© ESO, 2012

1. Introduction

Our ideas on Galactic globular clusters (GC) have been revolutionized in the last few years by the discovery of multiple sequences in their color magnitude diagrams (CMD; see Piotto 2009; Milone et al. 2010, and references therein) and by evidence that the well-known star-to-star spread in the abundance of light elements (e.g. O, Na, Mg, Al) is not due to some mixing mechanism, but was imprinted in the gas from which cluster stars formed (see Ramirez & Cohen 2001; Gratton et al. 2001, 2004, for discussion and references). While we lack a fully satisfying model for GC formation accounting for the variety of observational phenomena that are being unveiled, the notions that most GCs formed more than one generation of stars during the first few 10⁸ yr of life and that the subsequent generations were – at least partially – polluted by chemical elements produced by previous generations is now generally accepted (see, e.g. D’Antona et al. 2005; Decressin et al. 2007, 2010; Ventura & D’Antona 2008; D’Ercole et al. 2008; Renzini 2008; Carretta et al. 2010a; Valcarce & Catelan 2011; Bekki 2011; Schaerer & Charbonnel 2011, for a detailed discussion).

In the previous papers of this series, the chemical signatures of this self-enrichment process were studied in detail, with special attention to the anti-correlation between [Na/Fe] and [O/Fe], using a large sample (>2000) of stars in 19 GCs, for which medium-to-high resolution spectra were obtained with the Giraffe and UVES fiber-fed spectrographs, mounted at ESO/VLT (see Carretta et al. 2006; Gratton et al. 2007; Carretta et al. 2009a,b, for details, results and discussion). The main results of this large project have been considered in a wider context and correlated with other characteristics of the clusters, like the horizontal branch (HB) morphology, in Carretta et al. (2009c, 2010a), and Gratton et al. (2010). In the present contribution we use an obvious byproduct of the spectroscopic survey, i.e. relatively large sets of very accurate radial velocities (RV), to explore the kinematics of the 19 program clusters (Carretta et al. 2009a, Paper VII hereafter), plus NGC 1851 from Carretta et al. (2011, see Table 1.

These samples, which were collected for a very different scientific goal, are far from ideal to provide a full and detailed characterization of the cluster kinematics. The typical number of stars per cluster ( ≲ 150) is clearly not comparable to the most recent dedicated studies, based on several hundred RVs (see e.g., Lane et al. 2009, 2010a,b; Sollima et al. 2009), in some cases coupled with proper motions (van de Ven et al. 2006; van den Bosch et al. 2006; McLaughlin et al. 2006). Furthermore, the radial distribution of the stars does not cover all the relevant radial ranges, because of limitations imposed by the fiber allocation process, and also because to obtain the most reliable chemical abundances, it is actually preferable to avoid the most crowded regions of the clusters where contamination from stars other than the intended target can become an issue. In particular most of the stars in our samples lie beyond the half-light radius (r_h) of the clusters (see Table 1, below). On the other hand, the membership to the parent clusters of all the stars considered in this study has been established not only on the basis of radial velocity cuts but also on very detailed chemical analysis of each individual star¹. Moreover, our samples provide the unprecedented possibility of a systematic search for correlations between the chemical composition and the kinematics of the cluster stars.

The plan of the paper is the following. In Sect. 2 we briefly describe the global sample and assess the quality of the RV estimates. In Sect. 3 we explore the possible connection between the kinematics and the chemical abundance of Na, which is taken as the most reliable tracer of the light elements’ self-enrichment at the basis of the Na-O anticorrelation. In Sect. 4 we consider in more detail the RV distribution of the clusters whose kinematics have been previously studied only by means of integrated spectra of their center and/or with samples of RV for individual stars smaller than ours. In addition we search for systemic rotation in all the program clusters for which this analysis has not been performed in previous studies. In Sect. 5 we briefly summarize and discuss the main results of the analysis, including some intriguing correlations between rotation and other cluster parameters, which are found here for the first time.

2. The sample

In the following we use the symbols V_r and RV interchangeably to indicate heliocentric line-of-sight velocities. We make use of the data collected in the Harris (1996, H96 hereafter) catalog: in all cases we refer to the 2010 version of this catalog, publicly available at www.physics.mcmaster.ca/Globular.html. The coordinates of the cluster centers are taken from Noyola & Gebhardt (2006), when available, and from H96 in the other cases. The parameters of the King (1966, K66) or Wilson (1975, W75) models best-fitting the surface brightness profiles of the clusters are taken from McLaughlin & van der Marel (2005, MvM05), specifically the core and tidal radii r_c, r_t, while half-light radii r_h, lacking in MvM05, are from H96. We adopt the metallicity scale by Carretta et al. (2009c). Kouwenhoven & de Grijs (2008) has recently demonstrated that in relatively dense and massive clusters like those considered here, the effects of binary stars on the global kinematics should be minor or negligible (e.g. leading to an increase in the observed velocity dispersion  ≲ 0.5 km s^-1, even for binary fractions as high as 100 percent, see their Fig. 10). Since, in addition, GCs typically have binary fractions  ≲ 20 percent (Sollima et al. 2007; Milone et al. 2008), we consider binaries as a negligible factor for our analysis².

Any detail about the measure of RV and chemical abundances, as well as target selection and membership can be found in the previous papers of the series (Carretta et al. 2006; Gratton et al. 2007; Carretta et al. 2009a,b, 2011). All the data used in this paper are publicly available in electronic form at the CDS³ (see the original papers).

The program clusters are listed in Table 1. The second column of the table reports the number of member stars having a valid measure of RV. The number of stars per sample ranges from 30 to 156 stars per cluster, with a mean of 99. Each of these stars also has at least a measure of iron abundance, and in many cases the abundance of other elements is also available (Na, in particular). The selected stars not only have RV that is fully compatible with the systemic velocity of the cluster but also display chemical abundance pattern identifying them as cluster members. The fraction of sample stars lying within the half-light radius of the cluster is listed in the third column of the table.

Fig. 1 Upper panel: comparison between RVs estimated from spectra obtained with the HR13 and HR11 grisms. Different symbols correspond to different clusters. The continuous line is drawn at a typical value for the mean difference (ΔVr =  −0.5 km s-1), and the dotted lines enclose the  ± 2σ range about the mean, where a typical value of σ = 0.7 km s-1 has been adopted (see Table 1). Lower panel: comparison with the external dataset by L11 for two representative clusters, NGC 104 (filled circles) and NGC 6218 (empty circles). The continuous line marks ΔVr = 0.0 km s-1, the dotted lines enclose the  ± 2σ range. The fraction of stars lying within  ± 2σ is also reported [F(Δ < 2σ)].

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In the large majority of clusters most stars have been observed using two FLAMES-GIRAFFE set-ups, the high-resolution gratings HR11 (centered on 5728 Å) and HR13 (centered on 6273 Å), which were respectively chosen to measure the Na doublets at 5682–5688 Å and 6154–6160 Å, and the [O I] forbidden lines at 6300, 6363 Å, as well as several lines of Fe-peak and α-elements. The spectral resolutions are R = 24   200 (for HR11) and R = 22   500 (for HR13), at the center of the spectra. The fifth column of the table reports the number of stars having valid RV measures from spectra obtained with both set-ups. These stars therefore have two independent RV estimates and can be used to estimate the internal consistency and accuracy of our radial velocities. This is especially useful since the pipeline used for the survey does not provide uncertainties on the individual RV estimates.

However, it has been demonstrated by comparison with other independent datasets that the adopted pipeline provides RV estimates with typical errors that are smaller than 1 km s^-1 from spectra obtained with the same instrumental set-up (Carretta et al. 2010c)⁴.

