A&A 396, L25-L29 (2002)
DOI: 10.1051/0004-6361:20021623
J. S. Clark1 - I. Negueruela2,3
1 - Department of Physics and Astronomy, University College London,
Gower Street, London, WC1E 6BT, England, UK
2 -
Observatoire de Strasbourg, 11 rue de l'Université,
67000 Strasbourg, France
3 -
Dpto. de Física, Ingeniería de Sistemas y Teoría de
la Señal, Universidad de Alicante, Apdo. 99, 03080 Alicante, Spain
Received 2 October 2002 / Accepted 7 November 2002
Abstract
We report the discovery of a hitherto undetected population
of Wolf-Rayet stars
in the young galactic open cluster Westerlund 1. Optical spectroscopy of the
cluster identified 11 such objects; provisional classification suggests that 6 are nitrogen rich (WN) and 5 carbon rich (WC). Including the previously identified Blue, Yellow & Red Super- & Hypergiants,
Westerlund 1 clearly has a very rich population of massive post-Main Sequence objects.
To date, the post-MS population of Westerlund 1 is significantly larger than that of any other galactic young open cluster - with the possible exception of the Arches -
implying that it is potentially amongst the most massive young clusters yet identified in the Local Group.
Key words: stars: evolution - stars: Wolf Rayet - galaxies: starbursts
The highly reddened young open cluster Westerlund 1
(henceforth Wd 1) was first
identified by Westerlund (1961).
Subsequent broadband photometric surveys by Borgman et al. (1970), Lockwood (1974) and Koornneef
(1977) suggested the presence of a number of both early
and late type supergiants, while a comprehensive photometric and
spectroscopic survey of the
brightest cluster members was presented by Westerlund
(1987; West87). Despite reporting the
presence of a large number of very luminous
(
)
transitional objects
only one further (photometric) study of the cluster has been
made (Piatti et al. 1998).
Recently, radio continuum observations of Wd 1 revealed that a number of the cluster members appeared to be associated with very bright radio sources (Clark et al. 1998; Dougherty et al. in prep.). Motivated by these results we obtained low resolution optical spectroscopy of a number of the brighter cluster members in order to provide an accurate spectral classification for them. In this paper we present the first results of this program; the discovery of a significant population of Wolf-Rayet (WR) stars within the cluster.
Due to the crowded nature of the field, each long slit integration included a number of different cluster members. Examination of the fainter objects present in several of the exposures revealed the presence of a number of objects with rich emission line spectra (see Figs. 1 and 2). Given that the integrations were optimised to avoid saturating on the brighter cluster members, the serendipitous sources are of a low S/N ratio - though sufficient to identify the emission line objects as a previously unidentified population of massive, hydrogen depleted WRs.
Despite the low S/N of many of the spectra, it is immediately possible to identify both nitrogen rich WN (6 objects) and carbon rich WC (5 objects) stars (Figs. 1 and 2 respectively); a finding chart and co-ordinates for each object are presented in Fig. 3 and Table 1.
Accurate determination of the spectral types of the WN and WC stars in this spectral region is difficult, given that most commonly used diagnostics lie at shorter wavelengths. However initial spectral classification of the WR candidates using the catalogues of Vreux et al. (1983, 1990) was possible.
For preliminary classification of the WC candidates we use the ratio of
the C III(8500 Å)/C IV(8856 Å) and
C II(9900 Å)/C III(9710 Å)
lines (Vreux et al. 1983; Howarth & Schmutz 1992; Crowther priv. comm.).
C IV(8856 Å) is absent from the spectra of all candidates,
with an upper limit to emission in candidates F, E and C constraining
spectral types to later than WC6. No constraints are possible for H and K
due to weak or no emission in C III(8500 Å)).
C II(9900 Å)/C III(9710 Å) ratios of
,
and
for candidates F, E and H respectively,
suggest WC9 classifications while a
ratio of <0.08 suggests a WC8 classification for
candidate C
, while
a classification for candidate K is not possible.
Classification of the WN spectra proved more difficult, as there are fewer lines present and there is no linear progression in e.g. the N IV:He II ratios that might be used for classification
(Vreux et al. 1983).
