A&A 487, 453-460 (2008)
DOI: 10.1051/0004-6361:200809600

The bright galaxy population of five medium redshift clusters[*]

I. Color-magnitude relation, blue fractions, and visual morphology

B. Ascaso1 - M. Moles1 - J. A. L. Aguerri2 - R. Sánchez-Janssen2 - J. Varela1

1 - Instituto de Astrofísica de Andalucía-CSIC, Camino Bajo de Huetor 50, CP 18008 Granada, Spain
2 - Instituto de Astrofísica de Canarias, C/ via Láctea S/N CP La Laguna, Spain

Received 18 February 2008 / Accepted 28 May 2008

Aims. Using data from five clusters of galaxies within the redshift range $0.15 \leq z \leq 0.25$, imaged with the Nordic Optical Telescope (NOT) in the central $\approx$1 Mpc2 in very good seeing conditions, we have performed an exhaustive inspection of their bright galaxy population. That range of redshift, where only a small amount of data with the required resolution and quality is available, is particularly important for the understanding of the formation and evolution of clusters of galaxies.
Methods. We have inspected the color-magnitude relation (CMR) for those clusters and measured the blue fraction of galaxies in their cores to check for evidence of evolution as found in other works. Visual classification of the galaxy morphology has been performed and the morphology-radius relation examined.
Results. We have not found signs of evolution either in the slope of the CMR or in the blue fraction of galaxies. A diversity of situations regarding those parameters and in the morphological mixing has been noticed, with two out of five clusters containing a dominant late-type core population. The cluster A1878 stands out as some of its properties differ from those of the other clusters in the sample.
Conclusions. No clear signs of evolution appear in our analysis. The data support the view that the morphology and the stellar content of the galaxies in our clusters already have been settled at  $z \sim 0.2$. Only the fraction of interacting galaxies in the clusters appear to be larger than in clusters like Coma, although the number of clusters in the sample is too small to give a definitive conclusion.

Key words: cosmology: observations - galaxies: clusters: general - galaxies: fundamental parameters

1 Introduction

Clusters of galaxies are the largest structures in the Universe that are gravitationally bounded. They are crowded with hundreds to thousands of galaxies. Numerous studies have been devoted to the formation of clusters of galaxies. However, two main scenarios still remain. On the one hand, we have the monolithic scenario in which the clusters were formed first (Bower et al. 1998) and on the other, we have the hierarchical scenario (De Lucia & Blaizot 2007b; Kauffmann et al. 1994), in which the galaxies were formed at the outset. The monolithic scenario implies that the galaxies do not undergo substantial transformations after the cluster collapse (Merritt 1984) while the hierarchical scenario would imply that the environmental effects and interactions are transforming the galaxy population due to mechanisms that were operational until recent epochs, such as harassment (Moore et al. 1996), gas-stripping (Gunn & Gott 1972; Quilis et al. 2000), starvation (Bekki et al. 2002), or merging (Gerhard & Fall 1983; Aguerri et al. 2001; Eliche-Moral et al. 2006).

Likewise, the evolution of the galaxy population in clusters of galaxies has been broadly studied in many works. Some of the results found to date are the lower fraction of lenticular galaxies and the larger fraction of late type galaxies found in the cores of higher redshift clusters (Fasano et al. 2000; Dressler et al. 1997). The possible evolution of the slope of the color-magnitude relation (CMR) has also been widely explored (De Lucia et al. 2007a; Driver et al. 2006; Mei et al. 2006; López-Cruz et al. 2004). The agreed result is that the CMR does not change with redshift at least up to redshift $z \sim 1$. This feature is interesting in itself because it gives information about the metallicity and age of the galaxy population (Kodama 1999).

Another attribute that is considered in the context of the evolution of clusters of galaxies is the blue fraction of the galaxy population in clusters. In the early work by Butcher & Oemler (1984), an increase of this blue fraction with redshift was found for clusters up to redshift $\approx$0.5. That fact indicates that the galaxy population would be evolving. However, as shown by Aguerri et al. (2007), that variation would happen only for a limited redshift range. They studied a large sample of SDSS clusters up to redshift $z\leq 0.1$ and did not see any significant change of the blue fraction with the redshift. Therefore, exploring the next redshift range, $0.1 \la z \la 0.3$, would be needed to clarify the situation, since several works have explored and noticed the Butcher-Oemler effect in samples of clusters at lower (De Propris et al. 2004) and higher (De Lucia et al. 2007a) redshift.

Few works have been dedicated to study the morphology of the galaxy population at $z\approx 0.2$. Morphological studies generally have been confined to rather local samples, in part due to the need to establish a visual classification (Fasano et al. 2000; Dressler 1980) and more generally, to the difficulties in obtaining deep and high-resolution images for relatively large fields. Some of these studies have tried to establish an automatic morphological classification by inspecting the galaxy surface brightness and main structural parameters. Nevertheless, those samples often have been preselected to be only late type (de Jong 1996; Graham & de Blok 2001) or early type (Graham & Guzmán 2003). As a consequence, the present number of clusters that have been studied in that redshift range is small (Fasano et al. 2002; Trujillo et al. 2001; Fasano et al. 2000).

That range of redshift, however, should be inspected to link the results found for local clusters and for more distant objects that can be explored with the Hubble Space Telescope (HST). There is much evidence indicating that some properties of the clusters and their galaxies could change between the local and $\sim$0.4 redshift ranges.

In the present work we have studied five clusters of galaxies in a range of redshift from 0.15 to 0.25, observed with NOT at La Palma in two bands: Gunn-r and Bessel B, under very good seeing conditions. The clusters presented in this paper were considered by Fasano et al. (2002,2000) for their study of morphological mixing. They found that, for galaxies with $M_{V}\leq -20$, the fraction of S0 galaxies was lower for higher z clusters. Here we have analyzed the main characteristics of the bright galaxy population in the central part of those five clusters. We are interested in the possible evolution with z of properties of the galactic populations such as the CMR, the fraction of blue galaxies or the radial distribution of the different (visually determined) morphological types. We have used as templates at lower redshift the results obtained for galaxy clusters at $z \leq 0.12$ by De Propris et al. (2004) for comparison. The analysis of the surface brightness distribution and quantitative morphology of the galaxies will be presented in a forthcoming paper, (Ascaso et al. 2008, in preparation).

The structure of this paper is as follows. In Sect. 2 we present the data, including a brief description of the cluster environment and explain the observations and the reduction process. In Sect. 3, we describe how the galaxies were detected and extracted. Section 4 is devoted to the study of the color-magnitude diagrams and the Butcher-Oemler effect. Section 5 is dedicated to the study of the morphology of the galaxies from a qualitative point of view. We have considered several aspects such as the morphology-radius relation, the concentration parameter and the frequency of interaction systems in our sample. We present the discussion and conclusions in Sect. 6. Throughout the paper we have adopted the standard $\Lambda$CDM cosmology with H0=71 km s-1 Mpc-1, $\Omega_{\rm m}=0.27$ and $\Omega_{\Lambda}=0.73$.

2 Observations, data reduction and description of the selected clusters

Two of us (M.M. and J.A.L.A.) imaged five galaxy clusters with the 2.5 m Nordic Optical Telescope (NOT) located at the Roque de Los Muchachos Observatory (La Palma). The observations were taken with the Stand Camera, with a field of view of $3' \times 3'$, a plate scale of 0.176''/pix, a gain of 1.69 e-/ADU and a readout noise of 6.36 e-. All images were taken under photometric sky conditions and very good seeing (between 0.5'' and 0.8'').

The clusters were observed through two broad-band filters: Gunn-r' (r) and Bessel B (B). At least two exposures for each field in each filter were usually taken, allowing us to clean the combined images of cosmic-rays and spurious events. The data reduction and calibration was performed as presented in Fasano et al. (2002). Here we summarize the basic steps of the data reduction process; for more information we refer the reader to Fasano et al. (2002).

The bulk of the data reduction of the images was achieved using standard IRAF tasks. The electronic bias level was removed from the CCD by fitting a Chebyshev function to the overscan region and subtracting it from each column. By averaging ten bias frames, a master bias per night was created and subtracted from the images in order to remove any remaining bias structure. Dark images were also observed in order to remove the dark signal from the CCD. This correction turned out to be negligible, and was not considered. Twilight flats were also observed at the beginning and at the end of each observing night. They were combined and used to remove the pixel-to-pixel structure of the images.

The photometric calibration of the images was obtained by observing several standard stars from the Landolt (1992), Jorgensen (1994), and Montgomery et al. (1993) catalogues. They were observed each night at different zenith distances in order to measure the atmospheric extinction. The calibration constant was taken from Fasano et al. (2002).

2.1 Cluster environment

Table 1: The sample of clusters.

Given the scarce information on the clusters presented here, we comment briefly on the redshift data and the environmental situation of each of them.

A1643. The redshift of this cluster is attributed by Humason et al. (1956), who obtained a spectrum of the brightest galaxy in the area, finding z = 0.198. Our images were centered at that position $\alpha({\rm J2000})=12$h55m54.4s, $\delta({\rm J2000})= +44$d04m46s. More recently, Gal et al. (2003) detected an overdense region centered at $\alpha({\rm J2000})=12$h55m42.4s, $\delta({\rm J2000})= +44$d05m22s, identified as cluster NSC J125542+440522. They have determined a photometric redshift of 0.2515. Both clusters appear in our frames where we can identify A1643 as the one dominated by the galaxy observed by Humason et al. (1956) and, therefore, at z = 0.198. This is the value we adopt in this paper. We will exclude the frames that could be contaminated by the presence of NSC J125542+440522 in all the analysis regarding the galactic content of A1643.