The comparison between the RV estimates obtained from the two GIRAFFE set-ups is shown in the upper panel of Fig. 1. The mean difference and the standard deviation of the difference between the two sets of estimates are reported in the 4th and 5th columns of Table 1. It can be appreciated that both the mean difference and the rms are lower than 1 km s^-1 in the large majority of cases. The small differences in the zero-point between the two RV sets are not a reason for concern in the present analysis. We transformed HR11 RVs into the HR13 system by applying the shifts listed in the 4th column of Table 1, then we obtained a single RV estimate per star by adopting RV_HR13 as reference value, and the corrected RV_HR11 value when the HR13 velocity is missing. Velocities from HR11 were chosen as a reference since the associated spectra typically have higher signal-to-noise ratios than HR13 ones. On the other hand, we have to note that the HR13–HR11 comparison reveals that three clusters have RV estimates of significantly lower accuracy than the rest of the sample. These are NGC 4590, NGC 6397, and NGC 7078, three among the most metal-poor clusters of the sample. The lower quality of the RV measures for these clusters are likely accounted for by the extreme weakness of the spectral lines due to the extremely low metal content, possibly coupled with the relatively high temperature of the target stars. The latter effect depends on the actual distribution in color and magnitude of the targets, which can differ from cluster to cluster. For instance, considering the case of two very metal-poor clusters having RV measures of different quality, the median T_eff of the NGC 6809 sample (σΔ = 0.4 km s^-1) is 4797 K, while it is 5030 K for NGC 7078 (σΔ = 4.6 km s^-1). Cooler atmospheres imply more detectable lines, keeping all the other parameters fixed, thus allowing more accurate RV estimates.

In the lower panel of Fig. 1, we show the comparison between the RV from the present study and those from the public dataset by Lane et al. (2011, L11, hereafter) for two clusters in common between the two datasets taken as representative of the whole range of magnitude covered by our targets, i.e. NGC 104 and NGC 6752. The zero-points agree within less than 0.5 km s^-1 and, most important, the standard deviation in the RV difference is  ≤ 1.2 km s^-1, implying typical errors  ~1.2/ km s^-1. We note that 95–98% of the differences lie within  ± 2.0σ from the mean, which is fully consistent with the expectation for a Gaussian distribution. These results are in excellent agreement with those presented in Carretta et al. (2010c). In conclusion, internal and external comparisons consistently indicate that individual RV estimates in our sample have typical uncertainties smaller than 1 km s^-1, so their quality is fully adequate for studying the internal kinematics of GCs. It should be kept in mind that in the cases of NGC 4590, NGC 6397, and NGC 7078 the uncertainties are larger, typically 2 km s^-1, or even slightly larger in the case of NGC 7078.

The last column of Table 1 lists the main sources of kinematic data for each cluster available in the literature, i.e. from the largest samples and/or the most recent and comprehensive studies. Eight clusters are shared with the survey by Lane et al. (2009, 2010a,b, hereafter L09, L10a, L10b, respectively), whose data have been published in L11. These papers report comprehensive kinematical analysis based on very large samples (several hundred member stars per cluster) of R = 10   000 spectra (in the CaT region) obtained with the AAOmega instrument at the Anglo Australian Telescope, and can be considered as the state-of-the-art, at least from the observational point of view (see L11, for discussion). A few other clusters have been studied with smaller samples than in L11 but still larger than ours: Scarpa et al. (2011), Côté et al. (1995), Meylan & Mayor (1991), or assembled by Pryor & Meylan (1993, PM93 hereafter). PM93 also provide comprehensive references for studies performed before 1993–1994, and it remains the main source for central velocity dispersions (σ₀) of Galactic GCs. In several cases estimates of σ₀ derived from integrated spectra of the cluster center (from Illingworth 1976; Zaggia et al. 1992; Dubath et al. 1997) constitute a relevant complement to samples of RV for individual stars and, in some case, the only available measure of the cluster kinematics (NGC 2808, NGC 6388, NGC 6441). NGC 7078 has been the object of a very detailed and refined analysis based on nearly two thousand RV and proper motions by van den Bosch et al. (2006).

3. Kinematics and chemical composition

There are only very few massive Galactic GCs whose stars display a spread in iron (and/or calcium) abundance, either large (ω Cen, see Johnson & Pilachowski 2010; Marino et al. 2011a and references therein; Terzan5, Ferraro et al. 2009; Origlia et al. 2011) or small (M54, Bellazzini et al. 2008; Carretta et al. 2010b; M22, see Da Costa et al. 2009; Marino et al. 2011b and references therein; NGC 2419, Cohen et al. 2010; Ibata et al. 2011; Cohen & Kirby 2011; NGC 1851, Carretta et al. 2011). At present there is no firmly established case for a correlation between iron abundance (or metallicity, in general) and star kinematics in these clusters. Interesting correlations have been reported by various authors for ω Cen (Norris et al. 1997; Ferraro et al. 2002; Sollima et al. 2005; Gratton et al. 2011), but were not confirmed by other studies (Pancino et al. 2007; Bellini et al. 2009), hence they remain to be further verified (see also Bekki 2010). Carretta et al. (2011) found no difference in the kinematics of the “metal-rich” and “metal-poor” stars in NGC 1851.

With the only exception of NGC 1851, all the clusters in our sample are very homogeneous (internally) in iron abundance, with the observed star-to-star spread fully consistent with observational errors (Carretta et al. 2009c, Paper VII). Therefore, they seem the ideal sample for a systematic search of connections between the kinematics and the abundance of light elements known to display a significant spread within each cluster, and involved in the correlations and anti-correlations that were the main object of the overall program. As far as we know, this exploration has never been attempted before.

All the available observational evidence on multiple populations in GCs seems to indicate that the formation of the various generations of stars and the associated chemical enrichment must have occurred at very early epochs, approximately in the first few 10⁸ yr of cluster life. It is therefore likely that any possible sign of a difference in the kinematical properties between different generations of stars present at those times (predicted, for instance, in the models by Bekki 2011) have been erased by two-body relaxation during the lifetime of GCs (see Decressin et al. 2008). According to the H96 catalog, the median two-body relaxation time of Galactic GCs is just  ≃ 1 Gyr, while the typical age is  ≃ 12.5 Gyr. However, the same was expected for any difference in the radial distribution of various generation of stars, while it is generally observed that Na-rich/O-poor stars are more centrally concentrated than Na-poor/O-rich stars⁵ (see, for example, D’Ercole et al. 2008; Decressin et al. 2010; Lardo et al. 2011, references and discussion therein). Moreover, dedicated simulations are required to establish whether two-body relaxation is in fact able to remove all the signs of difference in the initial conditions over the whole radial range of the cluster (Lardo et al. 2011; Bekki 2010). Therefore, it is clearly worth verifying that any correlation between kinematic and light-element abundance is there, even if it is not expected to be observable at the present epoch. The main caveats for interpretating of our results are associated with the relatively sparse samples and by the radial distribution of the target stars that virtually misses the cluster cores (see Table 1, also recalling that the core radii of GCs are always smaller than their half-light radii).

Fig. 2 Velocity dispersion as a function of Na abundance for NGC 104, NGC 2808, NGC 288, NGC 1851, NGC 1904, NGC 3201, NGC 4590, and NGC 5904. Larger filled squares indicate cases where one star has been clipped from the sample because of an RV value more than 3 − σ from the mean. Only estimates obtained from  ≥ 10 stars (after clipping) are plotted. The vertical scale is different for NGC 104 and NGC 2808, to accommodate for the larger dispersion of these clusters.

