A&A 451, 431-434 (2006)
DOI: 10.1051/0004-6361:20040330
E. Livanou1 - M. Kontizas1 - I. Gonidakis1 - E. Kontizas2 - F. Maragoudaki1 - S. Oliver3 - A. Efstathiou4 - U. Klein5
1 - Department of Astrophysics Astronomy & Mechanics, Faculty
of Physics, University of Athens, 15783 Athens, Greece
2 - Institute for Astronomy and Astrophysics, National
Observatory of Athens, PO Box 20048, 11810 Athens, Greece
3 - Astronomy Centre, Department of Physics & Astronomy, University of
Sussex, Brighton, BN1 9QJ, UK
4 - Department of Computer Science and Engineering, Cyprus College, 6
Diogenes Str, 1516 Nicosia, Cyprus
5 - Radioastronomisches Institut der Universitat, Bonn, Auf dem Hugel
71, 53121 Bonn, Germany
Received 25 February 2004 / accepted 30 November 2005
Abstract
Aims. Filamentary structures of early type stars are found to be a common feature of the Magellanic Clouds formed at an age of about 0.9-2
.
As we go to younger ages these large structures appear fragmented and sooner or later form young clusters and associations. In the optical domain we have detected 56 such large structures of young objects, known as stellar complexes in the LMC for which we give coordinates and dimensions. We also investigate star formation activity and evolution of these stellar complexes and define the term "starburst region''.
Methods. IR properties of these regions have been investigated using IRAS data. A colour-magnitude diagram (CMD) and a two-colour diagram from IRAS data of these regions ware compared with observations of starburst galaxies and cross-matching with HII regions and SNRs was made. Radio emission maps at 8.6-GHz and the CO (
)
line were also cross correlated with the map of the stellar complexes.
Results. It has been found that nearly 1/3 of the stellar complexes are extremely active resembling the IR behaviour of starburst galaxies and HII regions. These stellar complexes illustrating such properties are called here "starburst regions''. They host an increased number of HII regions and SNRs. The main starburst tracers are their IR luminosity (F60 well above 5.4 Jy) and the 8.6-GHz radio emission. Finally the evolution of all stellar complexes is discussed based on the CO emission.
Key words: Magellanic Clouds - galaxies: starburst - stars: formation
Due to its proximity to our Galaxy and the SMC, the LMC offers two important
advantages: i) the possibility to study its stellar content down to low
stellar masses and ii) the possibility to follow the consequences of the close
interaction, about 2-4
ago (Gardiner & Noguchi
1996; Kunkel et al. 2000), with the SMC. Stellar complexes
are defined as large structures (clump like) in galaxies dominated by recently
formed stellar component mixed with very young clusters, stellar associations
and gas (Martin et al. 1976; van den Bergh 1981;
Elmegreen & Elmegreen 1983, 1987;
Feitzinger & Braunsfurth 1984; Ivanov 1987; Larson et al. 1988;
Efremov 1989, 1995; Larson et al. 1992; Efremov & Chernin
1994; Elmegreen et al. 1994; Kontizas et al.
1994; Battinelli et al. 1996; Elmegreen & Efremov 1996; Kontizas et al. 1996). Sofar they have been detected as regions with young
stellar component and enhanced stellar number density, compared to the
surrounding region. In the LMC stellar complexes have been detected using UK Schmidt plates (Maragoudaki et al. 1998). In the optical domain we have detected 56 large structures of young objects. These stellar complexes are associated
with the already known nine Shapley constellations (Shapley 1956),
which are referred to as large stellar structures of early type supergiants.
Helou (1986) found that the IRAS
versus
colour-colour diagram of "normal galaxies'' shows a distribution that extends continuously from the cool (
20 K) relatively constant "cirrus'' emission from the neutral medium to the warmer (
40-50 K) emission from the active, starburst end.
