Abstract

ABSTRACT We present a Bayesian method to identify multiple (chemodynamic) stellar populations in dwarf spheroidal galaxies (dSphs) using velocity, metallicity, and positional stellar data without the assumption of spherical symmetry. We apply this method to a new Keck/Deep Imaging Multi-Object Spectrograph (DEIMOS) spectroscopic survey of the Ursa Minor (UMi) dSph. We identify 892 likely members, making this the largest UMi sample with line-of-sight velocity and metallicity measurements. Our Bayesian method detects two distinct chemodynamic populations with high significance (in logarithmic Bayes factor, ln B ∼ 33). The metal-rich ([Fe/H] = −2.05 ± 0.03) population is kinematically colder (radial velocity dispersion of $\sigma _v=4.9_{-1.0}^{+0.8} \, \mathrm{km} \, \mathrm{s}^{-1}$) and more centrally concentrated than the metal-poor ($[{\rm Fe/H}]=-2.29_{-0.06}^{+0.05}$) and kinematically hotter population ($\sigma _v =11.5_{-0.8}^{+0.9}\, \mathrm{km} \, \mathrm{s}^{-1}$). Furthermore, we apply the same analysis to an independent Multiple Mirror Telescope (MMT)/Hectochelle data set and confirm the existence of two chemodynamic populations in UMi. In both data sets, the metal-rich population is significantly flattened (ϵ = 0.75 ± 0.03) and the metal-poor population is closer to spherical ($\epsilon =0.33_{-0.09}^{+0.12}$). Despite the presence of two populations, we are able to robustly estimate the slope of the dynamical mass profile. We found hints for prolate rotation of order ${\sim}2 \, \mathrm{km} \, \mathrm{s}^{-1}$ in the MMT data set, but further observations are required to verify this. The flattened metal-rich population invalidates assumptions built into simple dynamical mass estimators, so we computed new astrophysical dark matter annihilation (J) and decay profiles based on the rounder, hotter metal-poor population and inferred $\log _{10}{(J(0{^{\circ}_{.}}5)/{\rm GeV^{2} \, cm^{-5}})}\approx 19.1$ for the Keck data set. Our results paint a more complex picture of the evolution of UMi than previously discussed.

Highlights

  • The distribution of dark matter within galaxies is a key test for the CDM cosmological model

  • We have presented line-of-sight velocities and stellar metallicities from the largest spectroscopic data set of the classical dwarf spheroidal galaxies (dSphs) Ursa Minor (UMi)

  • Through a dSph and MW foreground mixture model, we utilized a combination of velocity, metallicity, position, and proper motion to identify 892 UMi members, doubling the number of known spectroscopic members

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Summary

INTRODUCTION

The distribution of dark matter within galaxies is a key test for the CDM (cosmological constant + cold dark matter) cosmological model. The Milky Way (MW) dwarf spheroidal galaxies (dSphs) have low stellar masses and are highly dark matter-dominated systems (McConnachie 2012; Simon 2019) They are excellent laboratories to distinguish between these solutions. The dynamics of multiple stellar populations has been utilized in three dSphs: Fornax (Walker & Penarrubia 2011; Amorisco, Agnello & Evans 2013), Sculptor (Battaglia et al 2008; Walker & Penarrubia 2011; Agnello & Evans 2012; Amorisco & Evans 2012b; Zhu et al 2016; Strigari, Frenk & White 2017), and Carina (Hayashi et al 2018) to infer the mass slope of the dark matter halo.

Observations and target selection
Reductions and measurements
Validation
Final catalogue selection
METHODOLOGY
Selection function
Likelihoods
Ursa Minor properties
Detection of two chemodynamical stellar populations
Search for rotation
Exploring additional populations
SIMPLE ESTIMATORS OF MASS SLOPE
CHEMODYNAMIC POPULATIONS THROUGHOUT THE LOCAL GROUP
DARK MATTER ANNIHILATION AND D E C AY R AT ESOFURSAMINOR
CONCLUSION
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