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	Fig. 3 The same as Fig. 2 for the remaining clusters of our sample. The vertical scale is different for NGC 6838 and NGC 6441 to accommodate the larger dispersion of these clusters.
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As the best tracer of the light element spread we take the sodium abundance [Na/Fe]. The main reasons for this choice are that (a) Na abundance is much easier to measure than, for instance, O abundance, and, as a consequence, reliable Na abundance estimates are available for the large majority of the stars in our sample, and, (b) Na is one of the elements showing the widest abundance spread within each globular.

In Figs. 2 and 3, we plot the velocity dispersion of cluster stars as a function of the [Na/Fe] abundance for all the program clusters. In these plots, each point corresponds to the value of the velocity dispersion σ estimated from the stars whose [Na/Fe] is enclosed within  ± 0.2 dex from the central values (marked by the plotted points); these are spaced by 0.1 dex. Only estimates obtained from  ≥10 stars (after clipping) are plotted. The errors on the velocity dispersion are computed with the jackknife bootstrapping technique (Lupton 1993), as in Bellazzini et al. (2008, B08 hereafter).

In the vast majority of cases dispersion curves as a function of [Na/Fe] are completely flat, within the uncertainties, so the main conclusion that can be drawn from Figs. 2 and 3 is that, in general, there is no correlation between the velocity dispersion and sodium abundance. There are only three cases that deserve some further comment. The two metal-rich and bi-modal HB morphology clusters NGC 6388 and NGC 6441 (Rich et al. 1997) show some marginal evidence of a drop in the velocity dispersion with increasing Na abundance, occurring around [Na/Fe]  ~ 0.4, in line with the predictions of Bekki (2011) models. The same seems to also occur for NGC 2808 (another cluster with multimodal HB, see Dalessandro et al. 2011, and references therein), but in this case the effect is more pronounced, also thanks to the larger sample and the lower uncertainties in the σ estimates. To check the significance of the observed difference we compared the mean RV and the velocity dispersion of the Na-poor and Na-rich samples, for two different thresholds⁶ separating the two subsamples, [Na/Fe] = 0.4 and [Na/Fe] = 0.5, for NGC 2808, NGC 6388, NGC 6441, and for NGC 6752 and NGC 6809, taken as examples of clusters with flat σ vs. [Na/Fe] distributions. The results are reported in Table. 2, together with the value of the F parameter (), and the probability that the two subsamples are drawn from populations having the same velocity dispersion, according to an F test (Brandt 1970). The probability is about 20 per cent for NGC 6809 and NGC 6752, independent of the adopted threshold. The possibility that the two subpopulations have the same σ is clearly far from excluded, for NGC 6388 and NGC 6441, but the probability is lower than ten per cent in both cases, at least for the [Na/Fe] = 0.5 threshold. Hence, the hint of a difference shown here may need to be explored with larger samples. On the other hand, the probability is lower than one per cent in the case of NGC 2808, independent of the adopted threshold. The NGC 2808 sample is rich enough to allow for a more detailed investigation.

3.0.1. The case of NGC 2808

An obvious possibility for the origin of the lower σ of Na-rich (w.r.t. Na-poor) stars in NGC 2808 is that the former may have a radial distribution less concentrated than the latter. In any isotropic mass-follow-light self-gravitating equilibrium system, the velocity dispersion reaches its maximum value at the center and declines with radius. Independently of anisotropy, this is also observed to be the case for NGC 2808 (see below). Although Na-rich stars are usually observed to be more centrally concentrated than Na-poor stars, still an unlucky selection of targets may turn out in a Na-rich sample typically lying at larger radii, thus implying a lower σ with respect to Na-poor. To check this possibility we plot in Fig. 4 the RV and radial cumulative distributions for Na-rich and Na-poor stars in NGC 2808 and NGC 6752, for comparison.

Fig. 4 Comparison of cumulative distributions for Na-rich (red continuous line) and Na-poor (blue dotted line) for NGC 2808 (upper panels) and NGC 6752 (lower panels). Left panels: distributions of the radial velocity in the cluster system. Right panels: distributions of the distances from the cluster center. The probability that the Na-rich and Na-poor populations are drawn from the same parent population, according to a Kolmogorov-Smirnov test, is reported in the lower right corner of each panel. The adopted threshold between Na-poor and Na-rich stars is [Na/Fe] = 0.5.

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In NGC 6752 the two RV distribution are indistinguishable, while the higher concentration of the Na-rich sample is obvious, and likely tracing a real difference in the radial distribution of the two populations (see Carretta et al. 2010a; Lardo et al. 2011). In NGC 2808 we see the opposite case: the radial distributions are indistinguishable, while the RV distribution of Na-rich stars is much steeper than for Na-poor. According to a Kolmogorv-Smirnov (KS) test, the probability that the two subsamples are from the same parent distribution of RV is just 1.1 per cent, in excellent agreement with the result of the F test, so the observed difference in σ does not come from a difference in radial distribution (the probability that the velocity distribution of Na-rich and Na-poor stars of NGC 2808 are drawn from the same parent population decreases to 0.2% if [Na/Fe] = 0.4 is adopted as threshold). However the upperleft hand panel of Fig. 4 provides an interesting hint in this sense. It can be readily appreciated that nearly 90 percent of the Na-rich subsample lies at negative velocity, in the reference system of the cluster (in the following RV or V_r have always to be intended as expressed in the reference system of the clusters, i.e. with the systemic velocity of the clusters subtracted). This is confirmed by looking at the mean velocities of the two samples, which are observed to differ by  ~4.0 km s^-1.

In the uppermost panel of Fig. 5, it is apparent that the distribution of RV with radius separates into two branches around r ~ 5   r_c, as if the velocity distribution was bimodal at large radii. This is strongly suggestive of systemic rotation, as is indeed confirmed in Sect. 4.2. Moreover, it is clear that the large majority of the Na-rich stars belongs to only one of the two branches. In Sect. 4.2 we will show that the two branches corresponds to the two wings of the cluster rotation curve. Likely by mere chance, our sample contains more stars from the half of the cluster that is approaching than from the half that is receding. This asymmetry in the distribution of targets has been exacerbated in the Na-rich sample, enough to produce the significant difference detected by the F and KS tests (that assume no selection effects, i.e. even sampling) but still compatible with a chance occurrence.

In our view, there are two interesting conclusions that can be drawn from this case. First, it would be worth verifying this result with a larger and more evenly distributed sample. While it is likely that the observed effect is from the described rotation+sampling conspiracy, we cannot exclude that there is a real difference. If this were the case, it would have a striking impact on any scenario for the formation of this very peculiar cluster (D’Antona et al. 2005; Piotto et al. 2007; Bragaglia et al. 2010; Amaro-Seoane & Konstantinidis 2011). Second, it provides an example of the possible dangers connected with neglecting rotation in the analysis of velocity of stars in a GC, when the amplitude of the rotation (A_rot, see Sect. 4.2) is relatively high with respect to the dispersion (A_rot/σ₀ ≳ 0.2).

Fig. 5 Radial velocity in the cluster system as a function of distance from the cluster center, expressed in core radii units, for less studied clusters. Na-rich and Na-poor stars are plotted with different symbols. The dotted line marks the tidal radius of the K66 model that best fits the surface brightness profile, according to McLaughlin & van der Marel (2005). The continuous curves are the  ± 3σ profiles of the same models, normalized to the central σ listed by Harris (1996), approximately representing the envelope of the allowed velocities for the bound members of the clusters. The dashed line marks the half-light radius, taken from Harris (1996).