Based on the strength of the N IV 7103-7128 Å feature we can exclude extreme WN3/WN9
subtypes for all objects, since these are the only spectral types for which it is not seen in emission.
Candidate A appears to be a WNE (WN4-5) given the large lines widths (
3000 kms-1)
and lack of
strong He I 7065 Å emission (seen for all stars between WN6-8; Vreux et al. 1983, 1990).
On the basis of emission in this line and the small emission line widths, candidates G, I and D appear to be WN6-8 objects.
Classification of candidates B and J is complicated by the low S/N in the blue
regions of the spectra due to the CCD response curve, but are also probably WNL objects.
![]() |
Figure 1: Spectra of the newly discovered WN candidates in Wd 1, with prominent transitions identified. |
| Open with DEXTER | |
![]() |
Figure 2: Spectra of the newly discovered WC candidates in Wd 1 with prominent transitions identified. |
| Open with DEXTER | |
![]() |
Figure 3: R broadband finding chart for the newly discovered Wolf Rayet candidates in Wd 1. Note that the exact counterparts of candidates H, J and K should be regarded as provisional since the crowded field in these regions of the cluster make identification of the correct counterpart difficult. Candidates A, E and F correspond to stars number 72, 241 and 239 respectively in the notation of West87. |
| Open with DEXTER | |
| Candidate | ||
| A | 16h47m8.324s | -45 |
| B | 16h47m5.354s | -45 |
| C | 16h47m4.395s | -45 |
| D | 16h47m6.243s | -45 |
| E | 16h47m6.056s | -45 |
| F | 16h47m5.213s | -45 |
| G | 16h47m4.015s | -45 |
| H | 16h47m3.905s | -45 |
| I | 16h47m1.668s | -45 |
| J | 16h47m0.885s | -45 |
| K | 16h47m2.697s | -45 |
Unfortunately, uncertainty in the distance and reddening estimates to Wd 1 (West87; Piatti et al. 1998), coupled with the poorly determined bolometric corrections for many massive transitional objects make determination of the luminosities of the WRs and the other evolved cluster members difficult. Indeed, the lack of accurate luminosity estimates for the yellow hypergiant candidates (YHG; West87) is particularly concerning, given that bolometric luminosity is one of several classification criteria for such objects (e.g. de Jager et al. 1998). If we are to constrain the post-MS population of Wd 1 in order to determine such fundamental properties as cluster age and mass we must address these issues.
For the WR candidates A, E and F (for which West87 provide photometry), adopting the
reddening and distance estimates given by West87
and the (conservative) bolometric corrections of
Smith et al. (1994) we find that their luminosities comfortably exceed 10
.
For luminous A, F and G stars
the strength of the O I 7774 Å feature can be used to
provide an additional measure of the absolute
visual magnitude
.
Comparison of the YHG candidates W4, W12, W16 and W265 and the YSG W7
(notation from West87) to the luminosity: line strength calibrations
of Ferro & Mendoza (1993) and Slowik & Peterson
(1995) indicates that they are all likely to be
intrinsically highly luminous. Indeed the EW(O I)
for these objects are significantly greater than any of the
stars in these studies - including
the bona fide YHG
Cas
(
)
-
implying luminosities of
.
Additionally, high mass loss
rates for these objects are implied by radio detections (W4, W12, W16 and W265) and broad H
emission (W7, W12, W16 and W265); therefore all these objects meet the classification
criteria of de Jager (1998) for bona fide YHGs.
Including the WRs and YHG candidates, the large population of luminous post-MS
objects in Wd 1 (West87 and Table 4)
suggests that it is unique in both the number and variety of massive
post-MS objects present. Of the 26 clusters within the solar circle studied
by Eggenberger et al. (2002), 6 contain both B and RSGs.
Of these, only 3 - Collinder 228, Trumpler 27 and Berkley 87 -
also contain WRs (1-2 per cluster; Table 4) and only
Trumpler 27 contains a yellow SG, albeit of significantly lower luminosity (
)
than those in Wd 1 (Massey et al. 2001;
note however that they claim the cluster is not co-eval.).
Of the galactic centre clusters, the Quintuplet cluster appears to contain 8 WRs of both WN and WC types along with a number of early OB supergiants
and a single RSG (10
;
Figer et al. 1999).
