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. Author manuscript; available in PMC: 2023 Jun 14.
Published in final edited form as: Proc Int Astron Union. 2021 Aug;17(Suppl 373):11–14. doi: 10.1017/S1743921322005038

Hierarchical star formation in the Magellanic Clouds with the VMC survey

Amy E Miller 1,2,3,4, Maria-Rosa L Cioni 3, Richard de Grijs 1,2, Ning-Chen Sun 5; The VMC Team
PMCID: PMC7614645  EMSID: EMS158215  PMID: 37324748

Abstract

The VISTA Magellanic Clouds Survey (VMC) is a near-infrared survey of the Magellanic system. The VMC data has been exploited to detect and study statistically correlated young groups of stars — also known as “young stellar structures” — in the Large and Small Magellanic Clouds (LMC and SMC). We showcase the ~ 3000 recently detected young stellar structures in the LMC and their similarity to the fractal interstellar medium. We discuss how their properties indicate their formation mechanisms and that there are no preferred scales of star formation in the LMC.

Keywords: stars: formation, galaxies: Magellanic Clouds, stars: early-type, methods: statistical

1. Introduction

Within star-forming galaxies we generally observe a young stellar hierarchy composed of (listed in decreasing density) stars, clusters (~ 100 pc), associations (~ 101 — 102 pc), and complexes (~ 103 pc). This hierarchical distribution of young stars is found to disperse rapidly, on timescales of ≥ 100 Myr (Bastian et al. 2009; Sun et al. 2017b). There is evidence that most stars form in clusters, but there is also evidence that stars form in more isolated environments, leading to two distinct star formation channels being proposed: ‘clustered’ and ‘distributed’ star formation (Lada & Lada 2003). However, there is emerging evidence that star forming structures exist in a continuous range of sizes, masses, and densities (Bressert et al. 2010). Further analysis of the young stellar hierarchy is necessary to improve understanding of the star formation distribution and to search for characteristic sizes that may correspond to physical star formation mechanisms.

When discussing the star formation hierarchy, most studies focus on the densest regions, clusters, or the loosest regions, galaxies. These two disparate spatial scales must be unified; therefore, we focus on the intermediate scale, from 10–1000 pc. To study this intermediate scale, Sun et al. (2017a,b, 2018) employed a contour–based clustering analysis of young stars in two small regions covering the Large Magellanic Cloud (LMC) and the entire Small Magellanic Cloud (SMC). Their methodology was inspired by and incorporated work done by Gouliermis et al. (2010, 2015, 2017). We applied their methodology to the entire LMC in Miller et al. (2022). Our goals were to check for preferred scales of star formation, probe the dominant physical properties behind star formation, and to compare to the interstellar medium. In the following sections, we describe the data used, the detection methodology, results, and the implications of our work.

2. VMC data and young stellar structure identification

The Visible and Infrared Survey Telescope for Astronomy (VISTA) Magellanic Clouds Survey (VMC; Cioni et al. 2011), is a deep near-infrared YJKs survey of the Magellanic system with spatial resolution of ≤1 arcsec. The VMC covers ~ 20 square degrees on the LMC. We use point spread function photometry catalogues and deredden the magnitudes based on the extinction map provided by Skowron et al. (2021). We construct (J — Ks) versus Ks colourmagnitude diagrams and use them to select ~ 400,000 young upper main-sequence stars (see Figure 2 of Miller et al. 2022). After binning the stars, we apply kernel density estimation (KDE) and make a surface density map with a resolution of 10 pc (see left panel of Figure 3 from Miller et al. 2022). From this map, we identify structures at 1 to 15σ above the median background density. After applying selection criteria that each structure on the 1 — 2σ levels have at least one structure at a higher significance level and that each structure have at least 5 stars, we identify about 3000 young stellar structures (see Figure 1).

Figure 2.

Figure 2

(Left) The size distribution of the young stellar structures. In red, the power-law we fit between 10–700 pc. (Right) The surface density distribution of the structures. In red, the lognormal distribution we fit. After Miller et al. (2022).