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3.1. Rotation and Na abundance

A distinctive prediction of the models for the formation of GCs with multiple populations by Bekki (2010, 2011) is that even if a very small fraction (s = 0.3 percent) of the kinetic energy of the gas forming the first generation (FG) of stars is in form of bulk rotation energy, stars in the second generation (SG) acquire significant rotation, much stronger than what remains in the FG. In particular, s values in the range 0.3–18.0 percent correspond to ratios of rotational velocity to velocity dispersion (V_rot/σ) from 0.75 to 2.5 for FG stars. Bekki (2010) concludes that “... the rotation of SG [stars, ndr] is due largely to dissipative accretion processes of AGB ejecta from FG with initially a small amount of rotation ...”. In Bekki’s model the formation of both generations of stars is essentially completed after a few 10⁸ yr from the formation of the very first star, so, this possible difference in the rotation of different generations of cluster stars should also have been largely smoothed out by subsequent dynamical evolution, during the  >10 Gyr of a cluster life (see Decressin et al. 2008). Nevertheless, dedicated simulations are required to check in detail whether some fossil of such difference may still be observable in GCs at the present epoch, given the initial conditions considered in Bekki (2010). On the other hand, significant rotation of the cluster as a whole is a general outcome of the merging of two clusters (Makino et al. 1991), another channel that has been suggested as playing a role in the formation of multiple populations GCs (Carretta et al. 2011; Amaro-Seoane & Konstantinidis 2011, and references therein).

We searched for differences in the rotation amplitude between Na-rich ([Na/Fe]  ≥ 0.4) and Na-poor ([Na/Fe] < 0.4) stars within each program cluster using the same kind of analysis adopted and described in Sect. 4.2, below, to look for rotation in the total samples. We cannot reach definitive conclusions from our data, since this kind of analysis would require larger samples to allow a fully reliable study of subsamples, and we lack coverage of the innermost regions of the clusters, where most of the SG population is expected to reside in Bekki’s model. In addition, rotation amplitudes are intrinsically small in GCs (L09, L10a,b), and we were forced to consider only the [Na/Fe] = 0.4 threshold to avoid too poorly populated Na-rich subsamples. It is also worth noting that Na features are among the most prominent ones for metal-poor stars in the spectral range covered by our data. Therefore stars with low Na abundance (i.e. weak Na features) may have slightly larger uncertainties in RV than stars with high Na abundance.

We simply report that we do not find any significant difference (i.e.  ≳ 2 km s^-1) in mean rotation amplitude (A_rot, see below) between Na-rich and Na-poor stars for cluster having at least 20 stars per subsample⁷. Furthermore, any marginal difference is in the opposite sense with respect to Bekki’s model expectations; i.e., in general, Na-poor samples tend to have larger rotation amplitudes than Na-rich samples.

In NGC 6171 the Na-poor group displays an amplitude of 5.5 km s^-1, but the Na-rich one only 0.5 km s^-1. The two subsamples contain only 20 and 13 stars, thus we should not trust this result at face value. In NGC 7078 the Na-poor group displays an amplitude of 6.5 km s^-1, and the Na-rich one just 1.0 km s^-1, but the two subsamples contains only 20 and 31 stars; in addition, this is the cluster having the worst quality RV estimates in our survey. It is also worth noting that Na features are among the most prominent ones for very metal-poor stars in the spectral range covered by our data. Therefore stars with low Na abundance (i.e. weak Na features) may have larger uncertainties in RV than stars with high Na abundance, which may be relevant in the case of NGC 7078 where the overall RV uncertainties are quite large.

Finally a brief comment is needed on the clusters showing signs of Na-abundance vs. σ correlation. The samples for NGC 6441 and NGC 6388 are as small as the one for NGC 6171; however, the Na-rich and Na-poor groups display very similar rotational patterns in both clusters (see below). In NGC 2808, where the Na-rich and Na-poor groups contain 41 and 82 stars, respectively, Na-poor stars display a larger rotational amplitude than Na-rich stars (A_rot ≃ 4.5 km s^-1 and A_rot ≃ 2.0 km s^-1, respectively). This is likely accounted for by the fact that the majority of Na-rich stars lie mainly on one of the rotation curve wings, as anticipated above and discussed in Sect. 4.2.

4. Dispersion and rotation for the less studied clusters

There are a few clusters among those listed in Table 1 for which the present sample can provide a significant improvement over existing kinematic data and analysis. For NGC 2808, NGC 6388, and NGC 6441, only estimates of σ₀ from integrated spectra are available. For NGC 5904, in addition to the integrated measure, a sample of RV for 46 individual stars was considered by Rastorguev & Samus (1991), still significantly smaller than our sample (136 stars). Finally, NGC 6254 lacks any integrated measure, the only existing estimate of the velocity dispersion for this cluster coming from RVs for 25 stars from Rastorguev & Samus (1991) in the range 0.6r_c − 6.9r_c, while our sample includes 147 stars. In the following we briefly discuss the properties of the RV distributions in these clusters, providing new estimates of σ₀ if we consider the case worth it (see below).

In Fig. 5 we show the RV distribution in the cluster system as a function of projected distance from the cluster center, expressed in units of core radius. We superposed the  ± 3.0σ contour of the K66 model that is found by MvM05 to best fit the surface brightness profile of the clusters, as a reference. The position of r_h and r_t are also reported⁸. Na-rich and Na-poor stars are plotted with different symbols.

At first glance, Fig. 5 reveals both (a) the (already noted) poor sampling of the innermost regions of the clusters provided by our data, and (b) the wide variety in the radial sampling from cluster to cluster. For example, the NGC 6254 sample has a significant fraction of stars within r_h and barely reaches 0.5r_t, while the innermost stars of the NGC 6388 and NGC 6441 lie around  ≳ 2r_h, and the farthest are far beyond the tidal radius. As discussed in the introduction our samples are not best suited to a full characterization of the clusters kinematics. Still, in several cases, they are competitive with the best samples available in the literature, and, for the five clusters considered in this section, they are clearly superior to other available samples.

The adopted K66 models appear to provide a reasonable description of the observed velocity distribution for NGC 6254, NGC 2808, and NGC 5904. In the last two cases there are some stars lying beyond the  ± 3.0σ contour of the best-fit model. This may be due to several trivial factors: uncertainty in the adopted value of σ₀ providing the normalization constant of the model profile, uncertainties in the parameters of the best-fit model and/or limitations in the available data for the surface brightness profile (see, for example Correnti et al. 2011, and references therein), and inadequacy of the K66 model in representing the kinematics of the clusters (e.g. rotation, anisotropy, see MvM05). In addition to these issues, recent detailed studies have pointed out that a large fraction of unbound (due to Galactic tides) cluster stars can contaminate the velocity dispersion profiles of actual GCs well inside their Jacobi radius. For example, in the M = 10⁴   M_⊙ models considered by Küpper et al. (2010), unbound stars are found to dominate the samples beyond a radius  ≃ 0.5 of the Jacobi radius.

The NGC 6388 and NGC 6441 samples are too sparse to let us draw firm conclusions. At face value they show a pretty flat dispersion curve over the considered radial range. This, along with the significant rotation (see below) and the presence of several members beyond the K66 tidal radius, may be suggestive of strong effects from Galactic tides (Muñoz et al. 2008; Sollima et al. 2009; Küpper et al. 2010, and references therein; see also the discussion in Sect. 5, below). The large number of members beyond the tidal radius seen in NGC 6441 may simply be due to the inadequacy of K66 to describe the outer regions of clusters that is discussed in detail by MvM05. These authors found that in most cases spherical and isotropic W75 models (more extended than K66 ones) provide the best overall fit of cluster observed light profiles. This is actually the case for NGC 6441, while for NGC 6388, K66 is better. The tidal radii for the best-fit W75 models are 4.2 times and 6.1 times larger than their K66 counterparts, for NGC 6388 and NGC 6441, respectively. All the stars in our samples would thus lie well within the W75 tidal radius of the clusters.