In addition to the single luminous RSG IRS 7 (10
;
Carr et al.
2000), Paumard et al. (2001) detect 16 "helium stars''
in the Galactic Centre cluster, of which they suggest the 7 narrow line objects correspond to mass losing BSGs (possible LBVs) and the 9 broad line
objects WRs (noting that a further 3 stars Blum et al. (1996) suggest are WCs lie outside their f-o-v).
Only the Arches cluster - which is significantly younger - appears to contain a comparable number of WRs to Wd 1, with Blum et al. (2001) identifying 15 candidate O4 If/WN7 stars
on the basis of narrow band imaging. However, as with the Quintuplet and Galactic Centre clusters, the
rich population of very luminous cool stars present in Wd 1 is absent
.
Clearly, such comparisons indicate that Wd 1 is both very young and very massive; however uncertainties in the post-MS evolution of massive stars, exacerbated by the lack of an identifiable MS turnoff and accurate bolometric luminosities for the evolved stars makes determination of the age and total mass of Wd 1 difficult.
Following the analysis of the Quintuplet cluster by Figer et al. (1999),
the presence of WC stars - apparently the most evolved stars present in Wd 1 -
implies a lower limit to the age of 2.5 Myr.
The presence of a number of very luminous RSGs within Wd 1 potentially provides
an upper limit to the cluster age; Figer et al. (1999) suggests that the Quintuplet
cluster requires an age of
4 Myr given the presence of a single (low luminosity) RSG,
broadly consistent with the age (7 Myr) Carr et al. (2000)
claim for IRS 7. However, large
uncertainties in the mass loss rate for very luminous cool stars render estimates of their ages, lifetimes
and progenitor masses highly uncertain; particularly concerning given the large population of YHGs
within Wd 1.
| Candidate | A | G | I | B | J | D |
| Transition | ||||||
| He II 6560 | 27 | S/N | 9 | S/N | S/N | S/N |
| He I 6678+He II 6683 | - | 30 | 37 | S/N | S/N | S/N |
| C IV 7061+He I 7065 | - | 59 | 50 | 45 | - | 46 |
| N IV 7103-28 | 110 | Bl | Bl | Bl | 19 | Bl |
| He II 8237 | 33 | 20 | 19 | 12 | 7 | 11 |
| HeII 5-8? | 38 | - | - | - | - | - |
| He II 10124 | 106 | 56 | 42 | 33 | 32 | 41 |
Considering their extreme rarity, the lifetime of YHGs is probably less than 105 yr for any
luminosity and progenitor mass. At very high luminosities it is likely that a very large mass
loss rate limits the YHG to a single passage from red to blue across the HR diagram, resulting in
a short lifetime (
30 000 yr; Stothers & Chin 1999). At lower luminosities
dynamical instabilites in the outer atmosphere of the star result in multiple blue loops for the
star out of the RSG region, leading to a longer lifetime as a luminous yellow star (e.g. Stothers & Chin 2001). Such estimates are qualitatively consistent with the results of unpublished simulations for the behaviour of
and 40
stars (Maeder
& Nieuwenhuijzen, priv. comm. 2002) which suggest YHG phases after 6.9 and 4.4 Myr lasting
49 000 and 2700 yr respectively; i.e. the YHG phase occurs earlier and
is shorter the more massive the progenitor is.
Despite the many uncertainties, the present stellar population of Wd 1 appears consistent with an
age of order 4-8 Myr if the cluster is co-eval, suggesting it is potentially
younger than previously thought (7 and
Myr; West87 and Piatti et al. 1998, respectively).
The uncertainties in post-MS evolution and incomplete stellar census inevitably makes a
determination of the total cluster mass uncertain. Maeder & Meynet (1994) find that for
solar metallicities, adopting twice the standard mass loss rate results in the appearance of
a WN phase for stars
25
- consistent with the findings of Massey et al.
(2001) - and a WC phase at
40
.
Given that the super- and
hyper-giants are less chemically evolved than the WRs, their progenitors are likely to
have been less massive.