A1878. This clusters appears with z = 0.254 in the NED[*]. A closer inspection shows that there is another value given to a galaxy in the field, namely z = 0.222. Both redshift values come from Sandage et al. (1976), who observed the brightest galaxy in the field, placed at $\alpha({\rm J2000})=14$h12m52.13s, $\delta({\rm J2000})= +29$d14m29s, and another, fainter galaxy at $\alpha({\rm J2000})=14$h12m49.13s, $\delta({\rm J2000})= +29$d12m59s. As quoted by the authors, the spectra were of low quality. The low z value corresponds to the brightest object that appears at the center of a strong concentration of galaxies that correspond to the cluster catalogued as A1878. More recently, Gal et al. (2003) identified a cluster labeled as NSC J141257+291256, with a photometric redshift z = 0.22. Its position and redshift value coincide with that of the bright galaxy observed by Sandage et al. (1976) that is accepted here as the brightest galaxy of A1878.

A1952. The redshift attributed to this cluster, z = 0.248, also comes from the work by Sandage et al. (1976) who observed the brightest cluster galaxy. The possible confusion regarding this cluster comes from the fact that the position given by Abell et al. (1989), $\alpha({\rm J2000})=14$h41m04.2s, $\delta({\rm J2000})= +28$d38m12s, does not coincide with that of its Brightest Cluster Galaxy (BCG) as given by Sandage et al. (1976), $\alpha({\rm J2000})=14$h41m03.6s, $\delta({\rm J2000})= +28$d36m59.68s. To add to the confusion, Gal et al. (2003) detected a cluster designed by NSC J144103+283622, at almost exactly the position of A1952's BCG, but the redshift they determined photometrically amounts to 0.2084. Taking all the information at hand, we consider that the cluster identified by Gal et al. (2003) is A1952, but the redshift we adopt here is that measured by Sandage et al. (1976), z = 0.248. The analysis we present here of the Color-Magnitude Relation support this conclusion.

A2111. This cluster has the largest amount of information available in the literature of all the clusters in our sample. The redshift was established from spectroscopic observations by Lavery & Henry (1986). The center given by NED comes from the ACO catalogue given by Abell et al. (1989), namely, $\alpha({\rm J2000})=15$h39m38.3s, $\delta({\rm J2000})= +34$d24m21s. However, the subsequent analysis of the X-ray data by Henriksen et al. (1999); Wang et al. (1997); Miller et al. (2006), led them to conclude that the cluster center position is at $\alpha({\rm J2000})=15$h39m40.9s , $\delta({\rm J2000})= +34$d25m04s, only 5.04 kpc away from the Brightest Cluster Galaxy. Miller et al. (2006) also provide a large number of spectra. Interestingly, the X-ray works showed that this cluster is undergoing a merger and presents a rather large blue fraction.

A2658. The redshift is taken from Fetisova (1982). The center, as given by Abell et al. (1989) is at $\alpha({\rm J2000})=23$h44m58.8s, $\delta({\rm J2000})= -12$d18m20s. However, our BCG is located at $\alpha({\rm J2000})=23$h44m49.83s, $\delta({\rm J2000})= -12$d17m38.93. After a visual inspection of the cluster image in the Digital Sky Survey, we conclude that the center of the cluster is given by the BCG, where a high concentration of galaxies is visually detected.

The adopted central position and redshift value for the five clusters discussed here are collected in Table 1. We also show in the table the details of the observations. Columns 1-4 give the cluster name, center coordinates (right ascension and declination in Equatorial coordinates, J2000) and redshift, respectively. The number of pointings observed for each cluster are indicated in Col. 5. These pointings cover the different cluster areas shown in Col. 6. The last column gives the seeing of the observed images. For the center position we adopted that of their respective BCGs except for A2111, for which the X-ray data has been used.

3 Galaxy detection and extraction

We used SExtractor (Bertin & Arnouts 1996) to detect the individual objects in our images, and to extract their photometric parameters. The extraction of the galaxies was performed on the deeper Gunn-r images. The photometry of the galaxies in the B-band was obtained using the ASSOC mode of SExtractor. We fixed several SExtractor parameters based on the properties of the images, such as: background level, stellar FWHM, zero-point, exposure time, or radius for aperture photometry. The values of the other SExtractor parameters such as the minimum area of pixels above threshold (DETECT_MINAREA), the number of deblending sub-thresholds (DEBLEND_NTHRESH) or the minimum contrast parameter for deblending (DEBLEND_MINCONT), were established after checking the results of the deblending images.

In this way, we obtained a first catalogue of 488 objects, including stars and galaxies. The stars were identified using the stellar index given by SExtractor. We considered an object as a galaxy when its stellar index was smaller than 0.2 and as star if the stellar index was larger than 0.8. The objects with intermediate values of the stellarity index were considered as doubtful objects. Only a small fraction of objects were classified as stars (27) or doubtful (5), so the final catalogue includes 456 galaxies.

SExtractor provides different magnitudes for each detected galaxy. We have considered two of them. The first one corresponds to a fixed-aperture of radius five kpc, useful to compare colors in the same physical region (Varela 2004). The other one is the magnitude called by SExtractor ``MAG_BEST'' that is determined in an automatic aperture that depends on the neighbours around the galaxy. If those neighbours are bright enough to affect the magnitude corresponding to an aperture enclosing the whole object by more than 10%, then that magnitude is taken as the corrected isophotal magnitude, which corresponds to the isophotal magnitude together with a correction. This magnitude provides the best measures of the total light of the objects (Stott et al. 2008; Nelson et al. 2002).

The B- and r- SExtractor magnitudes were k-corrected in the following way. For the B-band filter we adopted the relation kB = 4.4225 z+0.0294, obtained as an interpolation of the data given by Pence (1976) in the range $0.08 \leq z \leq 0.24$. The magnitudes of the Gunn-r filter were k-corrected using the approximation $k_r = 2.5 \log (1+z)$ (Jorgensen et al. 1992)

In Table 2 we show the mean r-band magnitude error provided by SExtractor for all the galaxies in each cluster. The last column shows the errors in colour, obtained as the quadratic sum of the errors of the fixed-aperture magnitude in the two filters B and r. For the calibration errors in the Gunn-r band, see Fasano et al. (2002).

Table 2: Photometric errors.

4 Properties of the cluster galaxies

4.1 The color-magnitude relation

In the early fifties, Baum (1959) and Rood (1969) realized that the color index of the bright, early type galaxies correlates with their luminosity. Later on, Visvanathan & Sandage (1977) and Visvanathan & Griersmith (1977) concluded on the universality of the so called CMR found for early type galaxies. Since then the study of the CMR has been used as a tool to analyze the evolution with z of the early type galaxies (see for example De Lucia et al. 2007a; Driver et al. 2006).

We present here the CMR for the galaxies found in our clusters. We use the color index B-r measured in a five kpc aperture. For the magnitudes we use the BEST magnitudes provided by SExtractor. All the detected galaxies in each cluster up to some limiting magnitude were used to build the relation. In Fig. 1, we have plotted the absolute magnitude distribution of the sample together with the completeness limit for each cluster and for the whole sample. The completeness limit has been defined as the maximum of the distribution. The sample appears to be complete up to $M_r \approx -19.8$. Therefore, to avoid possible problems with the magnitude limit, we have considered a safer limit. Only galaxies brighter than Mr=-20 have been used for the analysis of the CMR.

The definitive criterion to find the galaxies that actually belong to a given cluster is indeed the redshift. Unfortunately, the redshift information is in general scant for clusters at redshift $\sim$0.2 except for some particular cases. We have found in the literature 22 galaxies in the frame of A2111 with redshift data provided by Miller et al. (2006), whereas for the other clusters there are just one or two redshift entries in the NED. On the other hand, the CMR is well defined and it is not necessary to have the redshift information at hand to analyze it. Background galaxies are identified as those objects that are 0.2 mag redder than the value from the fitted CMR. That value seems safe if we take into account the combined uncertainty of the photometric errors and that 3 $\sigma \approx 0.1{-}0.18$. After applying this criterion the final number of galaxies retained as members of one of our five clusters is 408. They are collected in the table presented in the appendix. The first column gives the name of the cluster. The second and third columns give the coordinates of the galaxy, the fourth column gives the z information when available. The fifth and sixth columns give the r and B absolute magnitudes of each galaxy, assuming that they are located at the cluster redshift.

