Issue |
A&A
Volume 516, June-July 2010
|
|
---|---|---|
Article Number | A55 | |
Number of page(s) | 29 | |
Section | Galactic structure, stellar clusters, and populations | |
DOI | https://doi.org/10.1051/0004-6361/200913451 | |
Published online | 24 June 2010 |
Properties of stellar generations in
globular clusters and relations with global parameters
,![[*]](/icons/foot_motif.png)
E. Carretta1 - A. Bragaglia1 - R. G. Gratton2 - A. Recio-Blanco3 - S. Lucatello2,4 - V. D'Orazi2 - S. Cassisi5
1 - INAF - Osservatorio Astronomico di Bologna, via Ranzani 1, 40127
Bologna, Italy
2 - INAF - Osservatorio Astronomico di Padova, vicolo dell'Osservatorio
5, 35122
Padova, Italy
3 - Laboratoire Cassiopée UMR 6202, Université de Nice
Sophia-Antipolis, CNRS, Observatoire de la Côte d'Azur, BP 4229,
06304 Nice Cedex 4, France
4 - Excellence Cluster Universe, Technische Universität München,
Boltzmannstr. 2, 85748 Garching, Germany
5 - INAF - Osservatorio Astronomico di Collurania, via M. Maggini,
64100 Teramo, Italy
Received 12 October 2009 / Accepted 2 March 2010
Abstract
We revise the scenario of the formation of Galactic globular clusters
(GCs) by
adding the observed detailed chemical composition of their different
stellar
generations to the set of their global parameters. We exploit the
unprecedented set of homogeneous abundances of more than
1200 red giants in 19 clusters, as well as additional
data from literature, to give a new definition of bona fide
GCs, as the stellar aggregates showing the Na-O anticorrelation. We
propose a classification of GCs according to their
kinematics and location in the Galaxy in three populations: disk/bulge,
inner
halo, and outer halo. We find that the luminosity function of GCs
is fairly independent of their population, suggesting that it is
imprinted by
the formation mechanism only marginally affected by the ensuing
evolution.
We show that a large fraction of the primordial population should have
been
lost by the proto-GCs. The extremely low Al abundances found for the
primordial population of massive GCs indicate a very fast enrichment
process before the formation of the primordial population. We suggest a
scenario for the formation of GCs that includes at least three main
phases: i) the formation of a precursor population (likely due
to the interaction of cosmological structures similar to those that led
to the formation of dwarf spheroidals, but residing at smaller
Galactocentric distances, with the early Galaxy or with other
structures); ii) the triggering of a long episode of star
formation (the primordial population) from the precursor population;
and iii) the formation of the current GC, mainly within a
cooling flow formed by the slow winds of a fraction of the primordial
population. The precursor population is very effective in raising the
metal content in massive and/or metal-poor (mainly halo) clusters,
while its rôle is minor in small and/or metal-rich (mainly disk) ones.
Finally, we use principal component analysis and multivariate relations
to study the phase of metal enrichment from first to second generation.
We conclude that most of the chemical signatures of GCs may be ascribed
to a few parameters, the most important being metallicity, mass, and
cluster age. Location within the Galaxy (as described by the
kinematics) also plays some rôle, while additional parameters are
required to describe their dynamical status.
Key words: stars: abundances - stars: atmospheres - stars: Population II - globular clusters: general
1 Introduction
The assembly of the early stellar populations in galaxies is one of the hottest open issues in astronomy. Globular clusters (GCs) are a major component of these old stellar populations. They are easily detectable and can be studied in some detail even at large distances, providing a potentially powerful link between external galaxies and local stellar populations. A clear comprehension of those mechanisms that led to the formation and evolution of GCs and of the relations existing between GCs and field stars is a basic requirement for understanding how galaxies assemble (see e.g. Bekki et al. 2008). Various authors have proposed scenarios for the formation of GCs (Peebles & Dicke 1968; Searle & Zinn 1978; Fall & Rees 1985; Cayrel 1986; Freeman 1990; Brown et al. 1991, 1995; Ashman & Zepf 1992; Murray & Lin 1992; Bromm & Clarke 2002; Kravtsov & Gnedin 2005; Saitoh et al. 2006; Bekki & Chiba 2002, 2007; Bekki et al. 2007; Hasegawa et al. 2009; Marcolini et al. 2009; Hartwick 2009). While very suggestive and intriguing, these scenarios either do not convincingly reproduce the whole spectrum of observations, or are likely to be incomplete, describing only part of the sequence of events that lead to GC formation or only a subset of them. We still lack the clear understanding we would need; however, some recent progress is opening new promising perspectives.
For almost forty years, we have known that large star-to-star abundance variations for several light elements are present in GCs (see Gratton et al. 2004, for a recent review). Regarded for a long time as intriguing abundance ``anomalies'' restricted to some cluster stars, the observed peculiar chemical composition only recently was explicitly understood as a universal phenomenon in GCs, most likely related to their very same nature/origin (Carretta 2006; Carretta et al. 2006, Paper I). The observational pattern of Li, C, N, O, Na, Al, Mg in cluster stars has currently been assessed (see e.g. the review by Gratton et al. 2004), thanks to several important milestones:
- (i)
- Variations for the heavier species (O, Na, Mg, Al) are restricted to the denser cluster environment. The signature for other elements (Li, C, N) may be reproduced by assuming a mixture of primordial composition plus evolutionary changes. The latter were caused by two mixing episodes, occurring at the end of the main sequence (the first dredge-up) and after the bump on the red giant branch (RGB), both in low-mass Population II field stars and in their cluster analogues (Charbonnel et al. 1998; Gratton et al. 2000b; Smith & Martell 2003).
- (ii)
- The observed pattern of abundance variations is established in proton-capture reactions of the CNO, NeNa, and MgAl chains during H-burning at high temperature (Denisenkov & Denisenkova 1989; Langer et al. 1993).
- (iii)
- The variations are also found among unevolved stars currently on the main sequence (MS) of GCs (Gratton et al. 2001; Ramirez & Cohen 2002; Carretta et al. 2004; D'Orazi et al. 2010). This unequivocally implies that this composition has been imprinted in the gas by a previous generation of stars. The necessity of this conclusion stems from low-mass MS stars not being able to reach the high temperatures for the nucleosynthetic chains required to produce the observed inter-relations between the elements (in particular the Mg-Al anticorrelation). This calls for a class of now extinct stars, more massive than the low-mass ones presently evolving in GCs, as the site for the nucleosynthesis.
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Figure 1: Summary of the Na-O anticorrelation observed in the 19 GCs of our sample. Arrows indicate upper limits in O abundances. The two lines in each panel separate the primordial component (located in the Na-poor/O-rich region), the Na-rich/O-poor extreme component, and the intermediate component in-between (called P, E, and I, respectively as indicated only in the first panel). See Sect. 2 for details. |
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The observed abundance variations are also connected to the He
abundance, since He is the main outcome of H-burning (i.e., Na-rich,
O-poor stars should also be He-rich). However, the relation between He
abundance variations and
the light element abundance pattern may be quite complicated. Multiple
main sequences attributed to populations with different He fraction Y
have recently been found in some GCs ( Cen, see Bedin
et al. 2004,
and NGC 2808, Piotto et al. 2007). We
have found a clear indication that Na-rich and Na-poor stars in
NGC 6218 and NGC 6752 have slightly different
RGB-bump luminosities (Carretta et al. 2007b,
hereinafter Paper III), as expected from models of cluster
subpopulations with different He content (Salaris et al. 2006).
In separate papers (Gratton et al. 2010; Bragaglia
et al. 2010),
we examined the relation between He and light element abundance
variations from evidence based on horizontal branch (HB) and
RGB.
In summary, GCs are not exactly a simple stellar population, because they must harbour at least two stellar generations, as explained above, that are clearly distinct by their chemistry. These populations may be separated, provided data of adequate quality are available. The patterns of anticorrelated Na-O and Mg-Al and, partly, C-N and Li-Na (and associated correlations) must be regarded as the fingerprints of these different subpopulations, and may be used to get insight into the early phases of formation and evolution of GCs, which are still obscure. The timescale for the release of matter processed by H-burning at high temperature is of the order of 107 yr if it comes from FMRS and a few times longer if it comes from massive AGB stars. Thus, whatever the candidate producers, the observed patterns were certainly already in place within some 108 yr after the start of cluster formation. These processes occurred on timescales less than 1% of the typical total age of a GC. The dynamical evolution that occurred in the remaining 99% of the cluster lifetime, while likely important, did not completely erase these fingerprints. Their fossil record is still recognisable in the chemical composition of the low-mass stars.
To decipher the relevant information we need large and homogeneous data sets, like the one we have recently gathered (Carretta et al. 2009a,b). The goal of the present paper is to exploit this wealth of data to discuss the abundance patterns of the different populations within each GC. We correlate them with global cluster parameters, such as the HB morphology and structural or orbital parameters. This will allow a better understanding of the main properties of the stellar populations of GCs, hence getting insight into the early phases of their evolution. Using this information as a guide, we sketch a quite simple scenario for the formation of GCs, which is essentially an updated and expanded version of what was proposed more than thirty years ago by Searle & Zinn (1978). This scenario naturally explains the relation between GCs and other small systems (dwarf Spheroidals: dSphs), and suggests a connection between GCs and field stars. In fact, we propose that the primordial population of GCs might be the main building block of the halo, although other components are likely present.
The present paper is organised as follows. In Sect. 2 we give a
brief summary of our previous work to set the stage for the following
discussion. In Sect. 3
we recall some general properties of the GC
population and the division into subpopulations; we also present the
selection
criteria for our sample, discussing possible biases, and the parameters
used in
the analysis. In Sect. 4
we discuss the properties of the first stellar generation, and we
present a scenario for GC formation. In Sect. 5 we
consider the second phase of chemical enrichment in GCs, comparing the
properties of the second generation with those of the primordial one
and
presenting a number of interesting correlations. Finally, in
Sect. 6,
we more generally discuss the correlations with global GC parameters
and give a summary and our conclusions. In the Appendix, we present a
new classification
of all Galactic GCs, dividing them into disk/bulge, inner halo, and
outer halo
ones on a kinematical basis and list their metallicities on the scale
defined in Carretta et al. (2009c), their
ages, re-determined from literature using these metallicities, and a
compilation of [/Fe]
values that are used throughout the paper.
2 Synopsis of previous results
Before starting our present discussion, we summarise the results of our project ``Na-O anticorrelation and HB'' (Carretta et al. 2006). Up to a few years ago, obtaining adequate high-resolution spectroscopic data sets was painstaking, since stars had to be observed one-by-one. Thanks to the efforts of many researchers, mainly of the Lick-Texas group, spectra of some 200 stars in a dozen GCs were gathered using tens of nights over several years (see the reviews by Kraft 1994; Sneden 2000, and references therein). In the past few years, we used the spectacular data-collecting capability offered by the FLAMES multi-object spectrograph at the ESO VLT to secure spectra for more than 1400 giant stars, distributed over about 12% of all known GCs. With the increase of an order of magnitude in available data, the paradigm has changed. We now understand that the observed anticorrelations are not indicative of ``anomalies'', rather we are dealing with the normal chemical evolution of GCs.
Our survey has already been amply described elsewhere. Results for the first five GCs have been presented in a series of papers (Papers I through VI: Carretta et al. 2006, 2007a,b,c; Gratton et al. 2006, 2007), while the remaining clusters are analysed in Carretta et al. (2009a,b: Paper VII and VIII). In Fig. 1 we show a collage of the Na-O anticorrelations observed in all 19 clusters in our sample. Solid lines separate the primordial, intermediate and extreme populations, whose concept is introduced and defined in Paper VII and recalled briefly below.
We obtained GIRAFFE spectra (at
,
comprising the Na I
568.2-568.8 nm, 615.4-6.0 nm and [O I]
630 nm lines) of about 100 stars
per cluster. At the same time, we also collected UVES spectra (at
,
covering the 480-680 nm region, and providing information
about Mg, Al, and Si, in addition to O and Na) of about
10 stars (on average) per cluster. We homogeneously determined
the atmospheric parameters for these stars using visual and near-IR
photometry and the relations in Alonso et al. (1999,
2001). We
measured Fe, O, and Na abundances for more than 2000 stars (more than
1200 cluster members with both O and Na
detected), putting together the largest sample of this kind ever
collected.