Regarding the completeness of our sample we estimate that the spectral survey of potential cluster members of a similar visual
magnitude as the fainter WR candidates is at best 33 per cent complete, while preliminary analysis of our low resolution optical
spectroscopy (Negueruela & Clark, in prep.) finds many additional supergiant candidates
e.g. W70 and W71 (BSG), W32 and W33 (YSG) and W75 and W237 (RSG). Additionally, we might expect that if originally present
very massive stars will have been lost to SN; Maeder & Meynet (1994) suggest that stars of
85
will have a lifetime comparable to the lower estimate of the cluster age.
| Candidate | F | E | C | H | K |
| Transition | |||||
| He II 6560+C II 6578 | 42 | 49 | S/N | S/N | 13 |
| He I 6678 | 9 | 17 | S/N | S/N | - |
| C II 6725-42+C III 6727-73 | Bl | Bl | S/N | S/N | - |
| C II 6780 | 28 | 45 | S/N | S/N | - |
| C III 7037 | Bl | Bl | S/N | S/N | - |
| He I 7065+C II 7064 | 15 | 32 | S/N | S/N | - |
| C II 7236+C III 7210-12 | 55 | 108 | 45 | 24 | 3 |
| C III 7772-96 | S/N | 8 | S/N | - | - |
| C III 8196 | 12 | 15 | 16 | 5 | - |
| C III 8256 | Bl | 9 | Bl | - | - |
| C III 8328-59 | 39 | 27 | 18 | 10 | - |
| C III 8500 | 14 | 17 | 11 | 6 | - |
| C III 8664 | 19 | 12 | - | - | - |
| He II 9225+ C II 9224 | 16 | 25 | 20 | 14 | - |
| C III 9705 | 103 | 139 | 97 | 50 | 26 |
| C II 9903 | 18 | 25 | S/N | 9 | - |
Nevertheless, conservatively assuming that the present stellar census
is complete (see Table 4) and furthermore that the progenitor masses for these objects were
30
we can derive a lower limit to the initial cluster mass.
Adopting a Salpeter mass function (
)
with upper and lower cut
offs of 100
and 0.2
respectively and a slope,
)
we might
expect a total mass of stars of
750
for every star with an initial mass of
30
,
leading to a mass estimate of a few
(S. Goodwin priv. comm. 2002).
This lower limit to the initial mass of Wd 1 suggests that it is directly comparable to the galactic centre clusters such as
the Arches cluster (
;
Portegies Zwart et al. 2001). More reasonable estimates of completeness and
progenitor mass suggest a mass for Wd1 of a few
making it by far the most massive young Galactic cluster, and
one of the most massive in the Local Group. This conclusion is further reinforced by
considering the large number of YHGs within Wd 1, which is comparable
to the total population of the Milky Way (6; de Jager 1998). Assuming a lifetime for the YHGs of
25 000 yr,
following the arguments of Geballe et al. (2000) for the likelihood of finding several examples of a short lived evolutionary
phase within a single cluster also leads to the conclusion that a very large O star population (
several hundred)
is required to produce the number of YHGs observed.
Evidently a combined spectroscopic and photometric approach to both identify the MS turn-off and to properly classify evolved stars will be required to accurately determine the age and mass of Wd1. However if the above estimates are correct then Wd 1 would appear to be a Galactic equivalent of the super star clusters observed in merging and interacting galaxies and may possibly be more massive than the 30 Doradus cluster in the LMC. Therefore, as well as providing a unique laboratory for studying hot star evolution, Wd 1 would provide an unprecidented insight into an extreme mode of cluster formation, previously not thought to be occuring in the Milky Way.
| Cluster | Age(Myr) |
|
|
|
| Wd 1 | 4-8 | |||
| Trumpler 27a | NA | 8 | 1 | 2 |
| Collinder 228a | 3 | 1 | 1 | |
| Berkley 87a | 4 | 1 | 1 | |
| Quintupletb | 14 (+ 2 LBVc) | 1 | 8 | |
| Gal. Centerc,d | 3-8 | 7 He I | 1 | 9 He I |
| Archese | 2-4.5 | 0 | 0 | 15 |
Acknowledgements
We thank S. Goodwin, R. Stothers, R. Waters, S. Dougherty, P. Crowther, K. de Jager and H. Nieuwenhuijzen for informative discussions and the referee, W.-R. Hamann, for his constructive comments.