ARGOS III: Stellar Populations in the Galactic Bulge of the Milky Way

TL;DR

This study analyzes the metallicity and stellar populations of the Galactic bulge using spectroscopy of 28,000 stars to understand its formation history, distinguishing between merger and disk instability origins.

Contribution

It provides the first large-scale spectroscopic survey of the Galactic bulge, revealing distinct stellar populations and their spatial and kinematic properties, supporting a formation via disk instabilities.

Findings

Stars with [Fe/H] > -0.5 are part of the boxy/peanut bulge.

Lower metallicity stars are associated with the thick disk and halo.

Two bulge populations identified: a metal-poor and a more metal-rich, kinematically colder component.

Abstract

We present the metallicity results from the ARGOS spectroscopic survey of the Galactic bulge. Our aim is to understand the formation of the Galactic bulge: did it form via mergers, as expected from Lambda CDM theory, or from disk instabilities, as suggested by its boxy/peanut shape, or both? We have obtained spectra for 28,000 stars at a spectral resolution of R = 11,000. From these spectra, we have determined stellar parameters and distances to an accuracy of < 1.5 kpc. The stars in the inner Galaxy span a large range in [Fe/H], -2.8 < [Fe/H] < +0.6. From the spatial distribution of the red clump stars as a function of [Fe/H] (Ness et al. 2012a), we propose that the stars with [Fe/H] > -0.5 are part of the boxy/peanut bar/bulge. We associate the lower metallicity stars ([Fe/H] < -0.5) with the thick disk, which may be puffed up in the inner region, and with the inner regions of the metal-weak thick disk and inner halo. For the bulge stars with [Fe/H] > -0.5, we find two discrete populations; (i) stars with [Fe/H] ~ -0.25 which provide a roughly constant fraction of the stars in the latitude interval b = -5 deg to -10 deg, and (ii) a kinematically colder, more metal-rich population with mean [Fe/H] ~ +0.15 which is more prominent closer to the plane. The changing ratio of these components with latitude appears as a vertical abundance gradient of the bulge. We attribute both of these bulge components to instability-driven bar/bulge formation from the thin disk. We do not exclude a weak underlying classical merger-generated bulge component, but see no obvious kinematic association of any of our bulge stars with such a classical bulge component. [abridged]