The large number of clusters and stars per cluster allowed us to recognise that the amount of the abundance variations among different clusters is related in a non trivial way to global cluster parameters (Carretta 2006; Carretta et al. 2007a; 2009a, Paper VII: GIRAFFE data; 2009b, Paper VIII: UVES data). The GCs are dominated by the second (polluted) generation of stars, the fraction of primordial stars being roughly correlated with cluster luminosity. The Na-O anticorrelation has not only a different extension, but also a different shape, in different clusters, depending on cluster luminosity and metallicity. The Mg-Al anticorrelation is sometimes absent, this occurring in low-luminosity clusters. All these are clear indications that the polluters' properties change from cluster to cluster and that this change is apparently driven by the cluster luminosity and metallicity.
Carretta (2006) suggests using the interquartile range (IQR, the difference between the upper quartile and the lower quartile, see e.g. Tukey 1977) of the [O/Na] ratio as a quantitative measure of the extension of the Na-O anticorrelation. The IQR is useful because it is less influenced by extreme values, because it refers to the range of the middle 50% of the values, and because it is less subject to sampling fluctuations in highly skewed distributions. Statistically robust IQR values require large enough samples of stars. Our project was designed to obtain Na and O abundances for a large number of RGB stars in each cluster, typically 100 stars per cluster, although in some cases only a much smaller sample of stars could be used. The number of stars actually measured in each cluster depends on the richness of population, metallicity, S/N, and in some cases on field-star contamination (such as for the bulge clusters NGC 6388 and NGC 6441 or the disk clusters NGC 6171 and NGC 6838). The smallest sample (16 stars with both Na and O) is for NGC 6397, the largest (115 stars) for 47 Tuc (NGC 104).
![]() |
Figure 2: [Na/Fe] ratios as a function of the metallicity [Fe/H] in a range centred on the average metal abundance of NGC 6397. Filled triangles in grey-tones are field stars from Gratton et al. (2003a) and the compilation by Venn et al. (2004). Filled circles are stars in NGC 6397 with determinations of both O and Na (red: P component, blue: I component). Empty (green) star symbols are stars in NGC 6397 with only Na abundances derived. |
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![]() |
Figure 3:
Relative age parameter vs. absolute magnitude MV
for globular and old open clusters (see Appendix for details). Red
filled pentagons and triangles are GCs where Na-O anticorrelation has
been observed, in the Milky Way or the LMC, respectively; green squares
are clusters that do not show evidence of Na-O anticorrelation, both
members of Sagittarius dSph, either of the main body
(Terzan 7) or the stream (Pal 12). Open stars and
triangles mark clusters for which not
enough data is available, in the Milky Way or the LMC respectively.
Finally,
open circles are old open clusters (data from Lata et al. 2002).
Superimposed are lines of constant mass (light solid lines, see
Bellazzini et al. 2008a).
The heavy blue solid line (at a mass of
|
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In Paper VII we defined three population components in each
cluster: the first generation stars and two groups of second generation
stars. The lines separating the three components are shown in
Fig. 1.
The primordial P component includes stars between the minimum [Na/Fe]
observed and
[Na/Fe]
(see Paper VII).
These stars are defined as
first-generation objects since they show the same pattern of high O and
low Na typical of Galactic field stars of similar metallicity,
with the characteristic signature of core-collapse SNe. Since the
yields of Na are
metallicity-dependent (e.g., Wheeler et al. 1989), the
limit for the P component varies as a function of [Fe/H], as is evident
in
Fig. 1.
The separation between the two subcomponents of
second-generation stars (the intermediate I stars and the
extreme E stars) is
somewhat more arbitrary. On the basis of the [O/Na] distributions in
our
clusters, they were defined in Paper VII as those stars with [O/Na]
ratios
higher or lower than -0.9 dex, respectively.
Computing the fraction of stars in each component, we found that:
- (i)
- the extreme 2nd generation is not present in all GCs;
- (ii)
- the intermediate 2nd generation constitutes the bulk (50-70%) of stars in a GC;
- (iii)
- the primordial population is present in all GCs (at about the 30% level).
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3 Cluster and parameter selection
3.1 Definition of globular clusters
In this paper we intend to bring together the chemical properties derived from our in-depth study of various stellar populations in GCs with many other global observables. Moreover, we present a scenario for the formation of GCs in the more general context of the relationship between the Milky Way and its satellites. Thus, before entering into the discussion, we recall a few properties of the parent population of GCs that are of direct interest here.
The first point we would like to make concerns the operative
definition of bona fide GC. The distinction between
globular and other clusters (e.g., open clusters) is not well drawn,
and it is ambiguous in particular for the populous
clusters that are numerous in the Magellanic Clouds. To better clarify
this
point, we plot in Fig. 3
ages and absolute magnitudes for the
clusters listed in the database by Harris (1996, and web
updates). This list
includes 146 GCs. Seven of these GCs are actually thought to
be members of the
Sagittarius dwarf galaxy (see van den Bergh & Mackey 2004, and
references therein). To this sample, we add GCs in other satellites of
the Milky Way: 16 GCs in the Large Magellanic Cloud (LMC),
8 in the Small Magellanic Cloud (SMC), and 5 in the
Fornax dSph. Data for all these GCs are detailed in the Appendix.
Age data are actually available for slightly more than half of the
sample. We
also add a few old open clusters (NGC 188, NGC 6791,
Collinder 261, NGC 1193,
Berkeley 31, and Berkeley 39: data from Lata
et al. 2002)
that fall within the limits of the plot. From this figure, there is a
clear overlap between open clusters and objects from the list of GCs at
the faint end of the sequence. In
(almost) all studied GCs the Na-O anticorrelation has been found. One
exception
is Terzan 7, where no spread in O abundances has been found in
the (only) seven
stars observed by Sbordone et al. (2007), and may
then be the most massive
cluster observed so far without the Na-O anticorrelation. The other one
is Pal 12, where Cohen (2004)
finds very uniform O and Na abundances, but only for four stars.
Finally, there are GCs for which current data are not adequate to
state if a Na-O anticorrelation exists or not. Similar data are scarce
for open clusters (see Gratton 2007).
However, de Silva et al. (2009) have
compiled data for various old open clusters, finding no evidence of an
Na-O anticorrelation, and Martell & Smith (2009) did not
find any evidence of CN variation among
giants in three open clusters (including NGC 188). This
diagram indicates that
the Na-O and related anticorrelations have been observed in all old
clusters
with MV<-5.1
(which roughly corresponds to a mass of
for
old populations), including the vast majority of Galactic
GCs, and almost all the objects with a relative age parameter
>0.8. We
then propose to identify the GCs with those clusters where there is an
Na-O
anticorrelation. As we see in Sect. 4.1, this
identification
corresponds to a formation scenario that clearly separates GCs from
other
clusters. Operatively, we might also define GCs either as the old
clusters (age over 5 Gyr) with an MV<-5.1
or those with relative age parameter >0.8. These definitions
essentially include the same list of objects, at least in the Milky Way
and its satellites.
At the other mass limit for the GC population, the similarity
between GCs and
nuclei of dwarf galaxies has been pointed out by many authors (see e.g.
Freeman 1990;
Böker 2008;
Georgiev et al. 2009). Those nuclei or nuclear star
clusters of dwarf galaxies that can be studied in close detail (such as
M 54
for the Sagittarius galaxy) essentially share the full pattern of
properties
with GCs (see e.g. Bellazzini et al. 2008b;
Georgiev et al. 2009; Carretta et al. 2010),
although they may have wide spreads in Fe abundances, not observed in
GCs. This occurrence suggests that also Cen was (in) the
nucleus of a galaxy in the past.
3.2 Our sample of GCs
Ideally, we should have derived detailed chemical data for the
whole parent
population. However, this would have required too much observing time,
so we
analysed only a representative subset of clusters (representing
about 12% of
the total sample). The selection procedure was as follows. We started
from the complete sample of Galactic GCs, as listed by Harris (1996). We then
divided
clusters into different groups, according to the morphology of the HB.
For each group, we selected the two-four rich (MV<-5)
clusters, accessible from
Paranal (
),
with the smallest apparent distance modulus;
however, we did not consider some clusters that have quite large
differential
reddening (like M 22: Ivans et al. 2004
). The selected clusters
were: red HB clusters: NGC 104=47 Tuc, NGC
6838=M 71, NGC 6171=M 107;
Oosterhoff I clusters:
NGC 6121=M 4, NGC 3201, NGC
5904=M 5; blue HB clusters: NGC 6752, NGC
6218=M 12, NGC 6254=M 10,
NGC 288, NGC 1904=M 79; clusters with
blue, short HB's:
NGC 6397, NGC 6809=M 55; Oosterhoff II
clusters: NGC 7099=M 30, NGC
4590=M 68, NGC 7078=M 15; clusters
with very extended/bimodal distribution of stars on the HB: NGC
2808, NGC 6441, NGC 6388. As a result, within
each different class of HB
morphology, the sample is essentially distance-limited. On the other
hand, this
is not true for the whole sample, because the adopted limits depend on
the
morphological classes and reddening (so that clusters projected close
to the
Galactic plane are under-represented). However, for most classes
of HBs, the
limit is quite uniform at about
(m-M)V<14.5-15.5,
which is
10 kpc
from the Sun. We needed to sample a larger volume (
(m-M)V<16.5)
to include GCs with very extended/bimodal distribution of stars on the
HB, since these
clusters are rare. These choices mean that GCs with very extended blue
HB are over-represented in our sample (42% of the total).
3.3 The Galactic GC sample
To correctly explore the relations between the chemistry of different stellar generations and global GC properties, it is important to assess to what cluster population our programme GCs belong. Zinn (1985) demonstrated that Milky Way GCs can be divided into two main groups: disk (or bulge) GCs and halo GCs. This separation was done according to the metal abundance alone (with the limit at [Fe/H] = -0.8 dex). These two groups correspond to the main peaks of the metallicity distribution of GCs, but they can also be clearly distinguished from other properties (location in the Galaxy, kinematics, etc.). According to Searle & Zinn (1978), halo GCs result from the evolution of individual fragments, while disk clusters likely formed within the dissipational collapse. This distinction is thus likely to play an important rôle in defining the characteristics of GCs and, in particular, of their primordial population.
Further refinements (e.g., van den Bergh
& Mackey 2004;
Lee et al. 2007)
along Zinn's line of thought were done by using the HB morphology,
which is,
however, one of the features of GCs we intend to explain. In the
following, therefore, we adopt a combination of location in the Galaxy
and kinematics criteria to separate disk clusters from the halo ones. Full details are given in
the Appendix. Briefly, using the Harris (1996) catalogue,
we first classified as outer halo GCs the ones currently located at
distances greater than 15 kpc (Carollo et al. 2008) from the
Galactic centre, and clusters with Galactocentric distance less than
3.5 kpc
were instead considered as bulge GCs. To separate the inner halo
clusters from the disk ones, we used the rotational velocity around the
Galactic centre by Dinescu et al. (1999) and
Casetti-Dinescu et al. (2007) whenever
possible. When this information was not available, we used the
differences between the observed radial velocity (corrected to the LSR)
and the one expected from the Galactic rotation curve (see Clemens 1985). In the
Appendix we provide the disk/inner
halo/outer halo classification for each cluster listed in the Harris
catalogue. Finally, we consider GCs in the LMC and SMC and in dSphs
(Sagittarius and Fornax) as separate groups.
The procedure for selecting the programme sample, described in
Sect. 3.2,
results in a potential selection bias as a function of the distance.
This shows up in a correlation between a cluster's present-day mass (as
represented by the proxy of cluster total absolute visual magnitude, MV)
and distance modulus, so that in our sample more massive GCs are
typically the most distant ones. This correlation is at odds with the
total sample of GCs in the Harris (1996) catalogue.
However, since all programme GCs but one (NGC 1904, with
kpc)
are within 15 kpc of the Galactic centre,
they belong either to the disk or to the inner halo. Within this
subsample,
there is a correlation of MV
with Galactocentric distance similar to what
was noticed in our sample. We thus assume that our sample is
representative of
the properties of the disk and inner halo (but not of the outer halo)
GCs and
neglect the possible bias with luminosity.
![]() |
Figure 4: Cumulative luminosity functions of different groups of Galactic GCs (from the Harris 1996 catalogue) according to our present classification criteria and of GCs in dSphs (from van den Bergh and Mackey 2004; see Appendix for references on Fornax an LMC clusters). The red solid line indicates disk/bulge clusters, the blue dotted line the inner halo clusters, the dashed green line clusters in the outer halo, magenta dashed-dotted line is for clusters in dSphs, and the green-gold long dashed line for GCs in LMC. |
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Other properties of the parent population of Galactic GCs relevant to our discussion are the masses (luminosities) and the metallicities of the disk and inner halo GCs. These are two of the main parameters driving most of the observed properties of GCs, as we confirm later, so they are worth a few more words.