\par\includegraphics[width=5cm,clip]{9600fig1.ps}\end{figure} Figure 1: Absolute magnitude histogram of the galaxies in the five clusters. The dotted line shows the completeness magnitude limit for each cluster; the dashed line shows the common magnitude limit we have adopted for the five clusters.
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The fit of the red sequence of the CMR for each cluster has been determined by carrying out a least absolute deviation regression fit to the observed data (Armstrong & Kung 1978). The fit of the CMR for each cluster was obtained using an iterative procedure. A first fit was obtained using all the galaxies brighter than Mr=-20 for a given cluster. Then, the distance of each galaxy in B-r to the fitted CMR was computed. Those galaxies with a distance greater than three times the rms of the fitted relation were rejected, and a new fit to the CMR was performed with the remaining ones. This process was repeated until the fit to the CMR did not change further. The final fit was estimated using a nonparametric bootstrap method (Efron & Tibshirani 1986), with $n \log^2 n$ resamplings, n being the number of galaxies up to the completeness limit, as presented in Babu & Singh (1983). The slope and zero point are the median value of the resampling, and the standard errors we estimated as the rms of the bootstrap samples. We have checked that the early type galaxies that belong to A2111 are contained in the CMR. In Fig. 2, we show the colour-magnitude diagrams for all the galaxies in the frames and the CMRs fitted for all the clusters. We have also plotted in that figure the histogram of the color differences between the observed and the CMR-fitted values. We give in Table 3 the zero point, a0, the slope, a1 and the rms of the fitted CMRs for each cluster.

\par\includegraphics[width=8.3cm,clip]{9600fig2.ps}\end{figure} Figure 2: Left panels: the color-magnitude diagrams for the five clusters. The solid line is the fit to the red sequence and the dotted line is the upper 0.2 mag limit. The vertical line corresponds to the limit Mr = -20 at the cluster redshift. Right panels: the histograms of the B-r distance of the galaxies to the corresponding red sequence.
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Table 3: CMR parameters and the galaxy blue fractions.

In Fig. 3, we have plotted the slopes of the fitted CMRs in our clusters at medium redshift together with those obtained by López-Cruz et al. (2004) for clusters with z < 0.15. As the figure illustrates, there is no clear tendency of the change in slope of the CMR with redshift. The mean value of the slope of the CMR for our sample together with López-Cruz et al. (2004) is $-0.051 \pm 0.008$, and for our sample only is $-0.055 \pm 0.014$. These values are also very similar to the slope value found by Mei et al. (2006) for two clusters at $z\sim 1.26$. Thus, the slope values we find for our clusters at $z \sim 0.2$ are completely consistent with the values found for lower and much higher redshift values. Moreover, the range of values found at any redshift are also similar. Thus, we find no indication of a change of the CMR slope up to $z \sim 0.25$ and even up to $z\sim 1.26$. This result would indicate that the stellar population of the bright, early type galaxies defining the cluster red sequence was settled soon after the galaxy formation.

\par\includegraphics[width=7cm,clip]{9600fig3.ps}\end{figure} Figure 3: Slopes of the CMR for the sample of López-Cruz et al. (2004) (black circles) and our sample (empty triangles).
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4.2 The blue galaxy fraction

We have studied the fraction of blue galaxies, $f_{\rm b}$, in the bright population, $M_r \leq -20$, of the clusters presented here. The blue fraction was defined as the ratio of the number of blue galaxies observed out of the total number of galaxies within a fixed aperture. We have considered as blue galaxies those with a B-r color at least 0.26 mag bluer than the red sequence. This color index corresponds to the original definition by Butcher & Oemler (1984), who considered as blue those galaxies whose colors were bluer than B-V = 0.2 at z=0. Given the photometric errors and the statistical nature of the k-correction we adopted that common value of the color index for all the five clusters in spite of their differences in redshift. The results are not affected if individual color values were adopted.

The removal of foreground galaxies was done on the base of the measured redshift when available (just very few cases) or using statistical arguments. By integrating the luminosity function of field galaxies up to Mr=-20 in the solid angle corresponding to each of our clusters, we obtained 0.38 foreground galaxies per frame at z = 0.2. This estimation is in good agreement with previous findings by Fasano et al. (2000). The foreground contamination is therefore statistically negligible. The fraction of blue galaxies has been computed for each cluster using all the surveyed area. In order to be able to compare our results for the different clusters and with other studies, we have considered that our frames are representative of the area corresponding to a circular aperture that, set at the center of the cluster, includes all the area that we have covered. For comparison, we have adopted two apertures, of radius 420 and 735 kpc respectively. For the cluster A2658, only the smaller aperture could be used. Indeed, in the original definition given by Butcher & Oemler (1984), the fraction was calculated for an aperture containing 30% of the cluster population (R30). Since only the central parts of our clusters were sampled we could not determine the value of R30 for them. The fixed apertures we have used are a substitute for the canonical value. We notice that they are in the range of the expected R30 values as given by Butcher & Oemler (1984). The errors attributed to the measured fractions, listed in the last two columns of Table 3, were computed assuming Poissonian statistics, following De Propris et al. (2004).

In Fig. 4 we show the blue fraction of galaxies in our clusters as a function of redshift within a radius of 420 kpc (top panel) and within a radius of 735 kpc (bottom panel). We have also plotted for comparison the blue fraction of galaxies obtained from a sample of nearby galaxy clusters by De Propris et al. (2004) within an aperture of r200/2. As can be seen in the figure, our errors bars are very similar to those given by De Propris et al. (2004). In all cases, we have more than 10 galaxies per cluster to compute the blue fraction. The comparison with the data by De Propris et al. (2004) clearly indicates that there is no relation between the value of the blue galaxy fraction and the cluster redshift.

The range of values found is also similar to that found by De Propris et al. (2004) for lower redshift clusters. In particular, the very high blue fraction we obtain for A1878 is found for some lower z clusters in the quoted reference. The central median values we find for our sample are $\langle f_{\rm b}\rangle=0.090 \pm 0.138$ for the 420 kpc and $0.285 \pm 0.194$ for the 735 kpc aperture, in agreement with the median $f_{\rm b}$ value, $0.162 \pm 0.125$ of De Propris et al. (2004), for an aperture of r200/2.

Table 4: Fraction of morphological types.

\par\includegraphics[clip,width=0.8\hsize]{9600fig4.ps}\par\includegraphics[clip,width=0.8\hsize]{9600fig5.ps}\end{figure} Figure 4: Blue fraction of galaxies in our sample of clusters (triangles) compared with those obtained by De Propris et al. (2004) (black circles) for an aperture of r200/2. The top (bottom) panel corresponds to the blue fraction computed within a radius of 420 kpc (735 kpc).
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We find a nominal increment in the blue fraction as a function of the aperture. This is in agreement with the findings by De Propris et al. (2004); Margoniner & de Carvalho (2000); Goto et al. (2003).

Regarding the cluster A2111, Butcher & Oemler (1984) obtained a blue fraction of $0.16 \pm 0.03$ within a r30 that, for this cluster, corresponds to 892 kpc. Miller et al. (2006) obtained, for the same aperture, the values of $0.15 \pm 0.03$ and $0.23 \pm 0.03$ using photometric data or only galaxies with spectroscopic data, respectively. We have obtained $0.031 \pm 0.030$ and $0.125 \pm 0.052$ for our 420 kpc and 735 kpc aperture, a smaller value, in agreement with the smaller aperture, even if not significantly different when the errors are taken into account.

5 Galaxy morphology

For the analysis presented here, we have classified the galaxies visually. A quantitative analysis will be presented in a forthcoming work (Ascaso et al. 2008).

All the galaxies brighter than Mr=-20.0 were classified visually by two of us (B.A. and J.V.) into four different types: Ellipticals (E), Lenticulars (S0), Spirals (Sp) and Irregulars (I). We have compared our classification with that reported by Fasano et al. (2000) for the galaxies in common. In Fig. 5, we show the result of that comparison. 70$\%$ of the galaxies were classified as the same type, whereas 20$\%$ differ by only one type. The morphological classification for that bright subsample is given in the last column of the table in the appendix.

\par\includegraphics[width=6.8cm,clip]{9600fig6.ps}\end{figure} Figure 5: The visual classification differences between Fasano et al. (2000) and this paper.
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In Table 4, we show the percentages of the different galaxy types in the central part of each cluster in the 420 and 735 kpc aperture respectively. Notice that A1643 and A1878 have a large number of late type galaxies (about 60%). In particular, A1878 also contains a large fraction of irregular galaxies (19%). The rest of the clusters have an early-type population dominating in their cores. A diversity is clear as far as morphological populations is concerned.

5.1 Morphological distribution of the galaxies in the clusters

It is well known that early-type galaxies in clusters at low redshift are in general located in denser regions and closer to the center of the cluster than later types, (Dressler 1980). We want now to investigate the way in which those clusters at medium redshift are populated.

In Fig. 6, we have plotted the cumulative functions of the different types of galaxies versus projected distance of each galaxy to the center of the cluster. The solid lines represent the cumulative distribution of early-type, elliptical and lenticular, galaxies; the dotted lines correspond to the cumulative distribution of late-type galaxies, spiral and irregular. The vertical lines indicate the radius where the cumulative distributions reach 50% of the distributions.

We see that all the clusters are dominated in their central regions by early type galaxies except A1878, that has a sizable fraction of late-type, including irregular galaxies, which may explain its high (central) fraction of blue galaxies. However, this is not unique since similar cases can also be found at lower redshift (see for example Varela 2004). A1643 has also a large global fraction of late-type, spiral galaxies, but they do not dominate the core of the cluster. The rest of the clusters are also centrally dominated by a population of elliptical galaxies, with an overall population with a smaller fraction of late-type galaxies. As we noticed before, diversity seems to be the dominant aspect of our five clusters.

