Proceedings of the Workshop
"The Magellanic Clouds and Other Dwarf Galaxies"
of the Bonn/Bochum-Graduiertenkolleg

The Young Large-Scale Features in the Large Magellanic Cloud

Jochen M. Braun

Sternwarte der Universität Bonn, Auf dem Hügel 71, D-53121 Bonn,
Federal Republic of Germany, http://www.astro.uni-bonn.de/~webstw

Received 12th March 1998
Abstract. In this contribution I will present our project* of stellar population analyses and spatial information of the Magellanic Clouds (MCs).

The Large Magellanic Coud (LMC) is a suitable laboratory and testing ground for theoretical models of star formation. The distance of 50 kpc (huge compared to its depth < 300 pc) enables us to detect with today's techniques stellar light from the most massive and young stars, seen in OB associations and indirectly visible by the H II regions and Hα filaments, down to the low mass end of about 1/10 of a solar mass. Having a first glance at photographs of the MCs in the optical, the young population (< 25 Myr) with the associated emission nebulae (like the impressive 30 Dor region) and the large ring-like structures of about 800 pc diameters, the so called supergiant shells (SGSs), catch the eye. Despite being relatively well studied objects, these young features do not fit in a simple picture of stellar evolution history.

This article comprises the poster "Stellar content of supergiant shells in the LMC" dealing with an age analysis through a CCD photometry of the inner part of SGS LMC 4 and the talk "Large-scale star formation and the bow-shock trigger scenario", which introduces a new model for the origin of the stellar structures at the LMC outskirts.

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* The project is a collaborative effort with Klaas S. de Boer from the Sternwarte Bonn, Antonella Vallenari from the Astronomical Observatory in Padova, Ulrich Mebold from the Radioastronomical Institute in Bonn, Dominik J. Bomans at the Astronomy Department of the University of Illinois, and Jean-Marie Will, formerly at the Sternwarte Bonn, in the framework of the Bonn/Bochum - Graduiertenkolleg.

1. Introduction

On deep pictures of the Magellanic Clouds (MCs) taken in Hα light one can recognize huge bubbles with diameters of 600 - 1 400 pc, the so-called supergiant shells (SGSs or supershells). These bubbles, according to Goudis & Meaburn (1978), build a new group different from the smaller (< 260 pc) giant shells (GSs or superbubbles).

The 10 identified SGSs (see Meaburn 1981) plus an additional one detected in an H I survey (Kim et al. 1997) are listed in Table 1 and marked in Figs. 1 and 5. These structures need very effective creation mechanisms such as collisions of high velocity clouds (HVCs) with the disk of the galaxy or stochastic self-propagating star formation (SSPSF), both explaining the ring of H II regions and the 'hole' in the H I layer. According to the favorite SSPSF model, star formation will 'eat' its way from the initial point to all directions through the interstellar medium, creating a big cavity and a thick outer shell of neutral hydrogen ionized at the inner edge by the early-type stars (O-B2). Thus one should see a clear age gradient from the centre to the rim of about 15 Myr for structures extending 1.4 kpc like LMC 4.

[Click here to see Fig. 1!]
Table 1. The supergiant shells of the MCs
SGS Center coordinates (1950) Extension
[pc]
Rectascension Declination
LMC 1 5h 00m -65° 40' 700
LMC 2 5h 42m -69° 30' 900
LMC 3 5h 30m -69° 20' 1000
LMC 4 5h 31m -66° 50' 1400 × 1000
LMC 5 5h 22m -66° 10' 800
LMC 6 4h 58m -68° 45' 604
LMC 7 4h 54m -69° 35' 800
LMC 8 5h 02m -70° 30' 900
LMC 9 5h 25m -71° 05' 890
LMC ? 5h 12m -65° 20' 1400
SMC 1 1h 29m -73° 20' 600

This work (see Braun et al. 1997, hereafter Paper I) presents a photometric study of the stellar population inside the biggest SGS LMC 4. The found ages for this and other huge structures (see Fig. 5) hint at another plausible explanation: large-scale star formation triggered by the bow-shock (de Boer et al. 1998, hereafter Paper II).

2. Age Determination in LMC 4

Our data, containing 25 overlapping CCD fields (see Fig. 2), were taken in 1993 with the 0.91 m Dutch telescope in B, V passbands. The E-W strip covers the main part of the bean-shaped superassociation LH 77, which is indicated in Fig. 5. Photometry of 20 000 stars, using the Magellanic Catalogue of Stars (MACS, Tucholke et al. 1996) for absolute coordinates, was carried out with DAOPHOT II delivering colour-magnitude diagrams (CMDs, see Fig. 3). To these CMDs Geneva isochrones (Schaerer et al. 1993) were fitted by eye yielding ages and reddening values for all fields given in Table 2.

The ages we derived for the stars in the 'J'-shaped region inside LMC 4 lie in the interval from 9 Myr up to 16 Myr (∼13 Myr) and are the same as the ages determined for NGC 1948, NGC 2004, LH 72 north, LH 63, and LH 60 at the border of this SGS (see Sect. 5 in Paper I for details and references). The reddening is of the order of a 1/10 magnitude.