Inner and outer halo clusters have clearly distinct luminosity functions (LF), as illustrated by Fig. 4. Small clusters (MV> -6) only exist in the outer halo, where they make up half of the total. A Kolmogorov-Smirnov test returns a 1% probability that inner and outer halo LFs were extracted from the same population. Of course, this difference can be at least in part attributed to the destruction mechanisms, which are more efficient for clusters closer to the centre of the Galaxy. However, other mechanisms can also be considered. In fact, all young clusters (age parameter <0.8) reside in the outer halo, and they are all faint (MV>-6.5), overlapping open clusters in the MV/age distribution (Fig. 3). If we limit ourselves to old clusters (age parameter >0.82, essentially adopting the same definition of GC considered in Sect. 3.1), there is no clear difference between the LF of inner halo or disk and that of outer halo clusters (Kolmogorov-Smirnov tests applied to the distributions of GCs having age parameter result into a significance of 16 and 32%, respectively).
The comparison between the LFs of disk and inner halo GCs is also worth more attention. Again, we naively expected that destruction mechanisms would be more effective for disk clusters than for the inner halo ones. In this case, the LF for inner halo clusters should have a fraction of low-mass clusters intermediate between those observed in the outer halo and in the disk. However, while only 19% (4%) of the inner halo GCs have MV>-7 (MV>-6), this percentage is 41% (15%) for disk clusters. There are very few inner halo counterparts of the very frequent small disk clusters like M 71 and NGC 6397. Since such clusters are more easily destroyed in the disk than in the inner halo, this suggests a different original mass distribution between the disk and the inner halo (see also Fraix-Burnet et al. 2009, who attempted a multi-parametric classification of GCs, different from ours and leading to different conclusions about the properties of the different cluster populations, see the Appendix for further details).
All this suggests that the main difference between disk, inner, and outer halo clusters might be related to their formation (absence of young, small clusters in the inner halo) more than to the destruction efficiency, which is however very important for small clusters. This goes against a diffuse opinion, i.e., that we are now seeing only those GCs that occupied the survival zone of parameters; however, the notion that GCs can be formed only in a limited range of parameters is not new, as seen in Caputo & Castellani (1984).
It is also interesting to note that the luminosity function of the outer halo GCs is similar to that of GCs in dSphs (see Fig. 4): a Kolmogorov-Smirnov test gives a chance (73%) that they were drawn from the same parent population. This might depend on the fact that clusters in the outer halo and dSph shared similar environments at birth.
Disk and halo GCs also differ in other important
characteristics. Obviously,
the inner halo/outer halo GCs are on average more metal poor than
the disk ones (see Appendix). Furthermore, they seem to obey different
age metallicity relations: metallicity increased slower in the inner
halo than in the disk, and even slower in the outer halo, see
Fig. 5.
The age estimates were obtained as described in the Appendix.
Practically all disk/bulge GCs with [Fe/H]<-1 are very old,
while most of the inner halo GCs of intermediate metallicity (
)
have relative ages in the range 0.8-0.9; i.e.,
they are about 2 Gyr younger than disk GCs with the same
metallicity. If the
age/metallicity calibration is correct, after 2 Gyr from
the Big Bang, the central region of the Milky Way was enriched to
(and [
/H]
), while the
inner halo metallicity was still
very low
.
![]() |
Figure 5: Age-metallicity relation for different groups of GCs: outer halo clusters (green pentagons), inner halo clusters (blue circles), disk/bulge clusters (red squares). Magenta circles are GCs associated to dSphs. Different symbol sizes are used for clusters of different luminosity. |
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![]() |
Figure 6:
Relation between age and excess of |
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Finally, disk and inner halo GCs may differ in their element-to-element
abundance ratios, as suggested by the analysis by Lee & Carney (2002).
In part, this can be attributed to an age effect (see Fig. 6);
however, age cannot be the only explanation. This is shown by the close
comparison between M 4 and M 5 (NGC 6121 and
NGC 5904), performed by Ivans et al. (2001), which is
fully confirmed by our analysis (Carretta et al. 2009b). These
GCs are both inner-halo clusters according to our classification,
although M 5 has much more extreme kinematics, and it is also
likely younger by more than 1 Gyr. M 5 has a smaller
excess of -elements
and also seems to be deficient in nuclei produced by s-process
nucleosynthesys (Ivans et al. 2001; Yong
et al. 2008).
If confirmed, these two facts might at first look contradictory, since
a lower excess of
-elements
is usually attributed to a prolonged star formation, allowing
significant contribution by type Ia SNe. However, such a long phase of
star formation should also allow the contribution by the intermediate
and low-mass AGB stars, which efficiently produce s-elements.
In the next sections, we re-examine this point using our extensive
database and find a solution to this conundrum.
3.4 Cluster parameters considered in the analysis
Our choice was driven by the aim of sampling the full parameter space of GCs and to derive relations between the properties of different stellar generations in GCs and global parameters. Table 1 lists the 19 GCs in our programme set and gives structural and orbital parameters taken from literature. We considered the following parameters, mostly from Harris (1996):
- the apparent visual distance modulus, (m-M)V;
- the reddening, E(B-V);
- the Galactocentric distance,
;
- the total absolute visual magnitude, MV;
- the HB ratio, HBR, that is the fraction of blue and red HB stars over the total, as (B-R)/(B+V+R);
- the metallicity, [Fe/H] from our Paper VIII;
- the cluster ellipticity, ell;
- the concentration, c;
- the tidal radius,
(in pc, from Mackey & van den Bergh 2005);
- the half light radius,
(in pc, from Mackey & van den Bergh 2005).
- the total energy of orbit,
;
- the period of the Galactic orbit, P;
- the apogalactic distance,
;
- the perigalactic distance,
;
- the maximum distance from the plan,
;
- the eccentricity of the orbit, ecc;
- the inclination angle of the orbit,
;
- the rotational velocity,
.
Table 1: Properties of the 19 GCs in our sample.
Table 2: Quantities for the same GCs, derived by our works.
In Table 2 we report a few of the parameters derived by our works, related to the chemistry of first and second generation stars in GCs and their link with primordial abundances existing at the epoch of their formation. Other parameters derived, but not listed, in Papers VII and VIII are also given in this table.
Among these, we considered parameters related to the chemistry of first generation stars:
- the maximum O abundance, [O/Fe]
;
- the minimum Na abundance, [Na/Fe]
;
- the maximum Mg abundance, [Mg/Fe]
;
- the minimum Al abundance, [Al/Fe]
;
- the minimum Si abundance, [Si/Fe]
;
- the total Mg+Al+Si content, where the average is done in number, not in logarithm, [(Mg+Al+Si)/Fe];
- the overabundance of
-elements, [
/Fe], as given by the average of [Mg/Fe]
, [Si/Fe]
, and [Ca/Fe] (see Sect. 4.2.1 for an explanation of the choice).




![[*]](/icons/foot_motif.png)
Parameters related to the internal chemical evolution within the clusters are
- the minimum O abundance, [O/Fe]
;
- the maximum Na abundance, [Na/Fe]
;
- the minimum Mg abundance, [Mg/Fe]
;
- the maximum Al abundance, [Al/Fe]
;
- the maximum Si abundance, [Si/Fe]
;
- the relative fraction of stars in primordial (P), intermediate (I), and extreme (E) groups;
- the interquartile range of the [O/Na] ratio, IQR[O/Na].
Finally, to explore the connection between chemical patterns
of light elements, He abundances, and HB morphology we considered the
maximum temperature
reached on the blue tail of the HB (taken by Recio-Blanco
et al. 2006
or computed by us for programme clusters not listed in that study).
4 First generation stars, primordial abundances, and scenarios for cluster formation
The chemical pattern in first-generation GC stars is strictly related to the pre-enrichment established in the precursors of GCs, an issue for which we only have, at the very best, indirect evidence. In this section we discuss what evidence can be obtained from our data on the scenario of formation of GCs.
4.1 The masses of proto-GCs and the relation between the primordial population of GCs and the field
The scenario we are devising assumes that practically all GCs started their evolution as large cosmological fragments. To put cluster formation in a broader context, we try to establish the order of magnitude of the mass involved in cluster formation and discuss the possible link between GCs and field stars. Using different lines of thought, several authors (Larson 1987; Suntzeff & Kraft 1996; Decressin et al. 2008; D'Ercole et al. 2008) have suggested that present-day GCs are only a fraction (likely small) of the original structures where they originated. Large amounts of mass should be lost by proto-clusters during the early phases of formation (a few 107 yr), mainly for two reasons. First, the efficiency of transformation of gas into stars is unlikely to be larger than 50%, and it is more likely between 20 to 40% (Parmentier et al. 2008). The interaction with the high-velocity winds from massive stars and by their SN explosions expels the residual gas from the cluster and ram pressure probably contributes to the loss. Second, massive stars lose a large fraction of their mass before they become collapsed remnants. Several tens of per cent of the initial mass of the cluster may be lost by these stars, depending on the stellar initial mass function (IMF).
Owing to this huge mass loss, the clusters experience a violent relaxation (Lynden-Bell 1967), with a considerable expansion - beyond the tidal radius - and ensuing loss of stars. As shown by Baumgardt et al. (2008), the gas loss may destroy as much as 95% of the clusters, and this is a basic difficulty in forming bound star clusters. Only clusters with very high mass and initial concentration may survive. Clusters with a relatively flat stellar mass spectrum would be disrupted by this mass loss (Chernoff & Weinberg 1990). A bell-shaped cluster mass function, not too dissimilar to the observed one, can be reproduced by a proper tuning of parameters (efficiency of star formation, initial central concentration, original mass distribution, initial stellar mass function: see e.g., Parmentier & Gilmore 2007; Kroupa & Boily 2002). However, given the uncertainties existing in these parameters, the exact fraction of primordial mass lost by the proto-GCs is not determined well.
On the other hand, it is currently fully assessed that the second-generation stars (that presently make up some 2/3 of the stars of a typical GC, see Paper VII) should have formed from the ejecta of only a fraction of the first-generation stars, that actually coincide with the primordial component in GCs (Prantzos & Charbonnel 2006). To explain the present GC mass, we should then assume: (i) that the clusters originally had many more stars in the primordial component than we currently observe; and ii) that they selectively lost most of their primordial population, while retaining most of the second-generation stars. D'Ercole et al. (2008) presented a viable hydrodynamical scenario that meets both these requirements. In this scenario, a cooling flow channels the material, ejected as low-velocity winds from massive AGB stars of the first-generation, to the centre of the potential well. The first-generation stars were at the epoch expanding due to the violent relaxation caused by the mechanisms cited above. Given their very different kinematics, first and second generation stars are lost by the cluster at very different rates (at least in the early phases), leaving a kinematically cool, compact cluster dominated by second-generation stars. This selective star loss may continue until two-body relaxation redistributes energy among stars. This takes a few relaxation times, that is, some 108-109 yr in typical GCs. After that, the effect could even be reversed if He-rich second-generation stars are less massive than first-generation ones (see D'Ercole et al. 2008; Decressin et al. 2008).
We may roughly estimate the initial mass of the primordial population needed to provide enough mass for the second generation by the following procedure:
- (i)
- We assume an IMF for both the first and second generations.
For simplicity; we assumed that the two populations have the same IMF.
We considered both power-law (like the Salpeter 1955 one) and the
Miller & Scalo (1979,
MS) IMF's. As often done, in the first case we integrated the IMF over
the range 0.2-50
, while in the second case we considered the range 0.1-100
.
- (ii)
- We also assumed an initial-final mass relation. In
practice, we assumed a linear relation, with final mass ranging from
0.54 to 1.24
, over the mass range from 0.9 to 8
(Ferrario et al. 2005). A second linear relation with final mass ranging from 1.4 to 5
was assumed for the mass range from 8 to 100
. The latter relation is not critical, since massive stars lose most of their mass.
- (iii)
- We assume that the second generation is made of the ejecta
of stars in the mass range between
and
. The adopted ranges were 4-8
for the massive AGB scenario and 12-50
for the FRMS. Second-generation stars likely result from a dilution of these ejecta with some material with the original cluster composition. A typical value for this dilution is that half of the material from which second-generation stars formed was polluted, and half had the original composition. The origin of this diluting material is likely to be pristine gas (not included into primordial stars, see Prantzos & Charbonnel 2006).
- (iv)
- We finally assume that none of the second generation stars is lost, while a large fraction of the primordial generation stars evaporate from the clusters. Of course, this is a schematic representation.
Table 3: Original/final mass of GCs required to produce the observed ratios between number of stars in first and second generations.
We conclude that, during the early epochs of dynamical
evolution, a proto-GC should have lost 90% of its primordial stellar population. A GC of
a few 107 yrs old should have then
appeared as a compact cluster immersed in a much larger loose
association of stars and an even more extended expanding cloud of gas.