\par\includegraphics[width=5cm,clip]{9600fig7.ps}\end{figure} Figure 6: Cumulative functions of the different morphological types as a function of the projected radius to the center of the cluster. Early types: solid lines; late types: dotted lines. The vertical lines indicate the radius where the distributions reach the 50% level.
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To test whether the distribution of early and late type galaxies are similar, we have performed a Kolmogorov-Smirnov test. Excluding A2658, for which there are not enough points to extract significant results, we find that the two populations are significantly different in two clusters, A1878 and A1952, while for the other two, A1643 and A2111, the KS test does not allow us to extract significant results. Then, A1878 and A1952 show morphological segregation as found in low redshift samples such as, by Adami et al. (1998). Moreover, in the case of A1878 the dominant morphological population is late type galaxies.

5.2 The concentration parameter

We have calculated the concentration parameter of our clusters in the central 735 kpc using the definition given by Butcher & Oemler (1978), $\log$(R60/R20), where R60 and R20 are the radii containing 60% and 20% of the cluster populations within 735 kpc. Only the four clusters with enough area coverage were analyzed. The concentration values we have found are 0.311 for A1643, 0.389 for A1878, 0.329 for A2111 and 0.696 for A1952 as can be seen in Fig. 7. We have overplotted the values found for lower z clusters by Butcher & Oemler (1978) and for a higher redshift sample by Dressler et al. (1997). As can be seen in the figure, our concentration values span the full range of the values measured for lower redshfit clusters. Moreover, this range encompasses also that of the higher redshift cluster concentration values. It does not seem, therefore, that there is any clear tendency of the change in concentration parameter with redshift or morphological type. At most, it could be argued that clusters tend to progressively populate the lower half of the plane when the redshift increases.

Likewise, Butcher & Oemler (1978) and Dressler et al. (1997) suggested that the more irregular, less concentrated clusters would be preferentially populated by late type galaxies. In that sense, we notice that A1643, the cluster with the largest global fraction of late-type galaxies, presents the lowest value of the concentration parameter. Moreover, A1878, another cluster with a low concentration index also presents a rather high fraction of late type and irregular galaxies and, is dominated by this population. However, A2111, our third cluster with a low concentration, is dominated by an early-type population. Thus, although there is an indication of a higher fraction of irregular clusters with increasing redshift, the small statistics prevent us from reaching a firm conclusion.

\par\includegraphics[width=8.5cm,clip]{9600fig8.ps}\end{figure} Figure 7: Concentration parameter versus redshift for our clusters (triangles), a low-redshift compilation (Butcher & Oemler 1978: black points) and a higher redshift sample (Dressler et al. 1997: asteriks). The horizontal line is the mean concentration value of the clusters with enough area coverage.
Open with DEXTER

5.3 Interaction systems

Another interesting feature for consideration in clusters at that range of redshift is the proportion of interacting systems compared to lower redshift clusters. To investigate this, we have calculated the distribution of the f-parameter defined by Varela et al. (2004) for the galaxies in the final catalogue. It gives an account of the relative importance of the tidal forces for each galaxy. Larger values indicate a larger proportion of interaction systems. The result is plotted in Fig. 8. The median value of the distribution is -1.59, whereas the median value found for the Coma Cluster is -2.7 (Varela et al. 2004). Moreover, we find that 63.97% of the galaxies have a perturbation parameter higher than -2, which is the value chosen by Varela et al. (2004) to select truly interacting systems.

More specifically, the median f-values we find are -1.39 (A2658), -1.92 (A1643), -1.60 (A1878), -1.67 (A2111) and -1.29 (A1952), all of them larger than -2. This is indicative of the presence of a larger population of interacting systems in our sample than in the Coma Cluster.

\par\includegraphics[width=8.3cm,clip]{9600fig9.ps}\end{figure} Figure 8: Histogram of the f-parameter values for the galaxies belonging to our clusters.
Open with DEXTER

6 Discussion and conclusions

It is well known that locally, the color-magnitude relation for early-type galaxies has a well-defined slope with a small scatter, (Bower et al. 1992). Results based on HST data (Mei et al. 2006; Stanford et al. 1998; Ellis et al. 1997) demonstrated the existence of a tight red sequence in clusters at redshift up to 1.26, comparable in scatter and slope to that observed in the Coma Cluster and low redshift clusters. In agreement with these results, we find no significant difference in the slope of the CMR for our cluster sample and other samples at different redshift values. This reinforces the conclusion of the universality of the CMR on all the explored z-range.

Regarding the Butcher-Oemler effect, the values we obtain for the blue galaxy fraction are similar to those found by De Propris et al. (2004) for lower redshift SDSS clusters. The only outstanding case in our sample is A1878, with a large blue fraction. This goes together with a large fraction of late type and irregular galaxies in its central region and a low value of the concentration parameter. However, this case is not unique, (see for example, De Propris et al. 2004; Aguerri et al. 2007). The blue fraction values that we find indicate that there is no evolution in this parameter at least up to redshift 0.25. Thus, the Butcher-Oemler effect starts to manifest at even higher redshift. This is in agreement with previous results obtained with other samples (see Andreon et al. 2006). That conclusion, together with the universality of the CMR suggests that the stellar population in cluster galaxies has not evolved significantly in the last 2.5 Gyr.

We have found differences in the fraction of blue galaxies with the aperture considered for its determination, in the sense indicated by other reported results (De Propris et al. 2004; Margoniner & de Carvalho 2000; Goto et al. 2003), and in agreement with other values found in the literature for the blue fraction of A2111. However, these differences are not significant.

The morphological segregation between early and late-type galaxies observed in nearby clusters (Adami et al. 1998; Aguerri et al. 2004) has been shown to be present in two clusters from our medium reshift sample. However, the range of situations we find is similar to that found at lower redshift and no evolutionary trend is manifested through it.

We have also looked at the degree of interaction of the galaxies in our sample. We have found that the median value of the f-parameter is significantly higher than in the Coma cluster in all our five clusters. A wider sample at low redshift is lacking to enable us to draw conclusions about the possible higher incidence of interactions at higher redshift.

The results we have obtained suggest that the evolutionary status of clusters at $z \sim 0.2$ is not significantly different from that of clusters at lower redshift. Indeed, larger samples at intermediate redshifts are needed to establish whether the trends with z indicated by the concentration parameter are real or only artifacts produced by the small size of the available samples.

On the other hand, some parameters like the CMR slope are remarkably constant with redshift, strongly supporting the view that the red sequence was well established soon after the formation of the red, bright cluster galaxies. Regarding the Butcher-Oemler effect our results reinforce the view that it starts to appear at rather high z-values, larger than $z \sim 0.25$. As far as the morphological mixing is concerned, the values span a wide range, similarly to other samples at lower or higher redshift, indicating that here also diversity is the dominant aspect.

We acknowledge the anonymous referee for useful comments and suggestions. Begoña Ascaso is supported by an I3P Individual Fellowship from the Consejo Superior de Investigaciones Cientificas at the Instituto de Astrofísica de Andalucía. J.A.L.A. acknowledges finalcial support by the project ESTALLIDOS AYA2007-67965-C03-01. We also acknowledge a grant by the Spanish Ministerio de Educacion y Ciencia, reference PNAYA2006-14056 and Proyecto de Excelencia of the Junta de Andalucia, reference J.A FQM 1392.