There exist some examples of younger star groups likely having been built in secondary star forming processes and one can also find age gradients on small scales (< 150 pc), but seeing coeval stars on scales larger than 1 kpc is striking.

[Click here to see Fig. 2!]
Table 2. Age (t), reddening (EB-V) and number of stars (N*, BV) of all fields (Paper I)
Region Field N*, BV t
[Myr]
EB-V
[mag]
e 24 313     :11    0.08
23 368 :11 0.08
22 604 :11 0.09
21 819 :11 0.10
20 1 084 :11 0.11
d 19 980 11 0.11
18 1 132 11 0.11
17 1 060 10 0.11
16 1 067 10 0.09
15 1 120 10 0.09
c 14 1 166 11 0.04
13 698 11 0.00
12 904 11 0.09
11 998 11 0.11
10 1 062 11 :0.11
b 9 1 286 14 :0.11
8 1 582 13 :0.11
7 1 746 10 :0.11
6 1 562 9 :0.11
5 1 625 9 :0.11
a 4 532 10 :0.11
3 462 13 0.08
2 813 13 0.11
1 678 11 0.11
0 819 16 0.11

[Click here to see Fig. 3!]

3. Luminosity Function and Mass Function in LMC 4

To get better number statistics we combined 5 CCD fields to one region (see Table 2). For each of them we constructed the luminosity function (with slope γ) yielding values in the expected range (γ ∈ [0.22;0.41]), and by using the best fitting Geneva isochrone of 10 Myr the mass function (with slope Γ ∈ [-1.3;-2.4]; Salpeter 1955: Γ = -1.35). The total luminosity and mass function of our region is plotted in Fig. 4. Since the slopes we find fall in the normal interval (see e.g. Will 1996), no severe superposition of stellar populations with different ages is present.

[Click here to see Fig. 4!]

4. History of LMC 4

Based on the results listed above we extrapolate that the 5-7·103 stars with masses M in [18.3;125] Msun released a minimum of 1054.5 erg by explosions of supernova of type II. Thus we can explain the structure of this SGS as we see it today by the sequel of supernovae going off everywhere during the last 10 Myr inside LMC 4 at a fair and still increasing rate dumping energy rather evenly in the space of the original huge birth cloud.

5. Bow-Shock Triggering Scenario

The lack of an age gradient, contradictory to the theory of SSPSF predicting about 15 Myr for LMC 4 with a diameter of  > 1 kpc, urges to look for a large-scale trigger.

For the Magellanic System we can expect an effect by the motion of the LMC through the halo of our Galaxy. The first hint is the steeper density gradient of H I at the leading eastern edge of the LMC and Magellanic Stream extending to the west as a tidal tail of the clouds (see left part of Fig. 5). But could this affect the superstructure in the north-east?

The superstructures in the LMC (see right part of Fig. 5) are located at the outskirts. Furthermore we know that the dark cloud (DC), 30 Dor and LMC 4 are located at the rear side of the LMC fitting to the direction of the LMC motion. Taking the rotation of the LMC into account, we would expect star formation triggered by the compression of the gas due to the bow-shock at the leading edge (with a total relative velocity ∼450 km s-1; see p. 125, de Boer 1998 and Paper II), which changed its position from the north to the east according to the clockwise rotation. If we look at the ages of superstructures and its traversed distance (see Fig. 6 and Table 3), we get a good correlation by the age determinations fitting to the rotation of the galaxy (Paper II).

[Click here to see Fig. 5!]
Table 3. Parameters for age and position of superstructures along the edge of the LMC (see Paper II for references)
Name Distance
[kpc]
Age
[Myr]
Dark cloud   (DC) 0 <0
N 159 0.5 <3
30 Dor 1.1 3-5
LMC 4   (Sh III) 3.0 9-16
NGC 1818 and field 6.0 30
Field near NGC 1783 6.7 20-50

[Click here to see Fig. 6!]

If star formation is triggered by the bow-shock at the leading edge (now at the SE), one can predict ages and compare them with derived ones. To further support this model, we got a dataset at the 1.54 m Danish telescope at La Silla in December 1996 [ESO proposal 58.D-0149] pointing at N 70, LMC 2, N 214 and N 171. As a first preliminary result I present the CMD of N 70 which yields an age of ∼8 Myr (see Fig. 7). This value is in accordance with the expected age, but as star formation is going on all over the region of the LMC the huge features are better hints for triggering than the smaller associations and shells.

[Click here to see Fig. 7!]

Additionally we got U, B, V photometry of the interior of SGS LMC 1 and LMC 7 at the 1.54 m Danish telescope at La Silla in January 1998 [ESO proposals 60.E-0234 and 60.D-0147] to get further constraints on the creation mechanisms for these prominent features of the youngest stellar generation and to enlighten the difference in the Hα appearance of the SGSs. Is this caused by an age effect or are the SGSs divided into two distinct groups (LMC 1-5 and LMC 6-9)?

6. Conclusions

The data presented above lead us to the following hypotheses:
It will be quite interesting to see if these provoking theses will prove valid in the next years.

References


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First version: 12thMarch,1998
Last update: 24thOctober,1998

Jochen M. Braun   &   Tom Richtler
 (E-Mail: jbraun|richtler@astro.uni-bonn.de)