2020MNRAS.499.4793S


Query : 2020MNRAS.499.4793S

2020MNRAS.499.4793S - Mon. Not. R. Astron. Soc., 499, 4793-4813 (2020/December-3)

Models of distorted and evolving dark matter haloes.

SANDERS J.L., LILLEY E.J., VASILIEV E., EVANS N.W. and ERKAL D.

Abstract (from CDS):

We investigate the ability of basis function expansions to reproduce the evolution of a Milky Way-like dark matter halo, extracted from a cosmological zoom-in simulation. For each snapshot, the density of the halo is reduced to a basis function expansion, with interpolation used to recreate the evolution between snapshots. The angular variation of the halo density is described by spherical harmonics, and the radial variation either by biorthonormal basis functions adapted to handle truncated haloes or by splines. High fidelity orbit reconstructions are attainable using either method with similar computational expense. We quantify how the error in the reconstructed orbits varies with expansion order and snapshot spacing. Despite the many possible biorthonormal expansions, it is hard to beat a conventional Hernquist-Ostriker expansion with a moderate number of terms (>=15 radial and >=6 angular). As two applications of the developed machinery, we assess the impact of the time-dependence of the potential on (i) the orbits of Milky Way satellites and (ii) planes of satellites as observed in the Milky Way and other nearby galaxies. Time evolution over the last 5 Gyr introduces an uncertainty in the Milky Way satellites' orbital parameters of ∼15 per cent, comparable to that induced by the observational errors or the uncertainty in the present-day Milky Way potential. On average, planes of satellites grow at similar rates in evolving and time-independent potentials. There can be more, or less, growth in the plane's thickness, if the plane becomes less, or more, aligned with the major or minor axis of the evolving halo.

Abstract Copyright: © 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): methods: numerical - galaxies: haloes - galaxies: kinematics and dynamics - galaxies: structure

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 NAME Tuc IV G 00 02.9 -60 51           ~ 69 0
2 NAME Magellanic Stream HVC 00 32 -30.0           ~ 971 1
3 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 12643 1
4 NAME Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1358 4
5 NAME Sagittarius Stream St* 02 22 +00.0           ~ 874 0
6 NAME Fornax Dwarf Spheroidal G 02 39 59.3 -34 26 57   9.02 7.4     ~ 1741 1
7 NAME Reticulum III G 03 45.4 -60 27           ~ 55 0
8 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17428 0
9 NAME Col I G 05 31.4 -28 02           ~ 50 0
10 NAME Carina dSph G 06 41 36.7 -50 57 58   22.14 11.0 19.47   ~ 1124 0
11 NAME Antlia II Dwarf Galaxy G 09 35 32.8 -36 46 02           ~ 77 0
12 NAME Sextans C GlC 10 05 30.96 +00 04 15.4   15.5 13.9     ~ 327 1
13 NAME Sextans dSph G 10 13 02.9 -01 36 53   12 10.4     ~ 853 0
14 NAME Crater Cluster GlC 11 36 16.20 -10 52 38.8           ~ 91 1
15 NAME Crater II Dwarf Galaxy G 11 49 14 -18 24.8           ~ 137 0
16 NAME Centaurus A Sy2 13 25 27.61521044 -43 01 08.8050291   8.18 6.84 6.66   ~ 4483 3
17 NAME Bootes III G 13 57 07.4 +26 46 30     12.6     ~ 96 1
18 NAME Palomar 5 Stream St* 15 16 05 -00 06.7           ~ 103 0
19 NAME Dra dSph G 17 20 14.335 +57 55 16.39   12.40 10.6     ~ 1330 1
20 NAME SDG G 18 55 19.0 -30 32 43   4.5 3.6     ~ 2186 2
21 NAME Sagittarius II Gl? 19 52 40.5 -22 04 05           ~ 74 0
22 NAME Gru II G 22 04.1 -46 26           ~ 85 0
23 NAME Tuc V G 23 37.4 -63 16           ~ 60 0
24 NAME Phe II G 23 39 59.4 -54 24 22           ~ 86 0
25 NAME Orphan Stream St* ~ ~           ~ 253 0

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