Objects with these characteristics have been observed in galaxies with
very active star formation (see e.g. Vinko et al. 2009).
![]() |
Figure 7:
Comparison of [Na/Fe] values between field and GC stars as a
function of metallicity. In both panels the filled red circles are for
our sample of GCs, indicating [Na/Fe]
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Observational constraints to the ratio between first and second
generation stars may be obtained by comparing the number of stars
within the GCs with that of the related field population. To have an
estimate of the amount of mass lost by GCs during their evolution, we
may use the peculiar composition of GC stars, namely the large
excesses of Na that are often observed in GC stars, to trace these lost
stars in
the field. Figure 7
shows the run of [Na/Fe] among field stars,
comparing it to the extremes of the distributions for GC stars. To this
purpose,
we collected data for field stars from three different sources: Gratton
et al. (2003a);
Venn et al. (2004),
and Fulbright et al. (2007).
Besides the
abundance ratios, they indicated the population of each star on the
basis of
the kinematics. Gratton et al. divided stars into
``accretion'' and
``dissipation'', while Venn et al. used the more common
separation between halo and disk. The correspondence accretion/halo and
dissipation/disk is largely
true for the stars in common. Finally, all stars from Fulbright
et al. are bulge ones. In Fig. 7 we plot field
stars -taken only once if they are present in more than one source-
between metallicity -2.5 (to fit the lower limit of the GC metallicity
range) and -1 (to avoid thin disk stars). In the
upper panel we also plot [Na/Fe]
for our GCs, i.e. the
original,
first generation value that sits in the middle of the field stars
distribution.
In the lower panel we plot instead [Na/Fe]
for our GCs, i.e. the
second generation value, well above the bulk of field stars.
Examining this plot, we find that, while most of the field
stars roughly have
[Na/Fe],
there are a few objects with rather large excess of Na,
comparable to what is observed in second-generation stars of GCs. In
the sample
of 144 field stars with [Fe/H] <-1, there are
six stars with [Na/Fe] >0.3;
for comparison, 50% (735 over 1483) of the stars in our survey
of GC stars
have these large Na excesses
.
However, only two of these field stars are likely to be
second-generation stars evaporated from GCs: HD74000 and
HIP37335 (=G112-36). These two stars are also moderately
depleted in Li (Hosford et al. 2009;
Pilachowski et al. 1993), as
expected for second generation stars in GCs (see
Pasquini et al. 2005).
The remaining four Na-rich stars are extremely metal-poor stars
residing in binary systems, and the Na excess may be attributed
to mass transfer. Two of them (CS22898027 and
CS22947187) are C-rich stars. G246-38 is extremely
Li-poor (Boesgaard et al. 2005).
Finally, also HD178443 is a giant in a binary system. While
the statistics are poor, we may conclude that some 1.4% of the
field metal-poor stars are likely Na-rich stars evaporated from GCs.
Since these
are half of the GC stars, we may conclude that stars evaporated from
GCs make up
2.8% of the metal-poor component of the Milky Way. We may compare this
value
with the current fraction of stars in GCs, which is 1.2% using the
Juric et al. (2008)
in situ star counts and 5% using the Morrison (1993) ones. We
neglect the impact of
selective loss of low-mass stars; this is not too bad an approximation
because
spectroscopic data are only available for stars with typically the
current TO
mass. We conclude that the GCs should have made up some 4% of the
original
mass of metal-poor stars, if Juric et al. star counts are
used, and as much as
7.8% adopting the Morrison ones. These values may still be
underestimates. In fact, if the cooling flow scenario is correct,
second-generation stars were originally a very kinematically cold
population,
which means that they evaporated from the GCs only after dynamical
relaxation led to energy equipartition,
1 Gyr after the GC formation, i.e., much
later
than the formation phase. Then, there should be many more primordial
stars of
GCs now in the field, lost during the early phases. As discussed above,
these
values should be increased by an order of magnitude.
The conclusion is that precursors of GCs probably had a
baryonic mass 20 times
higher than the current mass (if both the efficiency of star
formation and the huge star loss factors are taken into account). If
they also contained dark matter, they were likely to be two orders of
magnitudes greater than they currently are, with total masses up to a
few
,
which is the size of dSph's (see also Bekki et al. 2007).
We propose that the fraction of the primordial population lost by GCs is a major building block of the halo, although we do not exclude other minor contributors. This is supported by many other arguments, including their total mass, the metallicity distribution, and the location within the Milky Way, all of which are discussed in a separate paper (Gratton et al. 2010). GCs might have played a similar role in the formation of the metal-poor component of the thick disk ([Fe/H]<-1), while the specific frequency is much lower (by an order of magnitude) for the metal-rich component ([Fe/H]>-1), and they are obviously absent from the thin disk.
The formation phase of GCs may be very important for understanding star formation in the early phases of the Milky Way (and probably of other galaxies). Any information on the composition of the primordial population would help to shed light on the formation mechanism of GCs. We now examine what evidence can be obtained from our data.
4.2 The chemical evidence: the primordial abundance ratios and the scenario for GC formation
![]() |
Figure 8:
[O/Fe]
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-elements
![]() |
Figure 9: Relation of the ratio [(Mg+Al+Si)/Fe] as a function of several orbital parameters: a) total energy of the orbit; b) orbital period; c) apogalatic distance, and d) maximum distance above the Galactic plane. Also indicated are the Spearman and Pearson correlation coefficients. |
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As demonstrated by several authors (Gratton et al. 1996, 2000, 2003a, 2003b;
Fuhrmann 1998,
2004),
the [/Fe] ratio
is a good population
discriminator. Nissen & Schuster (1997) found that
halo subdwarfs have an
[
/Fe] ratio
on average lower and with more scatter than what is typical of the
thick disk population at the same metallicity, a result later confirmed
by several other investigations (see e.g. Gratton et al. 2003b).
While several of the
-elements
are involved in the nuclear cycles related to high-temperature
H-burning, there are many possible indicators of the primordial [
/Fe] ratio
that we can obtain from our data. A short list includes the maximum O
and Mg abundances ([O/Fe]
and [Mg/Fe]
), the
minimum Si abundance ([Si/Fe]
), the total Mg+Al+Si content
[(Mg+Al+Si)/Fe] (see Sect. 3.4
and footnote there), and the average of [Mg/Fe]
,
[Si/Fe]
,
and the typical
-element
Ca. All these indicators give concordant results. In the following, we
mainly use the total [(Mg+Al+Si)/Fe] content.
In Fig. 8
we plotted the run of the original abundance
ratio of various -elements
with [Fe/H]: [O/Fe]
,
[Mg/Fe]
,
and [Si/Fe]
.
In the same figure, we also
plotted the distribution of field stars from Fulbright (2000),
Gratton et al.
(2003a),
Reddy et al. (2006),
Venn et al. (2004)
and Fulbright et al. (2003, 2006). GCs
lie close to the location of the field stars, especially considering
possible offsets among different analyses.
We do not have any a priori idea of what we should expect for the exact form of most of the relations between the new parameters we are introducing and global cluster parameters, so we adopt the simpler, linear relation. These relations are evaluated using the Pearson coefficient for linear regressions and the Spearman coefficient of rank correlation, which can be used to characterise the strength and direction of a relationship of two given random variables (e.g. Press et al. 1992).
Tight relations are obtained between the overabundance of -elements
(represented e.g., by Mg+Al+Si) and orbital parameters (confirming
earlier
findings by Lee & Carney 2002).
In Fig. 9
we show the relations of the ratio [(Mg+Al+Si)/Fe] with total energy of
the orbit, orbital period, apogalactic distance, and the maximum
distance above the Galactic
plane. The correlation coefficients, represented by the Spearman and
Pearson
coefficients (
and
),
are high, and they would increase further by excluding
NGC 5904 (M 5), the cluster affected by the largest
uncertainties in
the orbit.
Similar trends are seen when plotting the overabundance of Ca
or the average between Ca and Ti I. It
seems that clusters populating large-sized, more
eccentric orbits with large apogalacticon distances (i.e., mostly the
inner
halo GCs, in our classification) also have a proclivity
toward a lower abundance of elements produced in -capture processes. We
consider these results as an indication that the initial position
affected the chemical enrichment of GCs
Is there a risk of a bias introducing spurious trends among
orbital and chemical
parameters? The correlation existing in our sample between absolute
magnitude
MV and
distance (Sect. 3.3)
is not a source of concern. We find that
the total Mg+Al+Si sum is anticorrelated (with moderate significance,
between 90 and 95%) with MV:
the [(Mg+Al+Si)/Fe] ratio is lower in more massive
clusters. However, we found that there is a slight trend for orbital
parameters to be correlated
with the cluster mass (luminosity) for our
distance-limited sample. Although scarcely significant from a
statistical point
of view, this trend is also present in the control sample of GCs with
kpc and known
orbital parameters. Thus, when taken together,
these opposite trends should combine in such a way as to erase any
dependence
of the total Mg+Al+Si sum on orbital parameters, whereas we find good
and
significant relations. As a result, these trends are probably
significant and
should be considered when discussing scenarios for cluster formation.
We conclude that disk and halo GCs share the same [/Fe] ratio
of thick disk and halo stars respectively. As observed in the field,
halo GCs
have a smaller excess of
-elements
on average, and a scatter larger
than observed for the (thick) disk populations.
From the [
/Fe]
ratios collected in the Appendix, we
find that below a metallicity of [Fe/H]=-1, the average values are
dex
(
dex from
15 GCs) for disk/bulge clusters and
dex
(
dex from
14 GCs) for inner halo ones.
The explanation that we propose here is not the classical one
requiring the
contribution of SNe Ia to raise the iron content, hence lower the [/Fe]
ratio. We propose the possibility that
the contribution of core-collapse SNe to metal enrichment is weighted
towards
higher-mass SNe for the precursors of lower-mass clusters. The most
kinematically energetic products (rich in particular in
-elements)
might have been lost in more massive GCs, due to a powerful wind.
Evidence of such a
wind is found around very massive and young star clusters, such as the
one
observed in NGC 6946 (Sanchez Gil et al. 2009). In the
Milky Way, these massive
GCs are mainly found in the inner halo. This explanation is
substantiated by the comparison of M 5 and M 4,
providing a solution to the conundrum described in Sect. 3.3.
4.2.2 Aluminium
In Paper VIII we presented the run of [Al/Fe]
with [Fe/H] in GCs.
[Al/Fe]
is expected to represent the
Al abundance of the
primordial population. We underlined there the large scatter observed
in this
diagram, which exceeds the observational uncertainties by far. We also
noticed
that there is a group of clusters, mainly belonging to the inner halo,
characterised by very low values of [Al/Fe]
.
Similar results were
previously obtained for individual clusters (see e.g. Melendez
& Cohen 2009),
but our extensive survey shows that this is a widespread property of
GCs.
However, Fe is not the best reference element for Al, because
it has a very
different nucleosynthesis. Cleaner insight can be obtained considering
Mg as
reference. Mg and Al may both be produced by massive stars exploding as
core
collapse SNe. While Mg is an -rich element whose production
is primary,
Al requires the existence of free neutrons for its synthesis, and
therefore its
production is sensitive to the initial metallicity (Arnett &
Truran 1969;
Truran & Arnett 1971;
Woosley & Weaver 1995).
The
exact dependence of the ratio of Al to Mg as a function of overall
metallicity
has never been defined satisfactorily by theory, but it should show
some sort of secondary behaviour with respect to Mg.
![]() |
Figure 10:
Run of the [Al/Mg] ratio as a function of the [Mg/H] ratio in field
stars (grey-tone open circles), GCs in our sample (red and blue
filled circles and squares, respectively) and stars in dSphs (green
triangles,
the open ones are upper limits in Al, see text for references). The
[Al/Mg]
ratio in our sample refers to primordial abundances, namely [Al/Fe]
|
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Figure 10
shows the run of [Al
/Mg
]
(that is,
the ratio for the primordial population) with [Mg
/H] for our
programme cluster. We also plot the run of [Al/Mg] with [Mg/H] for
metal-poor
field stars in the Milky Way (Fulbright et al. 2007; Reddy
et al. 2003; Gehren
et al. 2006; Jonsell et al. 2005; Fulbright
2000),
as well as for stars in dSph
galaxies (Koch et al. 2008;
Geisler et al. 2004;
Shetrone et al. 2001,
2003;
Sbordone et al. 2004).
As shown by Gehren et al. (2006), the local subdwarfs
have markedly different [Al/Mg], depending on their kinematics: halo
subdwarfs
have much lower [Al/Mg] than thick disk ones, so much so that Gehren
et al.
propose using this ratio as a population diagnostics. The locus
occupied by
primordial populations in most GCs is clearly distinct from the one for
the
thick disk subdwarfs and close to the one defined by halo subdwarfs.