4.1. New σ₀ estimate for NGC 5904

Fig. 6 Comparison of the observed velocity dispersion profile for NGC 5904 as derived from our data (filled circles with error bars) and the prediction of the K66 model that best fits the SB profile, according to MvM05, with σ0 taken from H96 (thick continuous line). An alternative value of σ0, providing significantly better representation of the observed profile, is proposed (σ0 = 7.5 km s-1, from our own fit, dashed line).

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In the comparisons with other self-gravitating systems, the kinematic properties of a GC are usually summarized by a single number, i.e. the central velocity dispersion σ₀ (Djorgovski 1995; Bellazzini et al. 1998). This is the number usually reported in GC catalogs (PM93, H96), so it may be useful to provide refinements of such estimates or to confirm existing estimates on significantly sounder basis, when possible.

We used our data to produce velocity dispersion curves for the less studied clusters listed above, in the same way as described in B08, using jackknife resampling to compute uncertainties. We compared the observed curves with the predictions of the K66 models plotted in Fig. 5, normalized with the σ₀ listed in H96, to check that our new results are compatible with these values.

The agreement is acceptable or satisfying for NGC 6388, NGC 2808, and NGC 6254, so we confirm the σ₀ estimate reported in the literature for these clusters. From the sparse sample of NGC 6441 we were able to obtain only one point of the dispersion curve within the tidal radius of the best-fitting K66 model; this point is compatible with the listed value of σ₀. Outside of r_t the velocity dispersion remains fairly large (σ ~ 10 km s^-1).

A direct comparison of the observed velocity dispersion profiles with the predictions of the K66 models is plotted in Fig. 6 for NGC 5904, the only case where we found a mismatch between the current normalization of the velocity profile of the model and our data. The value listed by H96 (σ₀ = 5.5 ± 0.4 km s^-1, see Table 1 and PM93 for the original data sources) is clearly too low to match the observed dispersion curve. The adopted σ₀ = 7.5 ± 1.0 km s^-1  instead provides a satisfying fit, and we propose this value as a new, more robust estimate of the central velocity dispersion for this cluster. It has to be recalled that the accuracy of this estimate also depends on how good and appropriate the adopted K66 models are (see MvM05).

Fig. 7 Rotation in NGC 2808, NGC 6388, and NGC 6441. The plots display the difference between the mean velocities on each side of a cluster with respect to a line passing through the cluster center with a position angle PA (measured from north to east, north = 0°, east = 90°), as a function of the adopted PA. The adopted line coincides with the projected rotation axis. The continuous line is the sine law that best fits the observed pattern. The vertical scale used for NGC 6441 is larger, to accommodate the strong rotation signal. It is also worth noting that even limiting the NGC 6441 sample to the 21 stars lying within the tidal radius (see Fig. 5) the rotation pattern is very similar, with Arot ≃ 11 km s-1 and PA0 ≃ 225°.

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4.2. Rotation

Globular clusters are generally considered as classical examples of pressure-supported systems, in which rotation is nonexisting or negligible. The classical case of rotating GC is ω Cen, which has been considered as very peculiar in many aspects for a long time, and it displays a large-amplitude (~8 km s^-1) rotation pattern coupled with high isophotal ellipticity (Merritt et al. 1997; van de Ven et al. 2006; Sollima et al. 2009). However, recent studies based on large samples are revealing that rotation of typical amplitude 2 − 4 km s^-1 is far from uncommon in Galactic GCs (see Côté et al. 1995; Anderson & King 2003; van den Bosch et al. 2006, L09, L10a,b). Rotation amplitudes detected from RV samples are just lower limits to the true 3D amplitude, because of projection onto the plane of the sky. This may support the suggestion by MvM05 that W75 models may be more appropriate for describing actual GCs, as these models can account for rotation (see Sollima et al. 2009, for a recent application; however, Wilson’s models adopted by MvM05 do not include rotation).

We used our sample to search for rotation in all the clusters for which this characteristic has not been considered in previous studies⁹. In addition to these, we also analyzed NGC 1851 and NGC 1904, whose rotation has been considered by Scarpa et al. (2011), but only separated in two radial bins, while we aim at global properties to make proper comparisons among clusters. Our results are in good agreement with those by Scarpa et al. (2011). To get a rotation amplitude value that is homogeneous with the other clusters, we also studied the case of NGC 7078, whose kinematics have been analyzed in much greater detail by van den Bosch et al. (2006). We limit our analysis to rotation patterns that can be detected from radial velocities, since the data on rotation in the plane of the sky are only available for a handful of clusters (Anderson & King 2003; van de Ven et al. 2006; van den Bosch et al. 2006).

	Fig. 8 The same as Fig. 7 but for NGC 1851, NGC 1904, NGC 5904, NGC 6254, NGC 6171, NGC 6397, NGC 6838, and NGC 7078. The kinematics of some of these clusters has been studied with samples larger than ours, still they lack a study of rotation (NGC 6171, NGC 6397, NGC 6838) or an estimate of the rotation amplitude homogeneous with those obtained here.
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To look for rotation we used the same method as was adopted by Côté et al. (1995), Pancino et al. (2007), L09, and L10a,b. For any given cluster, we divided the sample in two, choosing stars lying on the opposite side of a line passing from the cluster center, and we computed the difference in mean RV between the two subsamples. Then we rotate the dividing line by a fixed amount (10° or 20°, depending on the number of stars of the considered sample) and repeated the computation. Recording the difference in the mean RV for each position angle (PA) of the dividing line we can plot the first as a function of the second: a coherent sinusoidal pattern is a clear sign of rotation. In the adopted approach PA is defined to increase anti-clockwise in the plane of the sky from north (PA = 0°) toward east (PA = 90°). We fit the observed patterns with the simple sine law: (1)where Φ = 270°−PA₀, and PA₀ is the position angle of the dividing line corresponding to the maximum rotation amplitude (in degrees), coinciding with the rotation axis, and A_rot is two times the actual mean amplitude (in  km s^-1; see L10a). However, it must be noted that, as the  ⟨ RV ⟩  difference is averaged over the full range of radius covered by the sample, A_rot/2 should be an underestimate of the maximum rotation amplitude, which should be the most informative global rotation parameter (Meylan & Heggie 1997), since the amplitude generally varies significantly with distance from the cluster center (see, for example, the case of ω Cen Sollima et al. 2009). By inspecting some well-populated rotation curves of GCs, we noted that A_rot is a reasonable proxy for the actual maximum amplitude (see Pancino et al. 2007); in the following we use this value as an estimate of the rotation amplitudes and, consequently multiply by two the values reported by L10b, to make the two sets of measures fully homogeneous. We explored the reliability of the derived parameters by repeating the analysis on subsamples and by comparing it with external samples (e.g. for clusters in common with L11), and we concluded that the estimates of A_rot are fairly robust (we assume a typical 1σ uncertainty of 0.5 km s^-1 for the largest samples, similar to L10b), while PA₀ is quite sensitive to the adopted sample and should be considered as uncertain at the  ± 30° level in the best cases.

The results of the analysis are displayed in Figs. 7 and 8. It is evident that the considered clusters cover a wide range of rotation properties, from no rotation (NGC 6397) to an amplitude of more than 10 km s^-1 (NGC 6441). It is interesting to note that three among the most peculiar clusters in terms of multiple populations, NGC 2808, NGC 6388, and NGC 6441, display particularly strong rotation patterns, possibly hinting at a similarity with some galactic nuclei (Seth et al. 2008). Other clusters for which we detect for the first time a significant amplitude of rotation are NGC 5904 and NGC 6171. The significant amplitude found for NGC 7078 agrees with the results by van den Bosch et al. (2006).