IRAS far-IR fluxes for 6 HII regions in the LMC have been studied by DeGioia-Eastwood (1992). These regions are the sites of massive star formation, where the radiative heatingsource is young stars rather than the general interstellar radiation field. Such regions are expected to lie in stellar complexes and/or to be the stage just before the stellar complex is formed.
The highly structured diffuse X-ray emission of the LMC has been imaged in
detail by ROSAT. The brightest regions are found east of LMC X-1 and in the
30 Doradus region. The latter is strikingly similar to the optical picture.
There is a strong correlation between diffuse features in the X-ray image and
ESO colour images of the LMC in visible light. Bright knots in the X-ray map
correspond to HII emission in the optical (Westerlund 1997). The
distribution of the SNRs in the LMC shows (i) a clumping of objects in the 30 Doradus region, (ii) several remnants within the Bar of the LMC and (iii) that
the remainder of the remnants are found in super-associations. Most SNRs in the
Bar are in regions where many young clusters are located, clusters as young as
(Westerlund 1997).
The LMC has been well studied in the radio continuum, which is connected to
the formation of new and massive stars. Fukui et al. (1999, 2001) found that
the molecular clouds in the LMC have a good correlation with the youngest
(
10 Myr) stellar clusters, while there is little spatial correlation of
these clouds with SNRs or with the older stellar clusters.
In this paper we describe how the stellar complexes were detected, using optical data and we give their location and dimensions. The total flux of each structure is presented. Their derived IR properties are compared to IR properties of galaxies in order to identify the distinction between ordinary stellar complexes and active star formation regions. Possible connection of the complexes determined here with known X-ray detected SNRs and candidates as well as HII regions is discussed. Finally, their correlation between high resolution radio data at 8.6-GHz and CO emission is examined, in order to determine the activity of the complexes and their evolution.
The large-scale structures in nearby galaxies require extended field
observational material in order to be treated homogeneously. Therefore
we used direct photographic plates taken
with the UK 1.2 m Schmidt Telescope, in various wavebands: U, R and HeII (
Å) down to a magnitude limit of
.
These plates were digitised using the fast measuring
machines APM and SuperCosmos. The derived data were produced as catalogues of
detected stellar images. Star counts were performed on the above catalogues
in order to derive isopleth contour maps of the LMC in the various wavebands
and magnitude slices, to trace the differences between faint and brighter
stellar populations. Star counts, in the optical wavelength range, of large areas in the LMC have
revealed 56 groupings of young stars, known as stellar complexes (with
dimensions from 150 pc to
1500 pc). Their coordinates, dimensions and properties are given in Table 2, whereas their ages span from a few
to very young (
). The ages are derived from their stellar component, as described by Maragoudaki et al. (1998), which consist of early type stars (O, B, A),
dust, young clusters and associations, very often in groups. The parental
density fluctuations, which were fragmented into stellar complexes can be
explained as a result of the close encounter of the SMC with the LMC that
happened a few
ago (Gardiner & Noguchi 1996;
Kunkel et al. 2000).
IRAS all-sky survey Images taken at 12, 25, 60 and 100
m have been
obtained from SkyView (http://skyview.gsfc.nasa.gov/skyview.html) for the
whole area of the LMC to study the IR properties of the stellar complexes
detected in the optical domain.
From the IRAS catalogues we calculated a total flux for each complex as the
sum of the fluxes corresponding to the pixels, which cover the predetermined
complex area. These total fluxes were corrected from the background.
The background value was assumed as the average of four flux/pixel values at the
four rather clear corners of each frame, for all IRAS wavelengths
respectively. The background corrected total
fluxes were averaged to a mean value (flux/pixel in MJy/sr) for all
complexes so that they can be more easily compared with the literature.