Several
clusters, including the most massive ones, have very low
primordial Al
abundances and lie close to the line of secondary production:
[Al/Mg] = [Mg/H].
The exception consists in a few small clusters (NGC 288,
NGC 6121, NGC 6171, NGC 6838), which have
large primordial Al abundances. A multivariate analysis,
using [Mg
/H] and MV
as independent variables, and [Al
/Mg
]
as dependent one, yields
![]() |
= | ![]() |
|
![]() |
![]() |
(1) |
with a highly significant linear correlation coefficient of r=0.80 (16 clusters, 13 degrees of freedom). This behaviour is different from what is observed in dSphs, which are typically characterised by rather large Al abundances.
4.2.3 A scenario for the formation of GCs
How can we explain this behaviour? First, the primary-like
run of Mg and
Al observed in disk subdwarfs requires that most of the Al in these
stars be
produced in a different site from massive stars (where the production
is
secondary). Second, we observed very high Al
abundances within second generation stars in GCs (Paper VIII
and Table 2)
even exceeding the values observed in disk subdwarfs and similar to
those observed in dSph's stars.
This suggests an obvious astrophysical site where these large amounts
of Al can be produced: the same stars responsible for the Mg-Al
anticorrelation (either fast-rotating massive stars - FRMS - or
intermediate-mass AGB stars). In this case, the very low Al abundances,
characteristic of the primordial population
of massive GCs, may be explained if the rise in metal content
in the
environment where these stars formed was so fast that no star with
intermediate
metallicity could form. On the other hand, pre-enrichment
should have had to
be more gradual for low-mass clusters, with different generations
making little
difference in the Mg content, and an efficient re-processing of Mg into
Al in
the next generation. A similar conclusion was drawn for the case of
M 71
(NGC 6838) by Melendez & Cohen (2009).
However, we find that this is a general
feature of GCs, even of clusters reputed to be younger than the disk
ones. This
is unlikely to be a coincidence, but is instead more probably related
to the
typical sequence of events that led to cluster formation.
This consideration suggests a (still qualitative) sketch for the formation of typical massive GCs, which is a more elaborated and updated version of what was proposed more than thirty years ago by Searle & Zinn (1978) and later elaborated on by many other authors (see e.g. Böker 2008, and references therein).
- 1.
- Consider a cosmological fragment/satellite of
i.e. the same range of masses of dSph's, but which is near the Milky Way (
kpc) at a very early epoch (<2 Gyr from the Big Bang). In a cold dark matter (CDM) scenario, we expect many such satellites to have existed (see e.g. Bromm & Clarke 2002; De Lucia & Helmi 2008). At this very early epoch, this satellite is still made of dark matter and gas (
), with negligible/small stellar contribution and metal pre-enrichment, depending on its age, i.e., on the time allowed for an isolated evolution before the phases described in the following.
- 2.
- Likely due to its motion, which brings the cluster in
proximity of the
denser central region of the Milky Way, this fragment has a strong
interaction,
possibly with the same early disk of the Milky Way or with another
substructure
(Bekki 2004).
This strong interaction triggers an early star formation
(Whitmore & Schweizer 1995).
On a short timescale (a few million years)
of gas are transformed into stars. The most massive of these stars explode as SNe after
107 yr. Hereinafter, we call this population precursor, because while needed to form the GC itself, it is unlikely that we will find any representative of this population within the present GC (see below).
- 3.
- The precursor core-collapse SNe have two relevant effects:
i) they enrich
the remaining part of the fragment/satellite of metals, raising its
metallicity
to the value currently observed in the GC
; and ii) efficiently trigger star formation in the remaining part of the cloud, before the intermediate mass stars can efficiently contribute to nucleosynthesis. This second episode (or phase, since it is not clear that there should not be a continuum in star formation) forms a few
of stars in a large association. These associations have mass and size (
100 pc) comparable to the knots commonly observed in luminous and ultra-luminous infrared galaxies (see e.g. Rodriguez Zaurin et al. 2007).
- 4.
- The strong wind from massive stars and core collapse SNe of
this huge
association disperses the remaining primordial gas on a timescale of
107 yr (see the case of the super star cluster in NGC 6946, Sanchez Gil et al. 2009).
- 5.
- While the large association is expanding, the low-velocity
winds from FRMS
or, perhaps more likely
, from the more massive intermediate-mass stars feed a cooling flow, which forms a kinematically cool population at the centre of the association (D'Ercole et al. 2008). Possible examples of objects in this phase are Sandage-96 in NGC 2403 (Vinko et al. 2009) or the super star cluster in NGC 6946 (Hodge 1967; Larsen & Richtler 1999; Larsen et al. 2006). A fraction of the primordial population stars (but very few precursors if any, since they are much rarer and possibly were at some distance from the newly forming cluster) remains trapped into the very compact central cluster formed by this second generation stars. This is the GC that may survive over a Hubble time, depending on its long-scale dynamical evolution and that we observe at present.
- 6.
- Core-collapse SNe from this second generation sweep the
remaining gas
within the cluster, terminating this last episode of star formation.
This
occurs earlier in more massive clusters: these clusters will then be
enriched
by stars over a restricted range of mass (only the most massive among
the potential polluters), leading to very large He abundances. As a
result, there should be correlations between He
enrichment, cluster mass, and fraction of primordial stars. However,
this may occur naturally only in a cooling flow scenario, where second
generation star formation is well separated from the evolution of
individual stars. In the original FRMS scenario of Decressin
et al. (2008),
second generation stars form within the individual equatorial
disks around the stars, as a consequence of the large mass loss rate
and fast rotation. Within this scenario, it is difficult (although not
strictly
impossible) to link properties of individual stars to global cluster
properties.
Table 4: Pearson's correlation coefficients and level of significance for relations in P, I, and E stars.
- 7.
- At some point during these processes or just after, the DM halo is stripped anyway from the GC and merges with the general DM halo (see e.g. Saitoh et al. 2006; Maschenko & Sills 2005). It is not unlikely that the loss of the DM halo stems from the same interaction which causes the formation of the GC. The cluster has now acquired the typical dynamical characteristics that we observe at present, and hereinafter has essentially a passive evolution (see e.g. Ashman & Zepf 1992).
As noticed by Zinn (1985),
within this scheme the different chemical histories
of disk and halo GCs may easily explain the most obvious
characteristics of
GCs, systematically observed in virtually all GC systems, such as:
i) the
bimodal colour and metallicity distribution, because blue clusters are
essentially self-enriched, while red clusters form from pre-enriched
material
in the early phases of dissipational collapses (note, however, that
there
should be a few blue and metal-poor disk clusters); ii) the
absence of
discernible metallicity trends with
for halo GCs (see Searle & Zinn 1978); and
iii) the presence of relatively young GCs in the halo (Zinn 1985).
This scenario also unifies the view of GCs and dSphs. In fact,
according to
this scheme, both GCs and dSphs start as DM-dominated cosmological
structures with masses in the range
.
The main difference is their
location with respect to the Galaxy. GCs formed from DM haloes closer
to the
centre of the Galaxy or to other structures (even NGC 2419,
the farthest known GC). They had only a limited significant,
independent chemical evolution prior
to their interaction with the Galaxy, which occurred quite early, when
the
structures were still gas-rich. The age-metallicity relation for halo
GCs (see
Fig. 5)
suggests that pre-cluster clouds that had more time to
evolve actually produced part of their metals during this pre-cluster
phase.
When they interacted with other structures or with the main Galaxy body
itself,
their independent evolution was interrupted by the sequence of phases
we
described above (see Melendez & Cohen 2009, for a
similar view).
On the other hand, dSphs formed much farther, at typical distances of several hundred kpc. They could have a long independent evolution before interaction (if any) with the Milky Way. Their evolution is determined essentially by their initial mass, so that they obey mass-luminosity and mass-metallicity relations. If any interaction with the Milky Way has occurred (as is the case for Sagittarius), this happened once the dSph had become gas poor, and this did not lead to any further GC formation (although more massive dSphs could include a few already formed GCs).
As noticed by the referee, the scenario we considered implies that significant GC formation may still occur in gas-rich environments insofar as the high pressure needed is available, e.g. owing to galaxy-to-galaxy interaction. This is possibly the case of the Antennae (Whitmore & Schweizer 1995) or even of the Magellanic Clouds, where there is evidence of formation of six young clusters in the Magellanic Bridge (Irwin et al. 1985).
5 The second phase of cluster self-enrichment
In our scenario, the early phases of the evolution of the structures that will ultimately form GCs are linked to the composition of the primordial population, and the late phases determine the cluster self-enrichment processes. We expect that such processes are linked to some global characteristic of GCs. In Papers VII and VIII we showed that very important rôles are played by mass and metallicity of the cluster. In this Section, we revisit this issue, considering many other parameters; a more global approach will be applied in next Section.
5.1 The chemistry of second generation stars
The chemical properties of second-generation stars in GCs were
discussed
quite extensively in Papers VII and VIII. They may be
described by the fraction of the intermediate I and of the
extreme E components, and by the extreme values associated to the
polluted stars using a dilution model, namely [O/Fe]
,
[Na/Fe]
,
[Mg/Fe]
,
[Al/Fe]
.
In Paper
VIII we demonstrated that the ratio [Si/Fe]
is an additional marker of
second-generation stars, because of the
leakage of the Mg-Al cycle which produces 28Si
at temperatures in excess of about 65 million K
(Carretta et al. 2009b; Arnould et al. 1999; Yong
et al. 2005).
In Table 4
we list Pearson's correlation coefficients, the number
of degrees of freedom, and the statistical significance level of the
correlations involving the extremes of the abundance distributions and
the
fraction of P, I, and E stars.
In addition, we also considered the interquartile
of the Na-O distribution IQR[O/Na].
We find several correlations with a high level of
statistical significance (better than 99%), as can be seen from the
table. The
most interesting correlations are shown in Figs. 11 to 16.
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Figure 11: Left: fraction of stars in the primordial P ( upper panel), intermediate I ( middle panel) and extreme E ( lower panel, with a different scale on the y-axis) components of GCs as a function of the IQR[O/Na]. Right: the same, as a function of [(Mg+Al+Si)/Fe]. The Pearson and the Spearman rank correlation coefficients are shown in the box, here and in the next figures. |
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Figure 12: Extension of the Na-O anticorrelation, measured by the IQR[O/Na], as a function of the total sum of Mg+Al+Si atoms for our sample of clusters. |
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From Table 4 and the lefthand panels in Fig. 11, we see that there is a tight correlation between the E fraction and the extension of the Na-O anticorrelation, IQR[O/Na]. This does not come as a surprise, since IQR[O/Na] is driven by the stars with extreme chemical modifications. The I fraction, which is the dominant group in all GCs, is anticorrelated with IQR[O/Na], while the primordial P component is not related to the extension of the Na-O anticorrelation.
The run of the P, I, and E fractions as a function of the total Mg+Al+Si sum is illustrated in the lefthand panels of Fig. 11. The fraction of stars in the P population is higher when this total sum is lower. Even tighter relations exist for the I and E components. The sign of these relations is opposite to those with IQR[O/Na]. The combination of the left and right panels in Fig. 11 results in the statistically significant anticorrelation between IQR[O/Na] and total Mg+Al+Si sum shown in Fig. 12: clusters where the Na-O anticorrelation is more extended have a lower value of the total Mg+Al+Si sum. This result is confirmed by the relations existing between the P, I, and E fractions and [Ca/Fe] (right panels in Fig. 13). However, we also notice that these findings are strongly influenced by the two bulge clusters NGC 6388 and NGC 6441.
The E population is the only one showing a significant
correlation with [Fe/H].
However, this is not surprising, because we found (Carretta
et al. 2009a) that
O,
whose value is related to the presence of the E component, is well
represented by a linear combination of MV
and [Fe/H]. We interpreted this
result as a proof that the mass of the average polluters varies
regularly as a
function both of cluster mass and metal abundance.