Online Material

Appendix A: Catalogue of galaxies detected in the cluster sample

Name $\alpha$ (J2000) $\delta$ (J2000) z Mr MB Morph
A 2658 23h 44m 47.99s -12d 18m 46.20s   -19.12 -18.24  
A 2658 23h 44m 55.21s -12d 18m 37.00s   -18.98 -18.20  
A 2658 23h 44m 49.55s -12d 18m 34.40s   -19.65 -18.99  
A 2658 23h 44m 49.62s -12d 18m 31.90s   -18.68 -18.01  
A 2658 23h 44m 50.35s -12d 18m 25.50s   -21.89 -21.06 S
A 2658 23h 44m 49.13s -12d 18m 19.80s   -19.29 -18.34  
A 2658 23h 44m 47.27s -12d 18m 13.40s   -19.24 -19.14  
A 2658 23h 44m 46.97s -12d 18m 10.40s   -20.94 -20.12 S0
A 2658 23h 44m 49.36s -12d 18m 07.90s   -18.44 -17.53  
A 2658 23h 44m 52.22s -12d 18m 04.60s   -19.99 -18.90 E
A 2658 23h 44m 54.99s -12d 18m 05.60s   -18.08 -17.23  
A 2658 23h 44m 54.27s -12d 17m 59.30s   -21.42 -20.39 E
A 2658 23h 44m 50.42s -12d 17m 56.40s   -19.39 -18.41  
A 2658 23h 44m 51.64s -12d 17m 53.30s   -18.71 -18.11  
A 2658 23h 44m 47.44s -12d 17m 47.40s   -20.92 -19.87 E
A 2658 23h 44m 50.34s -12d 17m 32.70s   -18.84 -20.30  
A 2658 23h 44m 49.28s -12d 17m 38.20s   -18.19 -19.65  
A 2658 23h 44m 50.26s -12d 17m 20.90s   -21.07 -20.35 S0
A 2658 23h 44m 49.84s -12d 17m 26.70s   -21.32 -20.95 E
A 2658 23h 44m 49.80s -12d 17m 39.50s   -22.39 -22.02 E
A 2658 23h 44m 54.96s -12d 17m 38.80s   -18.80 -18.35  
A 2658 23h 44m 55.87s -12d 17m 37.60s   -18.22 -17.40  
A 2658 23h 44m 51.86s -12d 17m 35.30s   -19.57 -18.55  
A 2658 23h 44m 47.85s -12d 17m 31.10s   -18.14 -17.23  
A 2658 23h 44m 50.96s -12d 17m 19.10s   -20.24 -19.17 E
A 2658 23h 44m 55.84s -12d 17m 17.60s   -20.18 -19.15 S0
A 2658 23h 44m 51.40s -12d 17m 11.00s   -18.35 -18.28  
A 2658 23h 44m 56.18s -12d 17m 07.50s   -21.14 -20.31 S
A 2658 23h 44m 51.13s -12d 16m 48.00s   -20.61 -19.49 E
A 2658 23h 44m 46.13s -12d 16m 49.10s   -18.82 -18.35  
A 2658 23h 44m 49.65s -12d 16m 35.80s   -20.56 -19.43 S0
A 2658 23h 44m 47.99s -12d 16m 36.20s   -18.29 -17.66  
A 2658 23h 44m 51.63s -12d 16m 28.80s   -18.70 -17.79  
A 2658 23h 44m 53.27s -12d 16m 23.60s   -18.27 -17.77  
A 1643 12h 55m 52.30s 44d 05m 47.30s   -19.88 -20.46 S
A 1643 12h 55m 52.44s 44d 05m 52.70s   -19.52 -20.82  
A 1643 12h 55m 54.14s 44d 05m 52.70s   -19.79 -18.64  
A 1643 12h 55m 59.31s 44d 05m 53.20s   -19.36 -17.98  
A 1643 12h 55m 53.80s 44d 03m 15.20s   -19.79 -18.61 S
A 1643 12h 55m 55.18s 44d 03m 47.50s   -20.67 -19.46 S0
A 1643 12h 55m 49.83s 44d 04m 08.80s   -19.82 -19.24  
A 1643 12h 55m 49.75s 44d 04m 05.50s   -20.61 -19.63 S
A 1643 12h 55m 47.93s 44d 04m 01.20s   -20.36 -19.10 E
A 1643 12h 55m 48.06s 44d 04m 06.70s   -18.24 -17.09  
A 1643 12h 55m 51.98s 44d 04m 05.90s   -18.93 -19.06  
A 1643 12h 55m 59.67s 44d 04m 05.20s   -19.64 -18.62 S
A 1643 12h 55m 53.06s 44d 04m 06.60s   -18.89 -17.82  
A 1643 12h 55m 55.75s 44d 04m 07.30s   -19.39 -18.88  
A 1643 12h 56m 01.43s 44d 04m 07.90s   -19.71 -19.19  
A 1643 12h 55m 53.64s 44d 04m 13.70s   -20.09 -19.36 S
A 1643 12h 55m 50.96s 44d 04m 31.00s   -21.15 -20.05 E
A 1643 12h 55m 59.04s 44d 04m 26.90s   -19.00 -17.81  
A 1643 12h 55m 55.35s 44d 04m 34.40s   -20.69 -20.35 E
A 1643 12h 55m 54.88s 44d 04m 33.90s   -20.14 -19.56 S
A 1643 12h 55m 56.61s 44d 04m 38.20s   -18.70 -20.14  
A 1643 12h 55m 52.33s 44d 04m 46.80s   -18.42 -19.14  
A 1643 12h 55m 52.97s 44d 04m 50.00s   -19.82 -19.09  
A 1643 12h 55m 52.96s 44d 04m 39.20s 0.1978 -19.73 -19.60 S
A 1643 12h 55m 52.70s 44d 04m 44.50s   -20.42 -19.74 S0
A 1643 12h 55m 54.94s 44d 04m 45.60s   -19.29 -19.15  
A 1643 12h 55m 48.16s 44d 04m 49.50s   -19.49 -18.74  
A 1643 12h 55m 47.94s 44d 04m 51.60s   -19.59 -18.95  
A 1643 12h 55m 51.98s 44d 04m 53.10s   -19.57 -19.08  
A 1643 12h 55m 55.21s 44d 04m 53.10s   -18.00 -17.50  
A 1643 12h 55m 54.40s 44d 04m 53.70s   -18.26 -17.50  
A 1643 12h 55m 59.29s 44d 04m 57.10s   -20.02 -18.94 S
A 1643 12h 55m 56.07s 44d 04m 58.00s   -18.49 -17.59  
A 1643 12h 55m 54.00s 44d 05m 12.40s   -21.61 -20.35 S0
A 1643 12h 56m 01.63s 44d 05m 09.10s   -19.45 -18.11  
A 1643 12h 55m 49.61s 44d 05m 09.50s   -18.25 -17.15  
A 1643 12h 55m 47.67s 44d 05m 15.70s   -18.15 -17.15  
A 1643 12h 55m 54.61s 44d 05m 21.40s   -19.23 -17.99  
A 1643 12h 55m 53.05s 44d 05m 23.40s   -20.19 -18.97 S0
A 1643 12h 56m 00.41s 44d 05m 29.90s   -19.20 -18.91  
A 1643 12h 55m 48.02s 44d 05m 35.90s   -19.73 -18.91  
A 1643 12h 55m 52.36s 44d 05m 38.40s   -19.16 -19.35  
A 1643 12h 55m 52.76s 44d 05m 37.90s   -19.88 -19.97 S
A 1643 12h 55m 54.21s 44d 05m 44.70s   -19.41 -18.29  
A 1643 12h 56m 01.53s 44d 03m 29.90s   -18.65 -20.27  
A 1643 12h 55m 50.27s 44d 03m 30.50s   -19.27 -18.68  
A 1643 12h 55m 53.07s 44d 05m 47.80s   -18.67 -17.64  
A 1643 12h 55m 48.08s 44d 05m 51.70s   -18.23 -17.80  
A 1643 12h 55m 34.43s 44d 08m 50.30s   -19.53 -18.37  
A 1643 12h 55m 44.49s 44d 08m 53.60s   -19.09 -18.13  
A 1643 12h 55m 45.49s 44d 06m 39.60s   -18.15 -19.35  
A 1643 12h 55m 44.70s 44d 06m 35.60s   -19.65 -18.94  
A 1643 12h 55m 38.43s 44d 06m 29.90s   -18.50 -17.72  
A 1643 12h 55m 38.94s 44d 06m 35.20s   -18.31 -17.92  
A 1643 12h 55m 45.18s 44d 06m 46.30s   -19.68 -18.40 E
A 1643 12h 55m 32.98s 44d 06m 50.40s   -19.92 -19.46 S
A 1643 12h 55m 33.62s 44d 06m 30.00s   -18.06 -17.72  
A 1643 12h 55m 37.87s 44d 06m 57.10s   -18.59 -17.40  
A 1643 12h 55m 46.43s 44d 06m 58.80s   -18.14 -17.06  
A 1643 12h 55m 33.82s 44d 07m 12.50s   -20.93 -19.67 E
A 1643 12h 55m 36.30s 44d 07m 15.70s   -18.80 -18.47  
A 1643 12h 55m 41.25s 44d 07m 15.00s   -18.32 -17.59  
A 1643 12h 55m 39.33s 44d 07m 21.30s   -19.72 -18.39 S
A 1643 12h 55m 37.74s 44d 07m 23.30s   -18.00 -17.63  
A 1643 12h 55m 38.60s 44d 07m 29.10s   -18.09 -16.93  
A 1643 12h 55m 46.75s 44d 07m 35.40s   -18.99 -17.90  
