8 research outputs found

    The Nucleus of the Sagittarius Dwarf Spheroidal Galaxy: M54

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    Nuclear star clusters are the densest stellar systems in the universe, hosted by galaxies across the entire Hubble sequence, including a high fraction of dwarf galaxies. The most massive, chemically complex globular clusters in the Milky Way exhibit similar characteristics as nuclear star clusters in dwarf galaxies. This raised the idea that these globular clusters are actually former nuclei of galaxies accreted by the Milky Way. In this context, M54 – the nuclear star cluster of the Sagittarius dwarf spheroidal galaxy (Sgr dSph) – offers a unique opportunity to understand this presumed direct connection between globular clusters and nuclear star clusters, and low-mass galaxy nucleation. The Sgr dSph is currently being disrupted by the tidal field of the Milky Way, leaving a long stellar stream as evidence of its advanced degree of disruption. M54 still lies at the center of its host, becoming a potential stripped nucleus, and presenting an outstanding example of this class of objects. From its discovery – long before the detection of the Sgr dSph – M54 was classified as a globular cluster, the second most massive in the Milky Way after ω Cen. M54 shows a high spread in iron abundance of its member stars, pointing towards an extended and complex star formation history. This Thesis presents a large Multi-Unit Spectroscopic Explorer (MUSE) data set covering a region of ∼2.5 times the effective radius of M54. The single spectra of more than 6 500 member stars extracted from the exceptional data set led to the recovery of the star formation history of this nuclear star cluster through age and metallicity information. This allowed disentangling the presence of – at least – three stellar subpopulations, whose kinematics show clear differences. The chemo-dynamical characterization of these subpopulations suggests that they originated in different star formation events. This work shows the complexity of M54 which appears to be a nuclear star cluster in a highly disturbed environment rather than a simple globular cluster. The evidence suggests that M54 is the result of the two proposed mechanisms for the formation of nuclear stars clusters, that happen at different stages of M54’s evolution: (i) at least two globular clusters are driven to the center of the host and merge to form a single high-mass cluster with a large age and metallicity spread, followed by (ii) in-situ star formation from enriched gas in the nucleus. The unprecedented details of this study help to understand low-mass galaxy nuclei, for which less information is available in contrast to the higher mass regime

    Light element variations within the different age-metallicity populations in the nucleus of the Sagittarius dwarf

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    The cluster M54 lies at the centre of the Sagittarius dwarf spheroidal galaxy, and therefore may be the closest example of a nuclear star cluster. Either in-situ star formation, inspiralling globular clusters, or a combination have been invoked to explain the wide variety of stellar sub-populations in nuclear star clusters. Globular clusters are known to exhibit light element variations, which can be identified using the photometric construct called a chromosome map. In this letter, we create chromosome maps for three distinct age-metallicity sub-populations in the vicinity of M54. We find that the old, metal-poor population shows the signature of light element variations, while the young and intermediate-age metal rich populations do not. We conclude that the nucleus of Sagittarius formed through a combination of in-situ star formation and globular cluster accretion. This letter demonstrates that properly constructed chromosome maps of iron-complex globular clusters can provide insight into the formation locations of the different stellar populations.Comment: Accepted by MNRAS Letter

    Constraining nuclear star cluster formation using MUSE-AO observations of the early-type galaxy FCC 47

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    Context. Nuclear star clusters (NSCs) are found in at least 70% of all galaxies, but their formation path is still unclear. In the most common scenarios, NSCs form in-situ from the galaxy's central gas reservoir, through the merging of globular clusters (GCs), or through a combination of both. Aims: As the scenarios pose different expectations for angular momentum and stellar population properties of the NSC in comparison to the host galaxy and the GC system, it is necessary to characterise the stellar light, NSC, and GCs simultaneously. The large NSC (r_eff = 66 pc) and rich GC system of the early-type Fornax cluster galaxy FCC 47 (NGC 1336) render this galaxy an ideal laboratory to constrain NSC formation. Methods: Using Multi Unit Spectroscopic Explorer science verification data assisted by adaptive optics, we obtained maps for the stellar kinematics and stellar-population properties of FCC 47. We extracted the spectra of the central NSC and determined line-of-sight velocities of 24 GCs and metallicities of five. Results: The galaxy shows the following kinematically decoupled components (KDCs): a disk and a NSC. Our orbit-based dynamical Schwarzschild model revealed that the NSC is a distinct kinematic feature and it constitutes the peak of metallicity and old ages in FCC 47. The main body consists of two counter-rotating populations and is dominated by a more metal-poor population. The GC system is bimodal with a dominant metal-poor population and the total GC system mass is \u30317% of the NSC mass (\u3037 7 10^8 M_sun). Conclusions: The rotation, high metallicity, and high mass of the NSC cannot be explained by GC-inspiral alone. It most likely requires additional, quickly quenched, in-situ formation. The presence of two KDCs likely are evidence of a major merger that has significantly altered the structure of FCC 47, indicating the important role of galaxy mergers in forming the complex kinematics in the galaxy-NSC system