Figure 1. The identified young stellar structures coloured by 1σ to 15σ. After Miller et al. (2022).

Figure 1

3. Results and comparison to gas structures

The main result from our work that we want to emphasize is the size (radius) distribution of the young stellar structures (see left panel of Figure 3). For such a size distribution, it is important to assess if the distribution is lognormal or a power-law. In our size distribution, there is clearly an excess of large structures on the right-hand side. We fit a power-law between the dashed lines at 10 pc and 700 pc. Mathematically, this power–law corresponds to the 2D fractal dimension (D2). This dimension encodes information about the spatial distribution of the young stellar structures. The one we derive, ~1.6, suggests our structures have a fractal morphology and that there is no preferred scale from 10–700 pc.

The peak of the size distribution is ~13 pc. The peak of a size distribution could be representative of a characteristic size of star formation. However, our structures are incomplete at R < 10 pc due to the resolution of our KDE map and due to our two selection criteria.

Therefore, it seems the peak is related to the detection limit of our study and is not evidence of a characteristic scale of star formation.

The mass–size relation and the perimeter–area relation follow a power–law (see Figures 7 and 8 in Miller et al. 2022). The surface density distribution follows a lognormal shape (see right panel of Figure 3). We summarize LMC results from Miller et al. (2022) along with results from Sun et al. (2018) in the SMC and compare them to results obtained in studies of gas structures in Table 1. Due to the striking similarities, the young stellar structures in the LMC and SMC might inherit the hierarchical, fractal properties from the interstellar medium from which they form. A further important highlight from this comparison is that the density distribution of the young stellar structures follows the same lognormal shape as probability density functions that are characteristic of supersonic, non–gravitating turbulent gas (Vazquez-Semadeni 1994; Padoan et al. 1997; Federrath et al. 2010).

Table 1.

Comparison with results from young stellar structures in the LMC (Miller et al. 2022) and SMC (Sun et al. 2018) with gas structures in the interstellar medium (references therein).

property young stellar structures gas structures
morphology irregular irregular[1],[2]
structure hierarchical hierarchical[1],[2]
size distribution power–law power–law[1]
mass–size relation power–law power–law[3]
density distribution lognormal lognormal [4]
perimeter-area relation power–law power–law[5]
2D fractal dimension D2 ≈ 1.6 D2 ≈ 1.7 [2]

4. Conclusion

In Miller et al. (2022), we identified ~ 3000 young stellar structures at 15 significance levels in the LMC using the near–infrared VMC survey. In this article we summarize our findings, and touch on those found in the SMC in Sun et al. (2018). We show the young stellar structures have:

  • Irregular morphology and hierarchical organization

  • Power–law mass–size relation, size distribution, and perimeter–area relation

  • Lognormal surface density distribution

  • Strong similarities with results in the interstellar medium and simulations of supersonic turbulence

Our findings imply that star formation creates a continuum of star–forming structures in the LMC from 10 pc to 700 pc and is scale–free. The findings are consistent with the hypothesis of turbulence–driven hierarchical star formation.

Acknowledgements

The author is supported by the International Cotutelle Macquarie University Research Excellence Scholarship. Under the European Union’s Horizon 2020 research and innovation programme, the European Research Council (ERC) has provided funding for this project (grant agreement no. 682115). The Australian Research Council’s Centre of Excellence for All Sky Astrophysics in Three Dimensions (ASTRO 3D), under the auspices of project CE170100013, also contributed to the funding of this study. We appreciate the support of the Science and Technology Facilities Council (STFC) in the UK, which enabled the Cambridge Astronomy Survey Unit (CASU) and the Wide Field Astronomy Unit (WFAU) in Edinburgh to provide the necessary data products. This investigation was conducted based on observations collected with VISTA at the ESO/La Silla Paranal Observatory with programme ID 179.B-2003.

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