![]() |
Figure 13:
Left: fraction of stars of the P,
I, and E components
(upper, middle, and lower panels, respectively) as a
function of |
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![]() |
Figure 14: Left panels: the fraction of stars in the P, I, and E components of second-generation stars as a function of the total absolute magnitude (hence, mass) of clusters. Right: the same, as a function of relative age. |
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![]() |
Figure 15: Interquartile range of the [O/Na] ratio as a function of the maximum temperature reached on the HB (taken from Recio-Blanco et al. (2006) or derived here). The line connects the value for M 15 based on our data and the one derived from the literature (open green triangle, see text). |
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![]() |
Figure 16: The extension of the Na-O anticorrelation (measured using IQR[O/Na]) as a function of the clusters' absolute magnitude MV from Harris (1996). The Pearson correlation coefficient is given and five GCs discussed in the text are indicated. |
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In Fig. 14 (right panels), the fractions of first and second generation stars are shown as a function of the relative GC ages. These relations are statistically significant, because the P and E components are anticorrelated and the I fraction correlated with age. This result might be an artefact owing to the relations with MV (left panels of the same figure). As seen in Sect. 3, the more massive clusters in our sample are those in the inner halo, where the younger clusters reside. However, we cannot exclude other factors; for instance, the presence of a population with enhanced He might alter the derivation of ages, as discussed in detail in Gratton et al. (2010).
In summary, we find the following:
- (i)
- A P component of first generation stars is present in each
GC. Its
incidence does not depend on the cluster metallicity, being
approximatively
constant (at a level of about one third of the cluster stars,
Paper VII) in each
GC. This component does not affect the extension of the Na-O
anticorrelation,
but it is less conspicuous in GCs with higher abundances of
-elements.
- (ii)
- The bulk of second generation stars is composed of stars
with
moderate alterations in the light elements Na, O, Mg, Al participating
to
proton-capture reactions in H-burning at high temperature (see
Paper VII). This I component is lower in GCs with
longer Na-O anticorrelations, and this fraction is higher in GCs with
larger
-element ratio.
- (iii)
- The E component, with extreme changes in light element
abundances
with respect to first generation stars, is not present in all clusters
(Paper VII). It is anticorrelated to the complementary I
component and is the key
component driving the extension of the Na-O anticorrelation, showing a
very
tight and significant correlation with IQR[O/Na]. The E component
decreases with increasing overabundance of
-elements.
5.2 Extension of the Na-O anticorrelation and (blue) HB
We demonstrated in Carretta et al. (2007d) that
there is a tight
correlation between IQR[O/Na] (derived from part of our sample or from
the
literature) and the maximum temperature of HB stars,
(HB)
(Recio-Blanco et al. 2006).
To verify that this relation
also holds for the more extended sample of clusters considered here, we
complemented the values of
(HB)
obtained by
Recio-Blanco et al. with new ones. We employed good quality
CMDs (Bellazzini
et al. 2001
for NGC 288; Marino et al. 2008 for
NGC 6121; Rosenberg et al. 1999
for NGC 6254; Momany et al. 2003 for
NGC 6752; Vargas Alvarez & Sandquist 2007
for NGC 6809) with the same HB models (Cassisi et al.
1999) as
used by those
authors. Furthermore, we replaced the values of IQRs of Carretta
et al. (2007d)
that were derived from the limited samples of stars with UVES spectra
available
at the time, with new ones obtained from the full sample of stars with
Na and O
determinations from GIRAFFE and UVES in all the 19 GCs in our sample
(Table 2).
We fully confirm our previous findings, as seen in
Fig. 15
.
The position of M 15 (NGC 7078) in
Fig. 15
is somewhat uncertain.
The value from literature lies very well on the sequence defined by all
other
clusters, while the value we derive is more offset from the main trend.
Since
M 15 is among the most metal-poor GCs and our GIRAFFE
resolution is worse than
the one in Sneden et al. (1997), it is
possible that we missed some very
O-poor or Na-poor stars. However, the O abundance of two most O-poor
stars in
Sneden et al. is flagged as uncertain. With these caveats in
mind, we adopt
here the value of the IQR[O/Na] for M 15 derived in our
analysis for
homogeneity. The correlation is at any rate very tight: the Spearman
test returns coefficients rS
of 0.69 (with our value for M 15), 0.82 (with M 15
from literature), or 0.81 (without M 15). The probability of
getting such a tight
relation by chance is negligible, because the (one-tailed) t-test
returns values of ,
10-6,
or 4
10-6 in the three cases, respectively.
We confirm that this is a real, very strong relation: the first conclusion we can draw is that the same mechanism drives or affects the extent of the pollution on the RGB and the morphology of the bluest end of the HB. However, this can be only considered a second parameter, because the global distribution of stars on the HB [as indicated e.g., by the HB ratio HBR=(B-R)/(B+R+V) - see Harris 1996 and web updates] is not correlated with IQR[O/Na], i.e. with the extension of the Na-O anticorrelation, as already discussed by Carretta (2006) and Carretta et al. (2007d). The relation between the distribution of stars along the HB and the Na-O anticorrelation is discussed further in a separate paper (Gratton et al. 2010).
Finally, the relations of the three individual stellar
components P, I, Ewith
(HB),
shown in the right panels of Fig. 13, simply
reflect the correlations and anticorrelations of the latter with
IQR[O/Na].
5.3 Extension of the Na-O anticorrelation and total cluster mass
Possibly a major result of our analysis is the good correlation we found between the IQR[O/Na] and the present-day total mass of the GCs (using the absolute magnitude MV as a proxy for the mass), see Table 4 and Fig. 16. A high mass seems to be a prerequisite for an extended anticorrelation. This is not unexpected, because Recio-Blanco et al. (2006) have already found a good correlation between total mass and highest temperature on the HB, and in the previous section we found that the latter is strictly related to the extent of the Na-O anticorrelation.
The correlation found in Recio-Blanco et al. is also
a good test of the reliability of our sample against a possible bias
related to selection criteria.
We do not have values for IQR[O/Na] for all clusters in the Harris
catalogue;
however, our distance-limited sample of 19 GCs shows a correlation
between MV
and (HB),
with a Pearson correlation coefficient
rp
=-0.47, 17 degrees of freedom, significant at better than 95%
level of
confidence. The same correlation is present in all clusters in the
Harris
catalogue with available log T
(HB)
(
rp
=-0.43, 54 GCs) and for clusters in the control sample
restricted to distances less than 12.9 kpc from the Sun (
rp
=-0.52, 42 GCs), both significant to more than 99%.
Thus this correlation does not come from selection bias.
Moreover, since we included GCs with all morphologies of HB in our
sample, it is not biased against HB type or
(HB).
It follows that the correlation we found between IQR[O/Na] and MV
is real.
The explanation of this correlation is quite complex. On one
hand, it is
clear that only massive enough clusters can have a second generation.
However, i) (almost) all GCs are massive enough (while open
clusters are probably not, see Fig. 3); and
ii) IQR[O/Na] does not depend on the fraction of second
generation stars (that is on I+E,
or P=1 - (I+E)).
Rather, IQR[O/Na] is correlated with E, and anticorrelated
with I (see left panels of Fig. 11). This
indicates that what is related to MV
is the extreme of the anti-correlation, not its median value. This has
already been found in Papers VII and VIII, where we
showed that O
and Al
are strongly correlated with a
combination of MV
and [Fe/H]. In these papers we connected this to the
typical mass of the polluters: the higher this mass, the higher the
H-burning
temperature, the lower O
and the higher Al
.
As a result, available data indicate that the typical polluter's mass is related to MV (i.e., total cluster mass). To explain this relation, either the maximum or the minimum mass (or both) defining the range of polluters is changing. This might be understood quite easily in the case of AGB polluters. The maximum mass may be reduced if the cooling flow is delayed by the effect of adjacent regions where massive stars are still present, as expected e.g. from formation of clusters in a spiral arm. The minimum mass may be higher in more massive clusters: the higher the cluster mass, the faster the critical mass needed for second generation star formation is reached, before the earliest second-generation SNe explode, halting star formation. In the case of massive stars polluters, the arguments are more complex but similar. Only stars formed by the ejecta of the most massive stars may contribute if the cluster mass is very high, perhaps due to devastating effect of super-winds blowing in very massive clusters.
However, the scatter we observe in Fig. 16 suggests that
high mass
alone is not a sufficient condition. Clusters lying off the global
relation, at the left edge, namely NGC 288,
NGC 6218, (M 12), and NGC 6838
(M 71) might be reconciled with the bulk of other
clusters if we assume that they lost a higher-than-average fraction of
their
original mass. We already gave in Sect. 4.1 arguments
suggesting
that a noticeable fraction of the original mass of GCs is lost after
the
formation phase. We searched the literature for observational evidence.
De
Marchi et al. (2006)
argue for severe tidal stripping in NGC 6218, and they
estimate that the present mass of this cluster might even be only one
fifth of
the original one. The flat mass function of NGC 6218 is also
consistent with a
large fraction of stars lost by evaporation or tidal stripping. A tidal
tail is
also suspected to be associated to NGC 288 (Leon
et al. 2000),
although other
studies (Kiss et al. 2007)
find no extended extra-tidal structures. The most
intriguing evidence of high mass loss in these later phases is maybe
the one
for M 71. It comes from a totally independent line of thought.
With its total
absolute magnitude of MV=-5.6
(Harris 1996),
this cluster is the least
massive object in Fig. 16.
Elsner et al. (2008)
published a study based on Chandra X-ray
observations of M 71, where they find
that there is an excess of sources for the present cluster mass, with
respect
to the relation defined by 47 Tuc, M 4, and
NGC 6397. Another way to state the
problem is that to bring M 71 on the relation given by the
other
clusters one must assume that 50 to 70% of its original mass was lost
in the
past. Elsner et al. use scaled values of the mass
inside the half-mass radii and a relation by Kong et al. (2006) linking
to the cluster
absolute visual magnitude. Using the same relation, but assuming that
the
scaled mass of M 71 is 1 instead of 0.3, we get a value of MV=-7.2
which
would shift this cluster on the relation between IQR[O/Na] and MV.
On the other hand, even if accounting for less massive clusters were possible, some problems are also left at the high-mass end. A high mass is not always matched by a very extended Na-O anticorrelation. NGC 104 (47 Tuc) is a notable example, because this cluster simply does not show very O-poor stars and presents a short/normal Na-O anticorrelation even if it is a very massive object. Some other factors must be involved. We reconsider the case of 47 Tuc in Gratton et al. (2010).
6 The next level of the game and conclusions
In the previous sections, as well as in Papers VII and VIII, we have seen the key rôle of the main parameters affecting the formation and early evolution of GCs, namely: (i) the mass; (ii) the metallicity; and (iii) the Galactic population/region to whom they belong (inner/outer halo vs disk). These main parameters summarise the history of a GC well, in the context of the evolution of the Galaxy itself. The correlations with chemical properties suggest that both the initial conditions at cluster's birth and the subsequent evolution while orbiting the Galaxy determine the resulting ratio of first and second generation stars and several other properties.
The next step is to systematically explore all the possible
relations
between the chemical signatures (in particular of second-generation
stars) of
GCs and global cluster parameters, to see whether they are independent
relations or may be explained with a combination of these three main
parameters.
We can divide the parameters into five broad groups:
i) structural parameters
(including HBR, concentration c,
ellipticity, ,
,
and
(HB));
ii) orbital parameters and/or parameters depending on
the location in the Galaxy (
,
|Z|,
,
age, MV,
[Fe/H]
); iii)
primordial abundances ([(Mg+Al+Si)/Fe] and average [
/Fe]) and
first
generation ones (Mg
,
Si
,
Al
,
Na
,
O
,
plus
fraction of P stars); iv) chemical parameters of second-generation
stars
(Mg
,
Si
,
Al
,
Na
,
O
,
and fractions of I and E stars);
and v) parameters linking first and second generation stars
(slope of the [Al/Fe] vs [Na/Fe] ratios and IQR[O/Na])
.
The GC family is a complex one, with properties depending on many often interconnected parameters (see e.g., Djorgovski & Meylan 1994). While finding dependencies of a particular cluster property on others may be a viable approach, a more comprehensive and detailed analysis should take all clusters' parameters into account using a multivariate approach, so we applied the principal component analysis (PCA) on our set. This method has been used many times to understand the properties of the GC system (e.g., Fusi Pecci et al. 1993; Djorgovski & Meylan 1994; Recio-Blanco et al. 2006), but this is the first time that it is also extended to the properties of the different stellar generations in GCs. The method finds the correlation matrix of the whole parameter set and defines the dimensionality of the data set, i.e., the minimum number of dimensions required to fully explain the data.
Table 5: Correlation coefficients for 21 parameters of the 19 GCs.
Unfortunately, a rigourous study using the PCA is hampered by
i) the limited
sizes of the sample, only 19 GCs, since this is the only set for which
detailed
and homogeneous abundances of first and second generation stars are
available at
present; and ii) the fact that not all parameters are available for all
(neither
for the same) clusters. We first tried it on the maximum sample for
which all
the 34 above-mentioned parameters are available. This means 15 GCs,
where NGC 6388 and NGC 6441 were excluded because
they do not have orbital
information, NGC 6397, because we did not measure Al, and
NGC 288 because it
lacks a measure of ellipticity in Harris (1996). However,
excluding four
clusters could result in loss of significance in some cases. For
instance,
-elements
show a good correlation with MV
in our complete sample, but
not in the reduced one, possibly because two very massive clusters are
excluded.