Fig. 9 Rotation curves for NGC 2808, NGC 6388, and NGC 6441. Filled and open symbols are adopted for Na-rich and Na-poor stars, respectively. Left panels: RV in the system of the cluster as function of distance from the center projected onto the axis perpendicular to the best-fit rotation axis found in Figs. 7 and 8. Stars inside and outside the tidal radius are plotted with different symbols for NGC 6441 and NGC 6388. All the stars in the NGC 2808 sample lie within the tidal radius on the cluster. Right panels: comparison of the cumulative RV distributions of stars having X(PA0) > 0.0 (continuous lines) and X(PA0) < 0.0 (dotted lines). The probability that the two distributions are drawn from the same parent population (according to a KS test) is reported in each panel. We show rotation curves only for the two clusters having PKS < 10% plus NGC 2808.

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In Fig. 9 we show the rotation curve for the cases of NGC 2808, NGC 6388, and NGC 6441, i.e. the distribution of RV as a function of the projection of the star position on the axis perpendicular to the axis of rotation [X(PA₀)]. In the righthand panels, the RV distribution of stars lying on opposite sides with respect to the rotation axis are compared. When there is no rotation, the two distributions should be indistinguishable, while with significant rotation a shift should be apparent. The degree to which the two distributions differ also depends on the ratio between rotation and velocity dispersion and on the actual shape of the rotation curve. In the considered cases the comparison is not fully conclusive, given the small samples under consideration. A KS test states that it is relatively unlikely (but clearly not impossible) that the observed patterns may emerge by chance from nonrotating systems. For NGC 2808 we had the opportunity to fully confirm the result presented here with a much larger, still unpublished sample of RV estimates (more than 800 stars, Bragaglia & Carretta, priv. comm.). The rotation pattern observed in NGC 1851 has also been independently confirmed with an unpublished sample of  ~100 HB stars observed within another program (Gratton & Lucatello, priv. comm.).

Figure 9 deserves a couple of further comments:

• In the upper lefthand panel of Fig. 9 the subtle selection effect of the uneven spatial sampling in NGC 2808 can be appreciated. The effect of rotation (that favors a certain range of velocities for stars in a given wing of the rotation curve) coupled with low-number statistics may well be at the origin of the correlation between Na-abundance and velocity dispersion discussed above. In fact, in each wing the velocity dispersion is lower than in the two wings considered as a whole.

• It is interesting to note that in NGC 6441 stars within and outside the tidal radius seem to trace the same rotation pattern. The kind of solid body rotation extending to large distances from the cluster center that is hinted at in Fig. 9 may be suggestive of a velocity gradient induced by tidal stripping (see Muñoz et al. 2008; Bellazzini et al. 2008; Sollima et al. 2009, discussion and references therein).

We have to stress again that the results presented in this section may also suffer from biases associated with the dimension of the samples and with the radial distribution of sample stars. However, most of the stars at relatively large distances from the cluster centers may not be a strong concern for detecting rotation, since it is expected that the highest rotation amplitudes are reached relatively far from the center (Merritt et al. 1997; Scarpa et al. 2011). Moreover, the adopted technique is not expected to be particularly sensitive, since any rotation curve is strongly smoothed out in the simple average velocity of two halves of the clusters: as a result, the detected signals should be considered as quite robust and homogeneous.

5. Summary and discussion

	Fig. 10 The ratio between the amplitude of the rotation Arot to the central velocity dispersion σ0 is plotted versus various other parameters. The clusters that appear to lie at odd positions with respect to the main trends are labeled. In the rightmost panel of the lower row, clusters having [Fe/H]  ≥  − 1.0 are plotted as filled circles.
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We used the radial velocity estimates obtained from a large spectroscopic survey (aimed at the study of the Na-O anticorrelation in GCs) to study the kinematics of the surveyed clusters, with the main aim of looking for correlations between kinematics and chemical abundance of elements involved in the anticorrelation issue. With all the limitations associated with the relatively small samples and the uneven radial distribution of target stars within each cluster, the data considered here allow the exploration of this interesting issue for the first time. By internal and external comparisons we have demonstrated that the typical uncertainty on individual RV estimates is smaller than 1 km s^-1.

In general, we did not find any evidence of correlation of Na abundance with velocity dispersion or rotation within each cluster. A possible decrease in velocity dispersion for [Na/Fe]  ≳ 0.4 for the peculiar clusters NGC 6388 and NGC 6441, in broad agreement with the expectations from the models by Bekki (2011), clearly requires larger datasets to be confirmed or disconfirmed. A statistically significant decrease in velocity dispersion for [Na/Fe]  ≳ 0.4 for NGC 2808 is found to likely come from an uneven spatial distribution of the target stars in this cluster.

We investigated in slightly deeper detail the cases of the clusters whose kinematics were previously studied in the literature with smaller samples than ours. We confirm (or provide support for) the central velocity dispersion estimates reported in the literature for NGC 6388, NGC 2808, and NGC 6254. We provide a revised estimate of the central velocity dispersion for NGC 5904.

Finally we looked for systemic rotation in the clusters that were lacking such analysis in the literature (or had been studied with different methods than that adopted here). We found that the considered clusters cover a remarkable range of rotational amplitudes, from  ~0 km s^-1 to  ~13 km s^-1. NGC 5904, NGC 6171, NGC 2808, NGC 6388, and NGC 6441 show especially strong rotation patterns (A_rot ≳ 2.5 km s^-1).

In Table 3 we list homogeneous σ₀ and A_rot estimates collected from this work and other sources in the literature (mainly L10b), together with other relevant cluster parameters from various sources (mainly from H96). We added to our original sample ω   Cen (NGC 5139), M54 (NGC 6715), M22 (NGC 6656), and M53 (NGC 5024) for which we had all (or most of) the relevant data in the same scales adopted here from other sources (L10b; B08; Carretta et al. 2010b; Pancino et al. 2007). It is interesting to check that the rotation properties of the clusters do correlate with some other characteristics, as this is the largest collection of rotational amplitudes for Galactic GCs currently available (see Meylan & Heggie 1997, for a summary of the data available circa one decade ago). Before going on with the analysis it may be worth recalling that projection effects should be at work, and the listed A_rot are only estimates of the amplitude of the projected rotation pattern, thus lower limits of the actual rotation amplitude. However, in Appendix A we show that A_rot is a reasonable proxy for the true amplitude, in a statistical sense (see also Chandrasekhar & Münch 1949).

As the most informative parameter, we use the ratio between the rotation velocity V_rot, here represented by A_rot, and the central velocity dispersion σ₀. In Fig. 10 we show scatter plots of A_rot/σ₀ vs. the inter quartile range (IQR), a parameter defined by Carretta (2006) to measure the extension of the Na-O distribution in clusters, the cluster ellipticity, the absolute integrated V magnitude (M_V), the iron abundance (metallicity, [Fe/H]), the classical HB morphology parameter ¹⁰ (Lee 1990), the logarithm of the central luminosity density (log ρ₀), the absolute value of the distance from the Galactic plane (|Z|), and the distance from the Galactic center (R_GC).