A 1643 12h 55m 42.78s 44d 07m 48.60s   -18.24 -16.93  
A 1643 12h 55m 36.40s 44d 07m 53.40s   -20.71 -20.57 I
A 1643 12h 55m 36.55s 44d 07m 54.10s   -20.34 -20.10  
A 1643 12h 55m 36.63s 44d 08m 20.30s   -20.17 -20.49 I
A 1643 12h 55m 36.38s 44d 08m 24.40s   -19.77 -19.13 S0
A 1643 12h 55m 36.57s 44d 08m 30.40s   -20.27 -19.84 E
A 1643 12h 55m 43.31s 44d 08m 28.90s   -18.20 -18.04  
A 1643 12h 55m 38.31s 44d 08m 38.70s   -18.02 -17.76  
A 1643 12h 55m 37.59s 44d 06m 21.10s   -19.42 -18.66 S
A 1878 14h 12m 54.12s 29d 16m 16.60s   -18.74 -17.61  
A 1878 14h 12m 49.83s 29d 13m 40.60s   -18.90 -18.43  
A 1878 14h 12m 47.43s 29d 13m 55.50s   -18.53 -20.39  
A 1878 14h 12m 47.82s 29d 13m 53.40s   -21.69 -20.68 S
A 1878 14h 12m 53.32s 29d 13m 47.00s   -18.37 -18.29  
A 1878 14h 12m 54.23s 29d 13m 57.60s   -20.23 -20.50 S
A 1878 14h 12m 50.11s 29d 13m 59.90s   -18.63 -19.32  
A 1878 14h 12m 49.97s 29d 14m 02.60s   -20.45 -19.30 S
A 1878 14h 12m 56.80s 29d 14m 03.60s   -20.38 -20.06 I
A 1878 14h 12m 54.78s 29d 14m 03.90s   -18.55 -17.39  
A 1878 14h 12m 47.17s 29d 14m 05.80s   -20.04 -19.70 I
A 1878 14h 12m 49.47s 29d 14m 09.90s   -21.57 -20.53 S
A 1878 14h 12m 49.03s 29d 14m 07.80s   -18.94 -21.00  
A 1878 14h 12m 52.50s 29d 14m 11.40s   -20.94 -20.28 S
A 1878 14h 12m 54.85s 29d 14m 17.30s   -19.91 -19.67 S
A 1878 14h 12m 54.65s 29d 14m 23.80s   -19.23 -19.19  
A 1878 14h 12m 47.85s 29d 14m 17.10s   -19.70 -18.95  
A 1878 14h 12m 54.15s 29d 14m 19.30s   -20.80 -19.49 E
A 1878 14h 12m 52.75s 29d 14m 20.20s   -18.72 -20.18  
A 1878 14h 12m 52.18s 29d 14m 28.40s 0.2220 -22.36 -21.69 E
A 1878 14h 12m 46.85s 29d 14m 26.40s   -21.02 -20.50 I
A 1878 14h 12m 54.72s 29d 14m 31.90s   -21.42 -20.23 E
A 1878 14h 12m 56.29s 29d 14m 31.40s   -20.24 -19.80 I
A 1878 14h 12m 51.24s 29d 14m 48.20s   -20.10 -20.01 S
A 1878 14h 12m 51.04s 29d 14m 39.30s   -19.72 -20.22  
A 1878 14h 12m 50.98s 29d 14m 42.30s   -20.84 -21.55 I
A 1878 14h 12m 46.74s 29d 14m 40.00s   -18.44 -18.10  
A 1878 14h 12m 53.29s 29d 14m 41.40s   -20.30 -20.22  
A 1878 14h 12m 53.32s 29d 14m 44.60s   -19.55 -21.50  
A 1878 14h 12m 49.12s 29d 14m 42.50s   -21.38 -20.33 S
A 1878 14h 12m 50.12s 29d 14m 47.30s   -20.40 -19.13 S0
A 1878 14h 12m 52.25s 29d 14m 53.70s   -20.41 -20.57 S
A 1878 14h 12m 51.99s 29d 14m 57.10s   -19.53 -19.92  
A 1878 14h 12m 50.96s 29d 14m 56.60s   -21.29 -20.33 S
A 1878 14h 12m 46.14s 29d 14m 55.60s   -19.94 -19.35 S0
A 1878 14h 12m 46.58s 29d 14m 59.10s   -20.94 -19.69 S0
A 1878 14h 12m 53.29s 29d 14m 56.90s   -18.53 -17.55  
A 1878 14h 12m 48.23s 29d 15m 01.10s   -19.28 -18.27  
A 1878 14h 12m 50.01s 29d 15m 05.00s   -18.23 -17.10  
A 1878 14h 12m 56.61s 29d 15m 05.30s   -19.18 -19.30  
A 1878 14h 12m 49.37s 29d 15m 12.10s   -18.79 -17.72  
A 1878 14h 12m 50.60s 29d 15m 13.20s   -18.64 -18.42  
A 1878 14h 12m 49.68s 29d 15m 14.20s   -19.56 -19.22  
A 1878 14h 12m 55.12s 29d 15m 14.70s   -18.85 -17.83  
A 1878 14h 12m 51.24s 29d 15m 22.10s   -19.89 -19.95 S
A 1878 14h 12m 53.39s 29d 15m 22.30s   -19.01 -18.65  
A 1878 14h 12m 51.04s 29d 15m 28.90s   -19.51 -21.46  
A 1878 14h 12m 53.49s 29d 15m 27.70s   -18.76 -18.14  
A 1878 14h 12m 52.60s 29d 15m 41.10s   -18.61 -18.01  
A 1878 14h 12m 52.43s 29d 15m 48.70s   -21.00 -19.79 S0
A 1878 14h 12m 55.73s 29d 15m 56.70s   -18.18 -17.32  
A 1878 14h 12m 53.61s 29d 16m 00.80s   -19.77 -18.60  
A 1878 14h 12m 53.04s 29d 16m 07.40s   -18.86 -21.15  
A 1878 14h 12m 47.96s 29d 16m 09.50s   -19.69 -19.16  
A 1878 14h 13m 00.54s 29d 13m 56.90s   -21.15 -20.41 S0
A 1878 14h 12m 56.76s 29d 14m 03.60s   -20.00 -20.14 I
A 1878 14h 12m 56.78s 29d 12m 00.30s   -19.87 -18.86 S0
A 1878 14h 12m 57.80s 29d 12m 01.60s   -20.47 -19.97 S0
A 1878 14h 12m 59.05s 29d 12m 14.40s   -20.60 -20.01 E
A 1878 14h 12m 59.84s 29d 12m 19.50s   -20.45 -21.96 S
A 1878 14h 13m 00.58s 29d 12m 22.90s   -20.30 -19.90 S
A 1878 14h 13m 01.89s 29d 12m 17.50s   -19.55 -18.93 S
A 1878 14h 13m 05.79s 29d 12m 20.80s   -18.24 -18.48  
A 1878 14h 12m 58.97s 29d 12m 33.00s   -18.13 -17.07  
A 1878 14h 13m 01.29s 29d 12m 36.90s   -20.97 -20.65 S0
A 1878 14h 13m 05.52s 29d 12m 36.60s   -18.59 -18.07  
A 1878 14h 13m 02.23s 29d 12m 40.50s   -18.23 -18.12  
A 1878 14h 13m 05.38s 29d 12m 42.80s   -18.24 -17.75  
A 1878 14h 12m 58.42s 29d 12m 53.60s   -18.05 -19.13  
A 1878 14h 12m 58.26s 29d 12m 54.90s   -19.49 -20.04  
A 1878 14h 13m 05.59s 29d 12m 54.20s   -20.53 -19.81 E
A 1878 14h 13m 04.82s 29d 12m 55.40s   -19.03 -18.41  
A 1878 14h 13m 02.81s 29d 12m 55.70s   -19.44 -18.73 S
A 1878 14h 12m 58.70s 29d 12m 56.60s   -18.92 -18.15  
A 1878 14h 13m 04.41s 29d 13m 00.70s   -20.06 -19.78 S
A 1878 14h 12m 55.45s 29d 13m 04.30s   -19.48 -19.63 I
A 1878 14h 12m 55.11s 29d 13m 09.90s   -19.13 -19.64  
A 1878 14h 12m 57.07s 29d 13m 19.80s   -18.08 -18.08  
A 1878 14h 12m 57.65s 29d 13m 22.20s   -18.09 -17.93  
A 1878 14h 13m 00.40s 29d 13m 37.50s   -19.13 -18.71  
A 1878 14h 12m 57.01s 29d 13m 43.90s   -19.27 -18.62  
A 1878 14h 12m 57.70s 29d 13m 48.90s   -19.78 -19.18 S0
A 1878 14h 13m 03.99s 29d 13m 53.50s   -19.36 -19.74  
A 1878 14h 13m 02.65s 29d 14m 01.20s   -18.08 -18.25  
A 2111 15h 39m 35.52s 34d 26m 56.20s   -20.46 -19.56 S
A 2111 15h 39m 37.64s 34d 27m 03.80s 0.2295 -21.26 -20.22 S0
A 2111 15h 39m 31.84s 34d 27m 05.10s   -19.01 -18.09  
A 2111 15h 39m 38.48s 34d 24m 32.40s   -19.37 -18.96  
A 2111 15h 39m 40.16s 34d 24m 18.10s   -19.38 -18.33  
A 2111 15h 39m 39.34s 34d 24m 44.50s   -20.26 -19.31 E
A 2111 15h 39m 38.45s 34d 24m 51.40s   -20.02 -19.08  
A 2111 15h 39m 40.16s 34d 24m 55.70s   -20.49 -19.27 S0
A 2111 15h 39m 42.76s 34d 24m 56.60s   -18.32 -17.38  
A 2111 15h 39m 37.84s 34d 24m 57.00s   -18.55 -17.54  