We repeated the analysis using the whole GC sample, excluding those
parameters
that were absent for at least one of the GCs, which was possible for 21
parameters.
We give in Table 5
(only available on-line) the complete list of the correlation
coefficients among the 21 parameters. We show in Fig. 17 four examples,
one taken from the first computation (
)
and three from
the second one (MV,
[Fe/H], and age). The correlation coefficients are for
linear relations. Table 6
gives information on the dimensionality (the number of eigenvalues
larger than 1, the limiting value usually assumed in this kind of
analysis) and on the fractional and cumulative contributions of the
components. This table refers to both cases: 34 parameters for 15 GCs
(first four columns) and 21 parameters for 19 GCs (last four columns).
In the first case, the dimensionality is eight, the first three
eigenvalues only account for 62% of the total variance, while eight
components account for 93%. In the second case, the dimensionality is
five (or six), the first three eigenvalues account for 66% of the total
variance, while five (six)
components account for 83 (87)%.
Besides monovariate relations, we tried a semiempirical
approach to explore the
dependencies of cluster parameters from the fundamental quantities. In
particular, we wanted to test whether the key parameters mass,
metallicity,
age, and orbital elements (the last two representing the position in
the Galaxy)
are actually those giving the most significant relations with
structural and
chemical parameters of GCs. We derived the correlations for parameters
chosen in all the groups defined above
as a function of all bi-variate combinations of MV,
[Fe/H], age, and
;
then, we counted the frequency of the most significant correlations
(larger than 99%) for each combination in each group.
The results are given in Table 7
(on-line only) and summarised in Table 8.
The best combinations are essentially two: MV-age
and [Fe/H]-age.
Obviously, this is only meaningful if the main parameters we are using are independent. From the monovariate correlations we see that MV is not correlated with age. A significant correlation does instead exist between [Fe/H] and age. This is evident both in our sample (Fig. 17) and in the global one of Galactic GCs (Fig. 5), and it is stronger when individual subpopulations (inner halo vs disk/bulge) are considered. However, the age-metallicity relation is a physical one, intrinsic to the system of GCs, and not a spurious bias affecting our sample. We may safely conclude that most of the ``phenotypes'' of GCs can be explained rather well by the variations of three fundamental parameters: total mass, metallicity, and age, linked by the origin and the interaction of GCs in, and with, our Galaxy.
![]() |
Figure 17:
Example of the linear monovariate correlations found for
|
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In summary, in this paper we combine the results of our extensive survey of abundances in RGB stars in 19 GCs (Carretta et al. 2009a,b,c) with previous knowledge of a GC, in order to discuss scenarios for their formation. The novelty of our approach is to fully take into account the fact that GCs cannot anymore be regarded as simple stellar populations. For the first time it is possible to include among the properties of GCs a quantitative estimate of the ratio and of the chemical composition of different stellar generations. Our main findings are:
- (i)
- We first analyse the definition of GCs. The presence of the Na-O anticorrelation may be very well used to separate GCs from smaller (open) clusters. Second, we divide GCs according to their kinematics and location in the Galaxy in three populations: disk/bulge, inner halo, and outer halo. We find that the LF of bona fide GCs (that is, those which exhibit the Na-O anticorrelation) is fairly independent of their population. This suggests that it is imprinted by the formation mechanism, and only marginally affected by the following evolution.
- (ii)
- We then use the evidence of different generations within GCs given by their chemistry, and consider separately the composition of the primordial population and of the second generation. A large fraction of the primordial population should have been lost by the proto-GCs. We propose that the fraction of primordial population stars lost by GCs make up the main component of halo field stars. Arguments in favour include the total number of stars, the metallicity, kinematic and density distribution, and the chemistry.
- (iii)
- In addition, we argue that the extremely low Al abundances found for the primordial population of massive GCs is an indication of a very fast enrichment process before the formation of the primordial population. We then suggest a scenario for the formation of GCs including at least three main phases: a) the formation of a precursor population (likely due to the interaction with the early Galaxy or with other cosmological structures similar to those that led to the formation of dwarf spheroidals, but residing at smaller Galactocentric distances); b) which triggers a large episode of star formation (the primordial population); and c) then the formation of the current GC, mainly within a cooling flow formed by the slow winds of a fraction of this primordial population. Some stars of the primordial population remains trapped in the newly forming cluster, producing the primordial component still observed in GCs. The precursor population is very effective in raising the metal content in massive and/or metal-poor (mainly halo) clusters, while its rôle is minor in small and/or metal rich (mainly disk) ones.
- (iv)
- We then re-examine the second phase of metal-enrichment (from primordial to second generation): we consider monovariate, bivariate relations, and an explorative PCA. Our conclusion is that most of the ``phenotypes'' of GCs (and in particular their detailed chemical characteristics) may be ascribed to a few parameters, the most important being metallicity, mass, and age of the cluster. Location within the Galaxy (as described by the kinematics) also plays some rôle, while additional parameters are required to describe their dynamical status.
Table 6: Eigenvalues, fractional, and cumulative contributions for the two cases discussed in the text.
Table 7: Correlations, with number of clusters, degrees of liberty, Pearson coefficients (without sign), and significance in percent.
Table 8: Number of significant correlations with different class of parameters.
While corroborating evidence is coming from these studies, several issues are still dramatically open and/or poorly explored. A full hydrodynamical treatment of the formation and early evolution of GCs is still missing, the relation between GCs and past and present dSphs needs to be well studied, the nature and the precise yields of candidate first generation polluters still have to be definitively assessed, the rôle of binaries has to be well understood; to mention only a few open problems. The road to a deeper understanding of the GCs has been opened in the past few years, but the way is still long.
AcknowledgementsWe warmly thank Michele Bellazzini for useful discussions and a careful reading of the manuscript. The comments of the referee were very useful for producing a clearer manuscript. A.B. thanks the Observatoire de la Côte d'Azur for hospitality during the preparation of the paper. This research has made use of the SIMBAD database, operated at the CDS, Strasbourg, France, and of NASA's Astrophysics Data System. This work was partially funded by the Italian MIUR under PRIN 2003029437 and PRIN 20075TP5K9, and by INAF by the grant INAF 2005 ``Experimenting nucleosynthesis in clean environments''. S.L. acknowledges the support by the DFG cluster of excellence ``Origin and Structure of the Universe''.
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Online Material
Appendix A: Classification of Galactic globular clusters
Since the work by Zinn (1985) a few progresses were done with respect to his criteria for the separation of the subpopulations of Galactic GCs. Many classification schemes rest on the appearance of the clusters' CMD and related parameters (namely metallicity, age and HBR index). However, one of the main aims of our project is to explain the HB morphology and its relations with chemical signatures of stellar generations in GC, so we cannot use the distribution of stars along the HB as a separation criterion. In Table A.1 we list the quantities used in Sect. 3.3 to separate disk/bulge clusters from the halo ones according to the combination of their location in the Galaxy and their kinematics.
Table A.1: Classification and main parameters adopted for GCs.
![]() |
Figure A.1: Classification of disk (red squares) and inner halo (blue dots) clusters. The curve is the discriminating line as obtained from our selection criteria. |
Open with DEXTER |
![]() |
Figure A.2: Absolute values of the difference dV between the observed radial velocity of GCs and the one expected from the Galactic rotation curve, as a function of the rotational velocity given by Dinescu et al. (1999) and Casetti-Dinescu et al. (2007). The dotted line indicates one-to-one correlation, while the red solid lines indicate the linear regression. |
Open with DEXTER |
Table A.2: Comparison of our classification with the one by Mackey & van den Bergh (2005).
Table A.3: Globular clusters of LMC, SMC, and Fornax dSph and their properties.
As said in Sect. 3.3,
outer halo clusters were simply classified as those currently located
at more than 15 kpc from the centre of the Galaxy (see Carollo
et al. 2008).
Clusters with
below 3.5 kpc were
considered as bulge GCs, even though some of them might be halo
clusters on
very elongated orbits presently close to the pericentres. To separate
the
remaining clusters into inner halo and disk GCs, we computed the
differences
(dV, Col. 8 in Table A.1) between the
observed radial velocity (corrected to the LSR) and the one expected
from the Galactic rotation curve (see Clemens 1985). In the dV-Z
plane (where Z is the clusters' distance from the
Galactic plane, in kpc, see Col. 10 of Table A.1), we defined an
ellipse with equation

Clusters with y<1 were classified as disk GCs, while we considered as halo GCs the ones with y>1, see Fig A.1. Of course, a better estimate of GC kinematic is possible when the whole orbit is available. Given the quite good correlation (see Fig. A.2) between dV and the rotational velocity (Col. 9 of Table A.1, where



It should, however, be clear that dV is not at all a synonymous of (

Column 11 in Table A.1 shows our
classification for the population of
the Galactic GCs in disk/bulge (D/B), inner halo (IH), outer
halo (OH), and GCs of dSphs. For each cluster we report the
integrated magnitude (,
Col. 2), the HB morphology parameter (HBR, Col. 6),
and the Galactocentric distance (
,
Col. 7)
as directly retrieved from the Harris catalogue. The metallicity values
([Fe/H], Col. 3) were instead replaced with the determinations
by Carretta et al. (2009c).
Additionally, we list in Col. 4
the [
/Fe] ratios
(with corresponding references given in the table
notes). Column 5 displays the age parameter; more in detail,
we computed an
average value between the two different estimates by Marin-Franch
et al. (2009)
and De Angeli et al. (2005), after
applying a correction of 0.08 to the second ones for GCs with
[Fe/H] ranging from -1.8 to -1.1 dex, as suggested by a
cluster-to-cluster comparison. When neither of these estimates was
available, we adopted the ones calculated by Vandenberg (2000),
normalised to the Marin-Franch scale by assuming that
13.5 Gyr = 1.00. We then corrected the
values so obtained for the difference between the metallicities
considered in those
papers and those listed in Carretta et al. (2009c),
transformed into [M/H] using an average [
/Fe] of +0.4 (see
Table 2).
This correction was made using the sensitivity of age on metallicity
given by
Marin-Franch et al. (2009).
First, we decided to compare our new classification with the
previous ones
relying only on metallicity and HB morphology (see Sect. 3.3). As
representative of this approach, we chose the work by Mackey &
van den Bergh
(2005).
Briefly, they defined as disk component all the GCs with
[Fe/H]>-0.8 dex; the so-called ``old'' halo and
``young'' halo clusters were then divided following Zinn (1993), namely
by computing the offset in HB type -at a given metallicity- with
respect to the fiducial line of the inner halo clusters. GCs with an offset larger
and smaller than -0.3 in HB type were classified as old halo
and young
halo, respectively. The Table A.2 schematically
shows the comparison and emphasises the different natures of the two
classifications. As (partially) expected, the matrix is not diagonal;
i.e., there is not a one-to-one correlation
between old halo (young halo) and inner halo (outer halo) subgroups.
More in
detail, the metallicity criterion is largely responsible for such a
discrepancy: had we adopted the requirement of
0.8 dex,
35 of the 36 clusters that we classified as disk/bulge and
Mackey & van den Bergh as old
halo should be moved into inner halo+old halo cell, while all the 5 GCs
placed in the disk+young halo box should become inner halo+young halo
clusters
thanks to their low metallicity. However, and most important, even
taking these changes into account in the relative population of the
matrix cells, the
resulting correspondence is not yet one-to-one. As to the inner halo
GCs, 80% constitute the old halo and the remaining 20% the
young halo clusters; for the outer halo GCs, the promiscuity is even
greater, resulting in 40% and
60%, respectively, for old and young haloes. This is direct evidence of
the strong difference between kinematics (and/or positional) criteria
and the
ones based only on metallicity and HB type.
One last word on the classification. While this work was in
preparation, a paper by Fraix-Burnet et al. (2009) appeared,
where they use a cladistic technique to divide a sample of
54 GCs into three subsamples (called Groups 1, 2,
and 3 and later identify with inner halo, outer halo, and
disk, respectively) on the basis of [Fe/H],
MV,
,
and age. We cross-checked the assignments for the clusters in common
and found good agreement only for disk clusters, and this in a limited
sense. When they classify a cluster as disk, we agree (in
17 cases out of 18), but we have many other disk
clusters that they instead
classify in the halo subsamples. In particular, for the 19 GCs
in our FLAMES
sample, the two classifications agree for seven clusters and disagree
for seven
others (five GCs are not present in their data set). We think that the
main
factor producing this difference is that they ignored the
kinematics, although the information is present for their sample, while
our
method rests on that.