    Uncertainty-aware blob detection with an application to integrated-light stellar population recoveries

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    Context. Blob detection is a common problem in astronomy. One example is in stellar population modelling, where the distribution of stellar ages and metallicities in a galaxy is inferred from observations. In this context, blobs may correspond to stars born in situ versus those accreted from satellites, and the task of blob detection is to disentangle these components. A difficulty arises when the distributions come with significant uncertainties, as is the case for stellar population recoveries inferred from modelling spectra of unresolved stellar systems. There is currently no satisfactory method for blob detection with uncertainties. Aims. We introduce a method for uncertainty-aware blob detection developed in the context of stellar population modelling of integrated-light spectra of stellar systems. Methods. We developed a theory and computational tools for an uncertainty-aware version of the classic Laplacian-of-Gaussians method for blob detection, which we call ULoG. This identifies significant blobs considering a variety of scales. As a prerequisite to apply ULoG to stellar population modelling, we introduced a method for efficient computation of uncertainties for spectral modelling. This method is based on the truncated Singular Value Decomposition and Markov chain Monte Carlo sampling (SVD-MCMC). Results. We applied the methods to data of the star cluster M 54. We show that the SVD-MCMC inferences match those from standard MCMC, but they are a factor 5–10 faster to compute. We apply ULoG to the inferred M 54 age/metallicity distributions, identifying between two or three significant, distinct populations amongst its stars

    Hubble Space Telescope Proper Motion (HSTPROMO) Catalogs of Galactic Globular Clusters. VII. Energy Equipartition

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    We examine the degree of energy equipartition in 9 Galactic globular clusters using proper motions measured with the Hubble Space Telescope. For most clusters in the sample, this is the first energy equipartition study ever performed. This study is also the largest of its kind, albeit with only 9 clusters. We begin by rigorously cleaning the catalogues to remove poor-quality measurements and to ensure high signal-to-noise for the study. Using the cleaned catalogues, we investigate how velocity dispersion σ\sigma changes with stellar mass mm. We fit two functional forms: the first, a classic power-law of the form σmη\sigma \propto m^{-\eta} where η\eta is the degree of energy equipartition, and the second from Bianchini et al. (2016) parameterised by an equipartition mass meqm_{eq} where η\eta changes with stellar mass. We find that both functions fit well but cannot distinguish with statistical significance which function provides the best fit. All clusters exhibit varying degrees of partial equipartition; no cluster is at or near full equipartition. We search for correlations of η\eta and meqm_{eq} with various cluster properties. The most significant correlation is observed with the number of core or median relaxation times (NcoreN_{core} or NhalfN_{half}) the cluster has experienced. Finally, we determine the radial equipartition profile for each cluster, that is, how the degree of equipartition changes with projected distance from the cluster centre. We do not detect statistically significant trends in the degree of equipartition with radius. Overall, our observational findings are in broad agreement with theoretical predictions from N-body models published in recent years.Comment: 26 pages, 16 figures, 2 tables, accepted for publication in Ap

    A Deep View into the Nucleus of the Sagittarius Dwarf Spheroidal Galaxy with MUSE. III. Discrete Multicomponent Population-dynamical Models Based on the Jeans Equations

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    International audienceWe present comprehensive multicomponent dynamical models of M54 (NGC 6715), the nuclear star cluster of the Sagittarius (Sgr) dwarf galaxy, which is undergoing a tidal disruption in the Milky Way halo. Previous papers in this series used a large MUSE mosaic data set to identify multiple stellar populations in the system and study their kinematic differences. Here, we use Jeans-based dynamical models that fit the population properties (mean age and metallicity), spatial distributions, and kinematics simultaneously. They provide a solid physical explanation for our previous findings. Population-dynamical models deliver a comprehensive view of the whole system, and allow us to disentangle the different stellar populations. We explore their dynamical interplay and confirm our previous findings about the build-up of Sgr's nuclear cluster via contributions from globular cluster stars, Sgr inner field stars, and in situ star formation. We explore various parameterizations of the gravitational potential and show the importance of a radially varying mass-to-light ratio for the proper treatment of the mass profile. We find a total dynamical mass within M54's tidal radius (~75 pc) of 1.60 ± 0.07 × 106 M ⊙ in excellent agreement with N-body simulations. Metal-poor globular cluster stars contribute about 65% of the total mass or 1.04 ± 0.05 × 106 M ⊙. Metal-rich stars can be further divided into young and intermediate-age populations, which contribute 0.32 ± 0.02 × 106 M ⊙ (20%) and 0.24 ± 0.02 × 106 M ⊙ (15%), respectively. Our population-dynamical models successfully distinguish the different stellar populations in Sgr's nucleus because of their different spatial distributions, ages, metallicities, and kinematic features
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