A 2111 15h 39m 39.81s 34d 25m 00.50s   -18.06 -17.79  
A 2111 15h 39m 37.21s 34d 25m 08.50s   -19.67 -18.70 S
A 2111 15h 39m 40.49s 34d 25m 27.30s 0.2282 -22.67 -21.51 E
A 2111 15h 39m 39.75s 34d 25m 23.10s   -19.57 -18.85  
A 2111 15h 39m 39.20s 34d 25m 11.50s   -21.13 -20.38 E
A 2111 15h 39m 39.39s 34d 25m 13.40s 0.2211 -21.34 -20.61 E
A 2111 15h 39m 36.23s 34d 25m 12.10s   -20.34 -19.21 S0
A 2111 15h 39m 34.90s 34d 25m 14.50s   -18.97 -18.02  
A 2111 15h 39m 40.27s 34d 25m 34.80s   -20.07 -21.06  
A 2111 15h 39m 38.15s 34d 25m 18.10s   -20.21 -19.01 S0
A 2111 15h 39m 37.53s 34d 25m 18.70s   -19.62 -18.72 S
A 2111 15h 39m 36.64s 34d 25m 29.00s   -18.96 -18.34  
A 2111 15h 39m 33.61s 34d 25m 34.00s   -18.48 -17.78  
A 2111 15h 39m 36.79s 34d 25m 39.10s 0.2312 -20.90 -19.65 S0
A 2111 15h 39m 39.69s 34d 25m 21.20s   -20.40 -19.70  
A 2111 15h 39m 31.27s 34d 25m 40.00s   -20.24 -19.65  
A 2111 15h 39m 38.68s 34d 25m 38.90s   -18.16 -17.04  
A 2111 15h 39m 37.29s 34d 25m 45.90s   -18.49 -17.33  
A 2111 15h 39m 36.42s 34d 25m 50.10s   -20.46 -19.50 E
A 2111 15h 39m 41.20s 34d 25m 50.90s   -20.53 -19.36 S0
A 2111 15h 39m 40.18s 34d 25m 50.80s   -18.60 -17.90  
A 2111 15h 39m 33.99s 34d 25m 51.30s   -19.30 -18.23  
A 2111 15h 39m 37.44s 34d 25m 54.80s   -20.12 -18.98 E
A 2111 15h 39m 39.52s 34d 25m 56.90s   -19.23 -18.23  
A 2111 15h 39m 39.91s 34d 25m 57.20s   -18.53 -17.69  
A 2111 15h 39m 41.69s 34d 26m 01.70s   -18.03 -16.89  
A 2111 15h 39m 31.72s 34d 26m 07.20s   -20.49 -19.37 S0
A 2111 15h 39m 36.84s 34d 26m 07.20s   -20.44 -19.68 I
A 2111 15h 39m 38.07s 34d 26m 09.50s   -18.64 -19.00  
A 2111 15h 39m 34.11s 34d 26m 19.20s   -20.80 -20.58 S
A 2111 15h 39m 34.26s 34d 26m 12.50s 0.2289 -21.97 -21.11 S0
A 2111 15h 39m 38.18s 34d 26m 06.90s   -19.72 -19.53  
A 2111 15h 39m 32.26s 34d 26m 12.80s   -19.25 -18.22  
A 2111 15h 39m 38.58s 34d 26m 28.20s   -20.23 -19.24 S
A 2111 15h 39m 39.03s 34d 26m 38.10s   -19.29 -19.48  
A 2111 15h 39m 38.70s 34d 26m 38.80s 0.2246 -20.85 -20.29 S
A 2111 15h 39m 37.81s 34d 26m 35.90s   -18.12 -17.73  
A 2111 15h 39m 31.99s 34d 26m 36.10s   -18.39 -18.00  
A 2111 15h 39m 35.47s 34d 26m 43.70s   -20.70 -19.87 S0
A 2111 15h 39m 41.19s 34d 26m 41.30s   -20.27 -20.24 I
A 2111 15h 39m 40.90s 34d 26m 45.40s   -19.28 -19.45  
A 2111 15h 39m 37.59s 34d 26m 44.20s   -18.92 -18.91  
A 2111 15h 39m 33.13s 34d 26m 45.60s   -19.25 -18.91  
A 2111 15h 39m 37.16s 34d 26m 45.70s   -18.26 -17.93  
A 2111 15h 39m 38.38s 34d 26m 50.50s   -18.01 -17.13  
A 2111 15h 39m 32.78s 34d 24m 22.40s   -19.21 -18.31  
A 2111 15h 39m 41.34s 34d 24m 34.30s 0.2294 -20.97 -20.81 S
A 2111 15h 39m 41.81s 34d 24m 42.70s 0.2292 -22.61 -22.18 E
A 2111 15h 39m 42.27s 34d 24m 40.40s   -19.08 -20.81  
A 2111 15h 39m 41.26s 34d 24m 43.60s   -20.43 -22.04 S
A 2111 15h 39m 47.09s 34d 27m 37.90s 0.2368 -21.25 -20.57 S0
A 2111 15h 39m 42.81s 34d 27m 44.60s   -19.68 -19.55 I
A 2111 15h 39m 52.99s 34d 27m 48.60s 0.2297 -20.98 -19.94 S0
A 2111 15h 39m 54.29s 34d 25m 06.60s   -18.05 -17.24  
A 2111 15h 39m 51.92s 34d 25m 18.80s   -18.85 -18.83  
A 2111 15h 39m 44.40s 34d 25m 22.70s   -19.46 -19.41  
A 2111 15h 39m 44.15s 34d 25m 21.30s   -18.78 -20.66  
A 2111 15h 39m 54.03s 34d 25m 24.60s   -18.87 -18.31  
A 2111 15h 39m 53.10s 34d 25m 26.50s   -18.75 -17.73  
A 2111 15h 39m 47.96s 34d 25m 32.10s   -20.49 -19.52 E
A 2111 15h 39m 52.98s 34d 25m 41.10s   -19.31 -18.24  
A 2111 15h 39m 43.94s 34d 25m 46.70s   -19.45 -19.01  
A 2111 15h 39m 42.69s 34d 25m 52.10s   -18.13 -16.99  
A 2111 15h 39m 42.04s 34d 26m 04.00s   -19.44 -18.39  
A 2111 15h 39m 42.02s 34d 25m 59.60s   -18.96 -20.78  
A 2111 15h 39m 44.85s 34d 25m 58.50s   -19.19 -19.08  
A 2111 15h 39m 47.82s 34d 26m 00.00s   -19.08 -18.05  
A 2111 15h 39m 53.40s 34d 25m 59.60s   -18.94 -18.56  
A 2111 15h 39m 52.50s 34d 26m 02.20s   -20.40 -19.62 S
A 2111 15h 39m 47.49s 34d 26m 11.10s   -18.84 -18.00  
A 2111 15h 39m 42.59s 34d 26m 14.00s   -19.82 -18.96  
A 2111 15h 39m 43.06s 34d 26m 23.00s   -18.42 -17.36  
A 2111 15h 39m 42.02s 34d 26m 30.30s 0.2258 -22.09 -20.96 E
A 2111 15h 39m 43.25s 34d 26m 32.90s   -19.02 -18.04  
A 2111 15h 39m 48.31s 34d 26m 36.70s   -18.79 -18.43  
A 2111 15h 39m 49.35s 34d 26m 41.50s 0.2299 -21.54 -21.03 S
A 2111 15h 39m 50.11s 34d 26m 44.40s   -19.48 -19.02  
A 2111 15h 39m 52.85s 34d 26m 46.80s   -20.45 -19.95 E
A 2111 15h 39m 42.09s 34d 26m 49.20s   -19.55 -18.52  
A 2111 15h 39m 45.75s 34d 26m 57.40s 0.2292 -21.07 -20.05 E
A 2111 15h 39m 42.98s 34d 27m 00.30s   -18.40 -18.28  
A 2111 15h 39m 42.30s 34d 27m 02.60s   -18.20 -17.92  
A 2111 15h 39m 52.55s 34d 27m 07.50s   -19.06 -20.58  
A 2111 15h 39m 52.04s 34d 27m 07.60s   -19.01 -21.29  
A 2111 15h 39m 52.15s 34d 27m 12.20s   -21.13 -21.23 S
A 2111 15h 39m 42.28s 34d 27m 17.10s   -20.12 -19.17  
A 2111 15h 39m 51.51s 34d 27m 31.30s   -19.54 -18.61  
A 2111 15h 39m 48.27s 34d 27m 34.80s   -18.70 -18.45  
A 2111 15h 39m 47.70s 34d 25m 16.40s   -19.85 -18.96  
A 2111 15h 39m 47.89s 34d 27m 39.90s   -20.28 -19.32 E
A 2111 15h 39m 47.34s 34d 25m 10.20s 0.2309 -21.07 -20.81 E
A 2111 15h 39m 47.26s 34d 25m 15.90s   -20.43 -20.38 S
A 1952 14h 41m 07.84s 28d 38m 29.40s   -22.05 -21.10 E
A 1952 14h 40m 59.08s 28d 38m 35.40s   -20.11 -19.24 S
A 1952 14h 41m 01.82s 28d 35m 57.10s   -20.13 -19.75 S
A 1952 14h 40m 59.60s 28d 36m 07.40s   -19.18 -18.44  
A 1952 14h 41m 02.64s 28d 36m 14.50s   -18.79 -18.40  
A 1952 14h 41m 01.57s 28d 36m 31.50s   -18.30 -18.20  
A 1952 14h 40m 59.42s 28d 36m 42.00s   -19.05 -18.36  
A 1952 14h 41m 04.07s 28d 36m 47.50s   -19.94 -19.04 E
A 1952 14h 41m 04.47s 28d 36m 49.70s   -18.71 -20.59  
A 1952 14h 41m 01.82s 28d 37m 09.60s   -18.17 -20.22  