The ratio A_rot/σ₀ does not display any clear correlation with M_V, ellipticity, logρ₀, |Z|, and R_GC. The lack of a connection with ellipticity may appear somehow surprising. However, it must be recalled that the two quantities may refer to different regions of the clusters, since it is hard to reliably estimate ellipticity at large distances from the cluster core. On the other hand, a hint of a trend with IQR is perceived. In general clusters with higher A_rot/σ₀ ratios have smaller IQR. Four of the five clusters lying on a nearly parallel sequence above the bulk of the other objects (at larger IQR for a given A_rot/σ₀ value) are among the most peculiar clusters, two of them also displaying a spread in the iron abundance. According to a two-tailed Student’s test, the probability that a Spearman rank correlation coefficient equal or larger (in absolute value) than the observed one (s =  −0.353) is produced by chance from uncorrelated quantities is P_t = 12.6 per cent, so the correlation cannot be considered as statistically significant (Press et al. 1992, see Table 4 for s and P_t for all the considered parameters). For this reason we refrain from any interpretation of this plot, which can be considered as a possible starting point for further analysis.

An interesting trend of A_rot/σ₀ is with the cluster metallicity: clusters with higher metallicity have greater fractions of ordered motion with respect to pressure support. In spite of the three outliers, the correlation is found to be remarkably significant by the same kind of Student test as used above, P_t = 1.5 per cent. Since larger metal content in a gas implies higher efficiency in energy dissipation by atomic transitions, the observed correlation, if confirmed, may hint at a significant role of dissipation in the process of cluster formation (see Bekki 2010, 2011).

The most significant correlation of A_rot/σ₀, however, is with the HB morphology (): the relevance of ordered motions with respect to pressure is stronger for clusters with redder HBs. The probability that the observed correlation arose by chance is negligible (P_t = 2 × 10^-5). It is well known that and [Fe/H] are correlated (since metallicity is the first parameter determining the HB morphology, see Lee 1990; Fusi Pecci et al. 1993; Gratton et al. 2010, and references therein), so it is likely that the correlation of one of the two parameters with A_rot/σ₀ is a secondary effect of the correlation with the other. We cannot provide a firm identification of the primary correlation; however, we note that for our sample the correlation of A_rot/σ₀ with (s =  −0.769) is much stronger than both that of A_rot/σ₀ with [Fe/H] (s = 0.492) and of with [Fe/H] (s = 0.661). As a result, the connection seems more direct with the HB morphology than with the metallicity¹¹. It is interesting to note that shows some degree of correlation (|s| ~ 0.3; not shown here) with other HB morphology parameters considered in Carretta et al. (2010a, like e.g., and/or estimates of Helium abundance (e.g. Y_max, Gratton et al. 2010), in the sense that clusters with larger and Y_max have lower A_rot/σ₀. These parameters, in turn, positively correlate with IQR that, as seen above, displays an anticorrelation with A_rot/σ₀. In summary, the overall observational scenario strongly suggests a significant link between the systemic rotation of the clusters and the processes that lead to the formation and evolution of the different generations of cluster stars, whose effects are likely imprinted (and most evident) in the current HB morphology (Fusi Pecci et al. 1993; D’Antona et al. 2005; Gratton et al. 2010, and references therein).

It should also be noted that the orbits of the most metal-rich (and HB-red) clusters are likely confined within the Galactic bulge, so they may be subject to stronger tides, possibly producing velocity gradients that can mimic rotation (see e.g., Muñoz et al. 2008). However, in this case one would expect to see a better correlation between cluster position and A_rot than with A_rot/σ₀, since the amplitude of the gradient should mainly depend on the orbital parameters. The Spearman rank correlation coefficients listed in Table 5 show that this is not the case; the correlation is poor also between A_rot and the orbital parameters of the clusters (R_per and Z_max from Dinescu et al. 1999; Casetti-Dinescu et al. 2007, see Table 5).

	Fig. 11 Arot vs. the four parameters displaying the strongest correlation with it (Table 5). In all cases, removing NGC 6441 from the sample has a negligible effect on the final value of Pt.
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On the other hand, A_rot displays significant correlations with , M_V, σ₀, and [Fe/H] (P_t < 1.0 percent, in all cases; see Fig. 11). Also in this case, the strongest and most significant correlation is, by far, with HB morphology, therefore A_rot seems strictly tied with intrinsic cluster parameters, not with their orbit or environment. Note that M_V and σ are also correlated between each other, both approximately tracing the cluster ranking in mass, but do not appear to correlate with [Fe/H] and/or . The only outlier of the correlations of A_rot with M_V and σ₀ is NGC 6441, which has a much larger A_rot for its M_V or σ₀ than do the other clusters of the sample. This may support the idea of a tidal origin for the strong velocity gradient observed in this specific cluster, as already suggested in Sect. 4.2. For the other clusters rotation is more likely of internal origin, possibly linked with the phase of cluster formation, with tides as a possible source of noise in the correlations. Removing NGC 6441 from the sample has a negligible effect on the Spearman coefficients and on the statistical significance of the correlations, as measured by P_t. We found two linear combinations of parameters displaying correlations with A_rot that are significantly stronger than all those with single parameters, and LC2 = M_V − 1.73[Fe/H]. The significance of both correlations is very high (P_t ≤ 10^-5). It is interesting to note that M_V (likely as a proxy of the total cluster mass) has been found to play a role in bi-variate correlations, both with some HB morphology parameters (Fusi Pecci et al. 1993; Recio-Blanco et al. 2006) and with parameters related to the anticorrelation phenomenon (Paper VII, Carretta et al. 2009b).

As typical of most exploratory studies, our analysis does not provide firm conclusions, but calls for further investigations and perhaps opens some new windows on the research on globular clusters. It is clear that a follow up of the possible chemistry-kinematics connection and of the rotation patterns detected here is necessary for NGC 2808 and, above all, for NGC 6388 and NGC 6441. The possible correlation between A_rot/σ₀ and IQR also deserves further study. This requires a considerable observational effort, e.g, to double the number of GCs with relatively large sample of Na abundances and RV estimates. The correlations between A_rot/σ₀, and [Fe/H] should be easier to verify and/or extend, since only large RV samples are required, with no need of detailed chemical abundance analysis of individual stars. The same is true for the correlations between A_rot and , M_V, σ₀, and [Fe/H]. These, together with those of A_rot/σ₀ with HB morphology and metallicity, are especially interesting since they are quite significant, from a statistical point of view, and far from trivial, since they indicate that rotation may be intimately linked with the internal physics of the clusters, and, possibly, with their origin.

Acknowledgments

This paper is dedicated to the memory of Robert T. Rood, whose contribution to the understanding of the Horizontal Branch phase of the evolution of low mass stars cannot be overstated. We acknowledge the financial support to this research by INAF through the PRIN-INAF 2009 grant CRA 1.06.12.10 (PI: R. Gratton).

References

Appendix A: The projected rotation amplitude as a tracer of the true rotation amplitude

To explore quantitatively the effect of projection on the distribution of observed rotation amplitudes of a population of GCs (or any other system whose inclination w.r.t. the plane of the sky i is unknown and unconstrained), we performed the following simulation. In a cluster with a true rotation amplitude A_true, we detect an observed rotation amplitude A_obs = A_truesin(i), where 0° ≤ i ≤ 90° (i = 0° corresponds to a cluster seen pole-on, i = 90° corresponds to a cluster seen “edge-on”, i.e. having A_obs = A_true).

Fig. A.1 Left panels: probability distribution of observing a rotation amplitude (Aobs) given a true value of the amplitude (Atrue) and a uniform distribution of inclination angles (i). Different tones of gray indicate different probability levels, from 8% (darkest gray) to 1% (lightest gray), in steps of 1%; white regions corresponds to probability below 1%. The continuous line is the Aobs = Atrue relation. In the upper panel Atrue values are drawn from a uniform distribution, in the lower panel they are drawn from a Gaussian distribution. The probability is estimated in square bins with sides of 1.0 km s-1 spaced by 0.25 km s-1 in both directions of the plane. Right panel: distribution of sin(i) for a uniform distribution of i.