To conclude, we report in Table A.3 the analogoues
of
Table A.1,
but for the LMC, SMC, and Fornax GC systems; as
in the previous case, the number in brackets corresponds to the
reference (for
[/Fe],
[Fe/H], age, and HBR) whose decoding is given in the Notes. The
integrated magnitudes MV
for the LMC and Fornax GCs are taken from
van den Bergh & Mackey (2000), while
for the SMC ones were computed from the apparent magnitudes UBV
by van den Bergh (1981),
along with the distance moduli as given in those papers providing the
clusters' age (Refs. 15-17 see
Table A.3).
As to age, for LMC and SMC GCs, since absolute values
were available (see ref. given in Table A.3), we report
them to our
relative scale, adopting the previous conversion of
13.5 Gyr = 1.00. For the
Fornax clusters, the ages were instead derived starting from the
cluster-to-cluster relative differences (
Age) obtained by Buonanno
et al. (1998,
1999) and
assuming that 1.05 =
14.2 Gyr.
Footnotes
- ... parameters
- Based on observations collected at ESO telescopes under programmes 072.-D0507 and 073.D-0211.
- ...
- Appendix A is only available in electronic form at http://www.aanda.org
- ...
2007)
- The strong objection made by Renzini (2008) on the outflowing
of matter from FRMS being unable to result in clearly separated MS with
different - and discrete - He content, still applies. However, up to now
the only clear cases of several discrete MSs are the very peculiar
Cen and NGC 2808. Indications for widening of the MS have been obtained for other clusters, such as NGC 104 (Anderson et al. 2009) and NGC 6752, where Milone et al. (2010) also see hint of a split. On the other hand, Renzini (2008) restricts his favourite candidate polluters, AGB stars, to those experiencing only a few episodes of third dredge-up. This might appear too specific and at odds with observed abundances of s-process elements in some GCs.
- ... present
- While writing this paper, Lind et al. (2009) published the analysis of an extended set of unevolved stars in NGC 6397, and we completed the analysis of turn-off stars in NGC 104 (D'Orazi et al. 2010), where Na abundances show similar variations.
- ...2004
- A chemical analysis similar to ours has been performed in M 22 by Marino et al. (2009). This data, kindly given to us before publication, nicely fit in our relations. However, we do not include it in the present analysis because it is not strictly homogeneous.
- ... ones
- Similarly, Pritzl et al. (2005) adopted kinematics to assign GCs to various Galactic components; however they were able to do so only for 29 of the 45 GCs they studied.
- ... low
- This does not mean that the pace of evolution was uniformly slower in the halo than in the disk. It is indeed possible that star formation (and chemical evolution) in the halo actually occurred in bursts separated by long quiescent phases, while it was characterised by prolonged phases at a relatively low level in the disk. This might lead to the paradoxical situation that stars in the halo have a chemical composition more appropriate to faster star formation than those in the disk, although the former might actually be younger. We come back to this point in the next section.
- ... cluster
- Of course, Al is not an
-element. However, in the primordial populations, Al abundance is always negligible with respect to that of Mg and Si; therefore, for these stars the sum of Mg+Al+Si is essentially the sum of Mg+Si. Within the GC, when some stars are very rich in Al, this comes from p-captures on 24Mg, 25Mg, 26Mg. This Al results then from material originally produced as
-rich, and the total of Mg+Al+Si is conserved throughout these reactions. For this reason, we may use this sum as an indicator of the abundance of the
-elements.
- ...
- Had we integrated the IMF over the range
0.1-50
, which clearly leads to overestimating the fraction of low-mass stars (see Chabrier 2003), the values in Cols. 5-7 of Table 3 should have been increased by
50%.
- ... excesses
- We only considered those GCs with [Fe/H] <-1. This ratio does not change significantly if we compute the fraction of Na-rich stars in each cluster and then average this value. In this way we underestimate the fraction of second generation stars, but we use this value here for consistency with the field stars.
- ... GC
- This enrichment
should be very uniform, suggesting a super-wind from the precursor association
(Mac Low & McCray 1988). There might also be a selection effect against
the most massive and energetic SNe, possibly reducing the typical [
/Fe] ratio of the next generation stars.
- ... likely
- Given the very fast evolutionary lifetimes of FRMS, it is possible that the SN explosions from this component would hamper the formation of an efficient cooling flow.
- ... IQR[O/Na]
- We verified that the corresponding quantity for the Mg-Al anticorrelation IQR[Mg/Al] shows a general correlation with IQR[O/Na], with some scatter. However, IQR[Mg/Al] could only be estimated for the comparatively few stars observed with UVES. Furthermore, we could not compute this index for four GCs of our sample, because three only had 5-7 UVES spectra per cluster (NGC 6171, NGC 6388, and NGC 6441) and one without Al determination (NGC 6397). Thus, IQR[Mg/Al] has large uncertainties and will not be used in the rest of this paper. On the other hand, the IQR[O/Na] for NGC 6397, based on only 16 stars, is quite indiscernible from the others (based on more stars) in all relations shown in the following. This also supports the robustness of this indicator for the GC in our sample with the smallest number of sampled stars.
- ...
- These results would not change had we used older
parameters measuring the length of the HB, such as
or BT from Fusi Pecci et al. (1993).
- ...
[Fe/H]
- [Fe/H] was included in this group to take into account that inner halo GCs are on average more metal-poor than disk clusters.
- ... IQR[O/Na])
- We used here all
the possible indicators of chemistry in first and second generation stars
because some are affected by saturation (e.g., Na
and O
) and others only show a small variation from the original value (e.g., Si).
- ...
clusters
- Both Zinn (1993) and Mackey & van den Bergh (2005) labelled inner halo GCs the ones more metal-poor than [Fe/H]=-0.8 dex and located at Galactocentric distance less than 6 kpc.
All Tables
Table 1: Properties of the 19 GCs in our sample.
Table 2: Quantities for the same GCs, derived by our works.
Table 3: Original/final mass of GCs required to produce the observed ratios between number of stars in first and second generations.
Table 4: Pearson's correlation coefficients and level of significance for relations in P, I, and E stars.
Table 5: Correlation coefficients for 21 parameters of the 19 GCs.
Table 6: Eigenvalues, fractional, and cumulative contributions for the two cases discussed in the text.
Table 7: Correlations, with number of clusters, degrees of liberty, Pearson coefficients (without sign), and significance in percent.
Table 8: Number of significant correlations with different class of parameters.
Table A.1: Classification and main parameters adopted for GCs.
Table A.2: Comparison of our classification with the one by Mackey & van den Bergh (2005).
Table A.3: Globular clusters of LMC, SMC, and Fornax dSph and their properties.
All Figures
![]() |
Figure 1: Summary of the Na-O anticorrelation observed in the 19 GCs of our sample. Arrows indicate upper limits in O abundances. The two lines in each panel separate the primordial component (located in the Na-poor/O-rich region), the Na-rich/O-poor extreme component, and the intermediate component in-between (called P, E, and I, respectively as indicated only in the first panel). See Sect. 2 for details. |
Open with DEXTER | |
In the text |
![]() |
Figure 2: [Na/Fe] ratios as a function of the metallicity [Fe/H] in a range centred on the average metal abundance of NGC 6397. Filled triangles in grey-tones are field stars from Gratton et al. (2003a) and the compilation by Venn et al. (2004). Filled circles are stars in NGC 6397 with determinations of both O and Na (red: P component, blue: I component). Empty (green) star symbols are stars in NGC 6397 with only Na abundances derived. |
Open with DEXTER | |
In the text |
![]() |
Figure 3:
Relative age parameter vs. absolute magnitude MV
for globular and old open clusters (see Appendix for details). Red
filled pentagons and triangles are GCs where Na-O anticorrelation has
been observed, in the Milky Way or the LMC, respectively; green squares
are clusters that do not show evidence of Na-O anticorrelation, both
members of Sagittarius dSph, either of the main body
(Terzan 7) or the stream (Pal 12). Open stars and
triangles mark clusters for which not
enough data is available, in the Milky Way or the LMC respectively.
Finally,
open circles are old open clusters (data from Lata et al. 2002).
Superimposed are lines of constant mass (light solid lines, see
Bellazzini et al. 2008a).
The heavy blue solid line (at a mass of
|
Open with DEXTER | |
In the text |
![]() |
Figure 4: Cumulative luminosity functions of different groups of Galactic GCs (from the Harris 1996 catalogue) according to our present classification criteria and of GCs in dSphs (from van den Bergh and Mackey 2004; see Appendix for references on Fornax an LMC clusters). The red solid line indicates disk/bulge clusters, the blue dotted line the inner halo clusters, the dashed green line clusters in the outer halo, magenta dashed-dotted line is for clusters in dSphs, and the green-gold long dashed line for GCs in LMC. |
Open with DEXTER | |
In the text |
![]() |
Figure 5: Age-metallicity relation for different groups of GCs: outer halo clusters (green pentagons), inner halo clusters (blue circles), disk/bulge clusters (red squares). Magenta circles are GCs associated to dSphs. Different symbol sizes are used for clusters of different luminosity. |
Open with DEXTER | |
In the text |
![]() |
Figure 6:
Relation between age and excess of |
Open with DEXTER | |
In the text |
![]() |
Figure 7:
Comparison of [Na/Fe] values between field and GC stars as a
function of metallicity. In both panels the filled red circles are for
our sample of GCs, indicating [Na/Fe]
|
Open with DEXTER | |
In the text |
![]() |
Figure 8:
[O/Fe]
|
Open with DEXTER | |
In the text |
![]() |
Figure 9: Relation of the ratio [(Mg+Al+Si)/Fe] as a function of several orbital parameters: a) total energy of the orbit; b) orbital period; c) apogalatic distance, and d) maximum distance above the Galactic plane. Also indicated are the Spearman and Pearson correlation coefficients. |
Open with DEXTER | |
In the text |
![]() |
Figure 10:
Run of the [Al/Mg] ratio as a function of the [Mg/H] ratio in field
stars (grey-tone open circles), GCs in our sample (red and blue
filled circles and squares, respectively) and stars in dSphs (green
triangles,
the open ones are upper limits in Al, see text for references). The
[Al/Mg]
ratio in our sample refers to primordial abundances, namely [Al/Fe]
|
Open with DEXTER | |
In the text |
![]() |
Figure 11: Left: fraction of stars in the primordial P ( upper panel), intermediate I ( middle panel) and extreme E ( lower panel, with a different scale on the y-axis) components of GCs as a function of the IQR[O/Na]. Right: the same, as a function of [(Mg+Al+Si)/Fe]. The Pearson and the Spearman rank correlation coefficients are shown in the box, here and in the next figures. |
Open with DEXTER | |
In the text |
![]() |
Figure 12: Extension of the Na-O anticorrelation, measured by the IQR[O/Na], as a function of the total sum of Mg+Al+Si atoms for our sample of clusters. |
Open with DEXTER | |
In the text |
![]() |
Figure 13:
Left: fraction of stars of the P,
I, and E components
(upper, middle, and lower panels, respectively) as a
function of |
Open with DEXTER | |
In the text |
![]() |
Figure 14: Left panels: the fraction of stars in the P, I, and E components of second-generation stars as a function of the total absolute magnitude (hence, mass) of clusters. Right: the same, as a function of relative age. |
Open with DEXTER | |
In the text |
![]() |
Figure 15: Interquartile range of the [O/Na] ratio as a function of the maximum temperature reached on the HB (taken from Recio-Blanco et al. (2006) or derived here). The line connects the value for M 15 based on our data and the one derived from the literature (open green triangle, see text). |
Open with DEXTER | |
In the text |
![]() |
Figure 16: The extension of the Na-O anticorrelation (measured using IQR[O/Na]) as a function of the clusters' absolute magnitude MV from Harris (1996). The Pearson correlation coefficient is given and five GCs discussed in the text are indicated. |
Open with DEXTER | |
In the text |
![]() |
Figure 17:
Example of the linear monovariate correlations found for
|
Open with DEXTER | |
In the text |
![]() |
Figure A.1: Classification of disk (red squares) and inner halo (blue dots) clusters. The curve is the discriminating line as obtained from our selection criteria. |
Open with DEXTER | |
In the text |
![]() |
Figure A.2: Absolute values of the difference dV between the observed radial velocity of GCs and the one expected from the Galactic rotation curve, as a function of the rotational velocity given by Dinescu et al. (1999) and Casetti-Dinescu et al. (2007). The dotted line indicates one-to-one correlation, while the red solid lines indicate the linear regression. |
Open with DEXTER | |
In the text |
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