Figure 1 shows the IRAS two-colour diagram of
vs.
for the detected stellar complexes. The black-filled
squares represent the integrated values for NGC 1068, M 82, M 31 and LMC
respectively, indicating the loci of different types of galaxies on this
diagram. NGC 1068 is a prototype AGN (Rowan-Robinson & Crawford 1989),
M 82 is a prototype starburst galaxy, while M 31 is a typical disk galaxy (Rice et al. 1988). The LMC HII regions of DeGioia-Eastwood (1992) are plotted with circles. We notice that many stellar complexes lie around the location of M 82, a prototype starburst, and the HII regions revealing enhanced star formation activity.
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Figure 1: IRAS colour-colour diagram for the detected stellar complexes. The black-filled squares mark the observed colours of the LMC (irregular galaxy) and three typical galaxies: M 31 (disk), M 82 (starburst) and NGC 1068 (AGN). The circles mark LMC HII regions. |
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Figure 2:
IRAS flux density in
|
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The IRAS flux densities in
versus the IRAS colour
for all the large structures detected here are illustrated in Fig. 2.
Lehnert & Heckman (1996) seeking to improve our
understanding of the range of physical processes occurring within IR selected
galaxies, found that the starburst galaxies are IR "warm'' if
(
)
and IR "bright''
if
Jy (
). From Fig. 2 it is
obvious that nearly 1/3 of the detected stellar complexes fulfil the criteria
defined by Lehnert & Heckman (1996) for the starburst galaxies.
The three upper points correspond to regions in 30 Doradus (complexes C17,
A21, A24), where there is the highest concentration of SNRs. The 15 structures
that have
and
,
resemble
the behaviour of starburst galaxies, whereas the rest 41 do not show enhanced
star formation activity.
We used the recently published 8.6-GHz map of Dickel et al. (2005),
with its angular resolution of 20
and linear resolution
5 pc
and the CO (1
0) line that was fully mapped by Fukui et al.
(2001), with angular resolution of 2.6
corresponding to a spatial resolution of
40 pc. In Fig. 3 we have superimposed
the stellar aggregates, complexes and super-complexes (yellow lines) onto the
radio 8.6-GHz (grey-scale) and CO (red contours) map. The time sequence evident
in this figure is such that the molecular gas (CO) traces regions of ongoing and
(near-) future star formation, the ionised gas (8.6-GHz) locates ongoing and
somewhat evolved star formation (107
108 yr). We examined the
correlation between 8.6-GHz radio emission, the CO emission and the location
of the 56 stellar complexes (Table 2, Cols. 8 and 9).
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Figure 3:
Maps of the LMC at 8.6 GHz (grey-scale) and in the
CO (1
|
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We notice that the majority (13 out of 15) of the regions
with
,
coincide well with the 8.6-GHz radio emission. The
existence of CO emission in seven of them, reveals future star formation
activity. The rest 2, that lack both 8.6-GHz and CO radiation, are actually
found to have values of F60 very close to 5.4 Jy.
Considering the 41 regions with
F60<5.4 Jy, the opposite behaviour is
revealed. 36 out of 41 regions do not exhibit significant amount of 8.6-GHz
radiation, while the remaining 5 that do exhibit 8.6-GHz radiation, are found
to have F60 very close to 5.4 Jy.
The CO emission is indicative of on-going and possible future star formation activity and there is no pattern revealed regarding the F60 of the complexes. 16 out of the 56 complexes have significant CO emission, indicating possible future star formation activity and only 10 of them are correlated with 8.6-GHz emission as well.
From optical observations, 56 stellar complexes are revealed in an area of
6
of the LMC. The IR properties are studied using the IRAS fluxes. The ratio of the flux densities
F60/F100, the flux density F60 as discussed above, the 8.6-GHz and CO radio emission, will be used in order to classify these complexes.
As mentioned in Sect. 3, Lehnert & Heckman (1996) showed that
starburst galaxies are IR "warm'' and "bright''. In the same manner, we
adopt the equivalent term "starburst regions'' for complexes that are
found to fulfil these criteria, namely
and
Jy. In addition, complexes that do not fulfil the previously stated
criteria will be called "active complexes''.