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We simulated a population of 10⁶ clusters whose inclination is drawn from a uniform distribution, since there is no preferred value for i. We explored two different distributions of A_true: a uniform distribution in the range 0.0 km s^-1  ≤ A_true ≤ 10.0 km s^-1, and a Gaussian distribution with mean  ⟨ A_true ⟩  = 4.0 km s^-1 and σ = 2.0 km s^-1. In the lefthand panels of Fig. A.1 we plot the density distributions obtained in the two cases in the plane A_true vs. A_obs. It is quite clear that the regions close to the A_obs = A_true relation display the highest probability density. Independently of the assumed distribution of A_true, for a uniform distribution of inclinations, observed rotation amplitudes are thus more likely close to the true value.

This is due to the simple fact that the sinus function maps a uniform distribution of angles i between 0° and 90° into a distribution of sin(i) that is strongly peaked toward sin(i) = 1.0, as shown in the upper righthand panel of Fig. A.1. In particular sin(i) ≥ 0.5 in  ≃ 66% of the cases, sin(i) ≥ 0.7 in  ≃ 50% of the cases, and sin(i) ≥ 0.9 in  ≃ 28% of the cases, while sin(i) < 0.2 in just  ≃ 12% of the cases. We can therefore conclude that A_obs is a reasonable proxy for A_true in a statistical sense. This supports the idea that the observed correlations between A_rot or A_rot/σ₀ and, e.g., M_V, [Fe/H] or , may trace physical correlations between these parameters and the true rotational amplitude.

All Tables

All Figures

	Fig. 1 Upper panel: comparison between RVs estimated from spectra obtained with the HR13 and HR11 grisms. Different symbols correspond to different clusters. The continuous line is drawn at a typical value for the mean difference (ΔVr =  −0.5 km s-1), and the dotted lines enclose the  ± 2σ range about the mean, where a typical value of σ = 0.7 km s-1 has been adopted (see Table 1). Lower panel: comparison with the external dataset by L11 for two representative clusters, NGC 104 (filled circles) and NGC 6218 (empty circles). The continuous line marks ΔVr = 0.0 km s-1, the dotted lines enclose the  ± 2σ range. The fraction of stars lying within  ± 2σ is also reported [F(Δ < 2σ)].
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In the text

	Fig. 2 Velocity dispersion as a function of Na abundance for NGC 104, NGC 2808, NGC 288, NGC 1851, NGC 1904, NGC 3201, NGC 4590, and NGC 5904. Larger filled squares indicate cases where one star has been clipped from the sample because of an RV value more than 3 − σ from the mean. Only estimates obtained from  ≥ 10 stars (after clipping) are plotted. The vertical scale is different for NGC 104 and NGC 2808, to accommodate for the larger dispersion of these clusters.
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In the text

	Fig. 3 The same as Fig. 2 for the remaining clusters of our sample. The vertical scale is different for NGC 6838 and NGC 6441 to accommodate the larger dispersion of these clusters.
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In the text

	Fig. 4 Comparison of cumulative distributions for Na-rich (red continuous line) and Na-poor (blue dotted line) for NGC 2808 (upper panels) and NGC 6752 (lower panels). Left panels: distributions of the radial velocity in the cluster system. Right panels: distributions of the distances from the cluster center. The probability that the Na-rich and Na-poor populations are drawn from the same parent population, according to a Kolmogorov-Smirnov test, is reported in the lower right corner of each panel. The adopted threshold between Na-poor and Na-rich stars is [Na/Fe] = 0.5.
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In the text

	Fig. 5 Radial velocity in the cluster system as a function of distance from the cluster center, expressed in core radii units, for less studied clusters. Na-rich and Na-poor stars are plotted with different symbols. The dotted line marks the tidal radius of the K66 model that best fits the surface brightness profile, according to McLaughlin & van der Marel (2005). The continuous curves are the  ± 3σ profiles of the same models, normalized to the central σ listed by Harris (1996), approximately representing the envelope of the allowed velocities for the bound members of the clusters. The dashed line marks the half-light radius, taken from Harris (1996).
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In the text

	Fig. 6 Comparison of the observed velocity dispersion profile for NGC 5904 as derived from our data (filled circles with error bars) and the prediction of the K66 model that best fits the SB profile, according to MvM05, with σ0 taken from H96 (thick continuous line). An alternative value of σ0, providing significantly better representation of the observed profile, is proposed (σ0 = 7.5 km s-1, from our own fit, dashed line).
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In the text

	Fig. 7 Rotation in NGC 2808, NGC 6388, and NGC 6441. The plots display the difference between the mean velocities on each side of a cluster with respect to a line passing through the cluster center with a position angle PA (measured from north to east, north = 0°, east = 90°), as a function of the adopted PA. The adopted line coincides with the projected rotation axis. The continuous line is the sine law that best fits the observed pattern. The vertical scale used for NGC 6441 is larger, to accommodate the strong rotation signal. It is also worth noting that even limiting the NGC 6441 sample to the 21 stars lying within the tidal radius (see Fig. 5) the rotation pattern is very similar, with Arot ≃ 11 km s-1 and PA0 ≃ 225°.
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In the text

	Fig. 8 The same as Fig. 7 but for NGC 1851, NGC 1904, NGC 5904, NGC 6254, NGC 6171, NGC 6397, NGC 6838, and NGC 7078. The kinematics of some of these clusters has been studied with samples larger than ours, still they lack a study of rotation (NGC 6171, NGC 6397, NGC 6838) or an estimate of the rotation amplitude homogeneous with those obtained here.
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In the text

	Fig. 9 Rotation curves for NGC 2808, NGC 6388, and NGC 6441. Filled and open symbols are adopted for Na-rich and Na-poor stars, respectively. Left panels: RV in the system of the cluster as function of distance from the center projected onto the axis perpendicular to the best-fit rotation axis found in Figs. 7 and 8. Stars inside and outside the tidal radius are plotted with different symbols for NGC 6441 and NGC 6388. All the stars in the NGC 2808 sample lie within the tidal radius on the cluster. Right panels: comparison of the cumulative RV distributions of stars having X(PA0) > 0.0 (continuous lines) and X(PA0) < 0.0 (dotted lines). The probability that the two distributions are drawn from the same parent population (according to a KS test) is reported in each panel. We show rotation curves only for the two clusters having PKS < 10% plus NGC 2808.
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In the text

	Fig. 10 The ratio between the amplitude of the rotation Arot to the central velocity dispersion σ0 is plotted versus various other parameters. The clusters that appear to lie at odd positions with respect to the main trends are labeled. In the rightmost panel of the lower row, clusters having [Fe/H]  ≥  − 1.0 are plotted as filled circles.
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In the text

	Fig. 11 Arot vs. the four parameters displaying the strongest correlation with it (Table 5). In all cases, removing NGC 6441 from the sample has a negligible effect on the final value of Pt.
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In the text

	Fig. A.1 Left panels: probability distribution of observing a rotation amplitude (Aobs) given a true value of the amplitude (Atrue) and a uniform distribution of inclination angles (i). Different tones of gray indicate different probability levels, from 8% (darkest gray) to 1% (lightest gray), in steps of 1%; white regions corresponds to probability below 1%. The continuous line is the Aobs = Atrue relation. In the upper panel Atrue values are drawn from a uniform distribution, in the lower panel they are drawn from a Gaussian distribution. The probability is estimated in square bins with sides of 1.0 km s-1 spaced by 0.25 km s-1 in both directions of the plane. Right panel: distribution of sin(i) for a uniform distribution of i.
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In the text