Can we really pick and choose? Benchmarking various selections of Gaia Enceladus/Sausage stars in observations with simulations

Author:

Carrillo Andreia12ORCID,Deason Alis J12ORCID,Fattahi Azadeh1ORCID,Callingham Thomas M3ORCID,Grand Robert J J456ORCID

Affiliation:

1. Institute for Computational Cosmology, Department of Physics, Durham University , Durham DH1 3LE , UK

2. Centre for Extragalactic Astronomy, Department of Physics, University of Durham , South Road, Durham DH1 3LE , UK

3. Kapteyn Astronomical Institute, University of Groningen , Landleven 12, NL-9747 AD Groningen , the Netherlands

4. Astrophysics Research Institute, Liverpool John Moores University , 146 Brownlow Hill, Liverpool L3 5RF , UK

5. Instituto de Astrofisica de Canarias , Calle Via Lactea s/n, E-38205 La Laguna, Tenerife , Spain

6. Departamento de Astrofisica, Universidad de La Laguna , Av. del Astrofisico Francisco Sanchez s/n, E-38206 La Laguna, Tenerife , Spain

Abstract

ABSTRACT Large spectroscopic surveys plus Gaia astrometry have shown us that the inner stellar halo of the Galaxy is dominated by the debris of Gaia Enceladus/Sausage (GES). With the richness of data at hand, there are a myriad of ways these accreted stars have been selected. We investigate these GES selections and their effects on the inferred progenitor properties using data constructed from APOGEE and Gaia. We explore selections made in eccentricity, energy-angular momentum (E-Lz), radial action-angular momentum (Jr-Lz), action diamond, and [Mg/Mn]-[Al/Fe] in the observations, selecting between 144 and 1279 GES stars with varying contamination from in-situ and other accreted stars. We also use the Auriga cosmological hydrodynamic simulations to benchmark the different GES dynamical selections. Applying the same observational GES cuts to nine Auriga galaxies with a GES, we find that the Jr-Lz method is best for sample purity and the eccentricity method for completeness. Given the average metallicity of GES (−1.28 < [Fe/H] < −1.18), we use the z = 0 mass–metallicity relationship to find an average $\rm M_{\star }$of ∼4 × 108 M⊙. We adopt a similar procedure and derive $\rm M_{\star }$ for the GES-like systems in Auriga and find that the eccentricity method overestimates the true $\rm M_{\star }$ by ∼2.6 × while E-Lz underestimates by ∼0.7 ×. Lastly, we estimate the total mass of GES to be $\rm 10^{10.5 - 11.1}~{\rm M}_{\odot }$ using the relationship between the metallicity gradient and the GES-to-in-situ energy ratio. In the end, we cannot just ‘pick and choose’ how we select GES stars, and instead should be motivated by the science question.

Funder

Science and Technology Facilities Council

STFC

Leverhulme Trust

MICINN

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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