A more detailed study of high resolution 8.6-GHz map (Fig. 3)
revealed that all complexes with F60 well above the 5.4 Jy limit are
very well correlated with the 8.6-GHz radio emission. In contrast, complexes
with F60 well below the 5.4 Jy limit lack 8.6-GHz emission.
However, 7 out of the 56 complexes (A5, A6, A7, C5, C7, C22 and A31) have
F60 close to the classification limit and deviate from the above
behaviour. Complex C22, for example, is well correlated with 8.6-GHz emission;
its F60(5.07
0.20 Jy) though is below the accepted limit.
In contrast A31 has F60 = 5.98
0.20 Jy, which would classify
it as a starburst region; however, there is no 8.6-GHz emission associated
with it. Since the F60 criterion is not trustworthy for these regions,
we additionally use the 8.6-GHz emission to classify the complexes as
"starburst candidates'' or "active complexes candidates'' depending on its
existence. Hence, using the 8.6-GHz radiation as an additional tracer in
tandem with the F60, we can classify the stellar complexes into 13 starbursts, 5 starburst candidates, 2 active complexes candidates and 36 active complexes as seen in Table 1. The characterisation of each complex is given in Table 2, Col. 10.
Table 1: Complexes characterisation.
Moreover, a discrimination concerning the evolution of all the complexes was attempted based on the CO data. More than half of the starburst and starburst candidate regions show enhanced CO emission indicating ongoing and future evolution, while the rest of them are thought to be more or less evolved. Regarding the active stellar complexes (and the two candidates), we found only 5 of them with significant amount of CO emission, giving additional indication of current star formation and revealing potential future starbursts. The lack of CO in the rest of them could indicate that these complexes have never been starbursts or that their starburst activity previously exhausted the molecular gas.
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Figure 4: The HII regions (triangles) and SNRs (squares), plotted over the stellar complexes as defined here. |
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In Fig. 4 we plotted the known SNRs and HII regions based on the literature (Williams et al. 1999; Haberl & Pietsch 1999; Filipovic et al. 1998; Sasaki et al. 2000) over the stellar complexes with triangles and squares respectively. The overplotted HII regions show an increased concentration in and around the very active star forming regions, as expected. Most of the defined starburst areas (and the candidates) are associated with SNRs. The detected complexes are also cross-matchedwith the catalogue of stellar associations (Gouliermis et al. 2003) and that of nebulae in the LMC (Davies et al. 1976). The majority of the complexes are loci of stellar associations, whereas all of them are associated with a large number of nebulosities (Table 2).
Acknowledgements
The authors wish to thank the British Council and the General Secretariat of Research and Technology for financial support. M. Kontizas would like to thank the University of Athens (ELKE) for partial financial support. Finally M. Kontizas, E. Livanou and I. Gonidakis are very much indebted to the Ministry of Education for the financial support through the "Pythagoras II'' program.
Table 2: List of the LMC stellar complexes. Column 1 indicates the adopted identification name. A denotes aggregate, C complex and SC super-complex. For a structure found inside a larger one, the name of the later is given in parenthesis. Columns 2-4 give the RA, Dec of the "centre'' of each stellar complex and its dimension. Columns 5-7 show the number of SNRs and candidates, stellar associations and number of Nebulae and Henize objects found in each complex. Columns 8 and 9 indicate presence of 8.6-GHz and CO line emission respectively. Finally in Col. 10 the complexes are characterised. I indicates starbursts; II starburst candidates; III active complexes candidates and IV active complexes.
Table 3:
List of the derived IRAS fluxes (MJy/sr per pixel), luminocities
(in units of solar luminocities) of the identified stellar groupings at 12,
25, 60 and 100
m, the IRAS ratio
F60/F100 and the flux at 60
m in Jy per pixel.