A 1952 14h 41m 01.92s 28d 37m 14.50s   -20.76 -20.80 E
A 1952 14h 41m 02.66s 28d 37m 10.00s   -22.11 -21.94 S0
A 1952 14h 41m 03.13s 28d 37m 10.10s   -21.41 -20.84 E
A 1952 14h 41m 02.67s 28d 37m 02.40s   -20.63 -19.99  
A 1952 14h 40m 58.41s 28d 36m 52.50s   -19.89 -19.03 S0
A 1952 14h 41m 01.19s 28d 37m 00.50s   -21.20 -20.33 E
A 1952 14h 40m 59.94s 28d 37m 22.10s   -18.59 -17.95  
A 1952 14h 40m 59.55s 28d 37m 34.20s   -18.29 -17.81  
A 1952 14h 41m 01.81s 28d 37m 34.70s   -19.48 -18.91  
A 1952 14h 41m 01.58s 28d 37m 48.30s   -18.21 -20.37  
A 1952 14h 41m 01.32s 28d 37m 43.20s   -21.57 -21.82 E
A 1952 14h 41m 01.53s 28d 37m 44.30s   -19.21 -18.96  
A 1952 14h 40m 59.15s 28d 37m 47.80s   -18.93 -20.67  
A 1952 14h 40m 59.50s 28d 37m 48.80s   -19.90 -19.01  
A 1952 14h 40m 58.98s 28d 37m 51.40s   -18.41 -18.51  
A 1952 14h 41m 03.17s 28d 37m 52.50s   -18.10 -17.71  
A 1952 14h 40m 59.94s 28d 38m 00.10s   -20.38 -19.53 E
A 1952 14h 41m 08.82s 28d 37m 59.00s   -19.72 -19.04 E
A 1952 14h 41m 05.82s 28d 38m 02.20s   -18.68 -17.82  
A 1952 14h 41m 00.90s 28d 38m 04.70s   -19.54 -18.59  
A 1952 14h 41m 04.06s 28d 38m 08.40s   -19.13 -19.23  
A 1952 14h 41m 07.98s 28d 38m 09.40s   -19.08 -18.20  
A 1952 14h 41m 03.17s 28d 38m 21.10s   -18.04 -18.15  
A 1952 14h 41m 05.43s 28d 38m 21.80s   -19.11 -18.99  
A 1952 14h 41m 02.63s 28d 35m 50.80s   -18.52 -18.54  
A 1952 14h 40m 59.43s 28d 38m 27.20s   -19.17 -19.37  
A 1952 14h 41m 01.91s 28d 35m 54.80s   -19.06 -20.83  
A 1952 14h 40m 59.20s 28d 38m 24.20s   -19.32 -18.60  
A 1952 14h 41m 13.59s 28d 37m 29.60s   -22.13 -21.43 S0
A 1952 14h 41m 05.84s 28d 37m 41.60s   -20.22 -19.27  
A 1952 14h 41m 14.94s 28d 37m 42.60s   -21.80 -20.98 S0
A 1952 14h 41m 05.68s 28d 37m 46.70s   -18.22 -18.33  
A 1952 14h 41m 08.53s 28d 37m 49.00s   -19.26 -19.18  
A 1952 14h 41m 03.16s 28d 37m 52.20s   -18.08 -17.86  
A 1952 14h 41m 15.18s 28d 35m 29.10s   -18.16 -20.08  
A 1952 14h 41m 15.04s 28d 35m 21.20s   -19.32 -21.52  
A 1952 14h 41m 15.18s 28d 35m 24.30s   -19.61 -21.59  
A 1952 14h 41m 03.94s 28d 35m 21.30s   -20.35 -19.38 E
A 1952 14h 41m 13.55s 28d 35m 21.80s   -19.77 -19.72  
A 1952 14h 41m 05.92s 28d 35m 29.90s   -20.77 -19.82 S0
A 1952 14h 41m 08.36s 28d 35m 28.50s   -18.46 -18.64  
A 1952 14h 41m 08.59s 28d 35m 30.80s   -19.01 -19.42  
A 1952 14h 41m 08.51s 28d 35m 32.50s   -20.41 -20.52 S
A 1952 14h 41m 04.76s 28d 35m 32.40s   -19.40 -19.16  
A 1952 14h 41m 07.83s 28d 35m 32.30s   -18.39 -20.48  
A 1952 14h 41m 07.59s 28d 35m 35.00s   -21.58 -21.23 S
A 1952 14h 41m 11.01s 28d 35m 33.00s   -19.87 -18.93  
A 1952 14h 41m 10.10s 28d 35m 33.70s   -19.03 -18.15  
A 1952 14h 41m 05.91s 28d 35m 38.50s   -19.36 -18.50  
A 1952 14h 41m 08.19s 28d 35m 44.50s   -21.61 -20.93 S0
A 1952 14h 41m 03.56s 28d 35m 44.20s   -19.69 -19.45  
A 1952 14h 41m 13.72s 28d 35m 54.10s   -18.37 -18.45  
A 1952 14h 41m 13.55s 28d 35m 52.00s   -18.78 -21.38  
A 1952 14h 41m 03.27s 28d 35m 56.30s   -19.34 -18.51  
A 1952 14h 41m 08.00s 28d 36m 03.20s   -18.96 -18.97  
A 1952 14h 41m 09.73s 28d 36m 02.80s   -18.20 -17.44  
A 1952 14h 41m 05.67s 28d 36m 05.30s   -18.64 -17.72  
A 1952 14h 41m 12.15s 28d 36m 07.00s   -19.45 -18.73  
A 1952 14h 41m 10.72s 28d 36m 07.50s   -18.10 -18.28  
A 1952 14h 41m 14.47s 28d 36m 26.20s   -19.86 -19.18  
A 1952 14h 41m 05.45s 28d 36m 26.40s   -18.40 -17.58  
A 1952 14h 41m 04.06s 28d 36m 26.50s   -18.06 -20.09  
A 1952 14h 41m 04.22s 28d 36m 27.80s   -18.35 -19.37  
A 1952 14h 41m 12.94s 28d 36m 27.30s   -19.29 -18.61  
A 1952 14h 41m 06.81s 28d 36m 31.50s   -20.01 -21.90 E
A 1952 14h 41m 07.10s 28d 36m 37.30s   -20.67 -20.27 E
A 1952 14h 41m 07.03s 28d 36m 39.20s   -22.10 -22.55 S0
A 1952 14h 41m 03.36s 28d 36m 37.10s   -20.43 -19.40 E
A 1952 14h 41m 14.04s 28d 36m 40.80s   -18.80 -18.92  
A 1952 14h 41m 03.11s 28d 36m 46.60s   -20.74 -19.93 S0
A 1952 14h 41m 04.07s 28d 36m 52.70s   -19.32 -20.90  
A 1952 14h 41m 03.57s 28d 37m 00.30s   -22.61 -24.23 E
A 1952 14h 41m 03.14s 28d 36m 57.00s   -19.55 -21.16  
A 1952 14h 41m 10.75s 28d 36m 47.30s   -19.16 -21.67  
A 1952 14h 41m 06.34s 28d 37m 01.30s   -18.75 -18.04  
A 1952 14h 41m 06.48s 28d 37m 06.90s   -20.14 -19.23  
A 1952 14h 41m 08.25s 28d 37m 13.80s   -21.85 -21.21 S
A 1952 14h 41m 12.33s 28d 37m 11.00s   -19.03 -19.11  
A 1952 14h 41m 06.26s 28d 37m 12.20s   -18.15 -17.28  
A 1952 14h 41m 09.40s 28d 37m 13.00s   -18.55 -18.59  
A 1952 14h 41m 09.72s 28d 37m 17.80s   -19.85 -20.07 S
A 1952 14h 41m 05.02s 28d 37m 34.90s   -18.05 -20.08  
A 1952 14h 41m 06.27s 28d 37m 27.50s   -20.01 -20.84 S0
A 1952 14h 41m 05.49s 28d 37m 33.90s   -19.02 -21.47  
A 1952 14h 41m 05.32s 28d 37m 35.90s   -19.18 -20.34  
A 1952 14h 41m 04.78s 28d 37m 31.60s   -19.79 -21.64  
A 1952 14h 41m 04.76s 28d 37m 35.50s   -19.83 -19.94  
A 1952 14h 41m 04.77s 28d 35m 05.50s   -18.30 -18.55  
A 1952 14h 41m 06.32s 28d 37m 18.30s   -18.30 -17.78  
A 1952 14h 41m 14.57s 28d 37m 18.70s   -19.65 -19.37  
A 1952 14h 41m 11.82s 28d 37m 19.30s   -18.39 -18.59  
A 1952 14h 41m 07.53s 28d 37m 23.60s   -19.14 -18.20  
A 1952 14h 41m 04.29s 28d 37m 23.00s   -18.54 -18.27  
A 1952 14h 41m 05.23s 28d 35m 06.80s   -19.10 -18.75  
A 1952 14h 41m 03.35s 28d 37m 29.50s   -20.17 -19.26  
A 1952 14h 41m 06.39s 28d 37m 33.60s   -18.12 -17.60  
A 1952 14h 41m 12.23s 28d 35m 06.70s   -19.05 -18.27  
A 1952 14h 41m 08.44s 28d 35m 09.00s   -18.39 -17.78  
A 1952 14h 41m 05.36s 28d 37m 40.50s   -18.42 -17.71  
A 1952 14h 41m 10.78s 28d 35m 12.30s   -18.24 -18.05  
A 1952 14h 41m 13.01s 28d 35m 15.30s   -19.08 -19.23  
A 1952 14h 41m 10.45s 28d 35m 16.60s   -19.36 -19.26  
A 1952 14h 41m 14.88s 28d 35m 29.70s   -18.45 -19.98  

Copyright ESO 2008