarzschild-Str. 2, D-85741 Garching, Germany

6. Department of Physics and Astronomy, McMaster University, Hamilton, ON L8S 4M1, Canada

7. CNRS, Observatoire Astronomique de Strasbourg, Université de Strasbourg, UMR 7550, F-67000 Strasbourg, France

8. Department of Astronomy and Astrophysics, University of Toronto, 50 George Street, Toronto, ON M5S 3H4, Canada

Abstract

ABSTRACT Recent photometric observations revealed a massive, extended (MGC ≳ 105 M⊙; Rh ∼ 14 pc) globular cluster (GC) in the central region (D3D ≲ 100 pc) of the low-mass (M* ∼ 5 × 106 M⊙) dwarf irregular galaxy Pegasus. This massive GC offers a unique opportunity to study star cluster inspiral as a mechanism for building up nuclear star clusters, and the dark matter (DM) density profile of the host galaxy. Here, we present spectroscopic observations indicating that the GC has a systemic velocity of ΔV = 3 ± 8 km s−1 relative to the host galaxy, and an old, metal-poor stellar population. We run a suite of orbital evolution models for a variety of host potentials (cored to cusped) and find that the GC’s observed tidal radius (which is ∼3 times larger than the local Jacobi radius), relaxation time, and relative velocity are consistent with it surviving inspiral from a distance of Dgal ≳ 700 pc (up to the maximum tested value of Dgal = 2000 pc). In successful trials, the GC arrives to the galaxy centre only within the last ∼1.4 ± 1 Gyr. Orbits that arrive in the centre and survive are possible in DM haloes of nearly all shapes, however to satisfy the GC’s structural constraints a galaxy DM halo with mass MDM ≃ 6 ± 2 × 109 M⊙, concentration c ≃ 13.7 ± 0.6, and an inner slope to the DM density profile of −0.9 ≤ γ ≤ −0.5 is preferred. The gas densities necessary for its creation and survival suggest the GC could have formed initially near the dwarf’s centre, but then was quickly relocated to the outskirts where the weaker tidal field permitted an increased size and relaxation time – with the latter preserving the former during subsequent orbital decay.

Funder

Natural Sciences and Engineering Research Council of Canada

German Research Foundation

Deutscher Akademischer Austauschdienst

Ministry of Economy and Competitiveness

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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