arXiv subjects

P. Katgert

Publications and source records attributed to P. Katgert.

26 records · Page 2Linked to original sources

arXiv1998

ENACSVII, Galaxy density profiles of rich clusters of galaxies

We have analyzed the projected galaxy distributions in a subset of the ENACS/ COSMOS cluster sample. We made Maximum-Likelihood fits to the distribution of COSMOS galaxies for 4 theoretical profiles, with `cores' (generalized King- and Hubble-profiles) and with `cusps' (generalized Navarro et al., or NFW, and de Vaucouleurs profiles). We use the Likelihood ratio to investigate whether the observations are better described by profiles with cusps or with cores. Taking the King and NFW profiles as model of either class, we find that about 75% of the clusters are better fitted by the King profile than by the NFW profile. However, for the individual clusters the preference for the King profile is rarely significant. When we limit ourselves to the central regions it appears that the significance increases drastically, with 65% of the clusters showing a strong preference for a King over an NFW profile. We constructed composite clusters from the COSMOS and ENACS data, taking special care to avoid the creation or the destruction of cusps. We scale by different ways (projected distances, core radii, r_{200}).In all three cases we find that the King profile is clearly preferred over the NFW profile. However, this preference is not shared by the brightest galaxies. We conclude that these galaxies are represented almost equally well by King and NFWprofiles, but that the distribution of the fainter galaxies clearly shows a core rather than a cusp. Finally, we compared the outer slope of the galaxy distributions in ourclusters with results for model calculations with different cosmological parameters. We conclude that the observed profile slope indicates a low value for Omega_0. This is consistent with the direct estimate of Omega_0 based on the M/L ratios of the individual clusters.

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arXiv1997

The Fundamental Plane of clusters of galaxies

We have used the ESO Nearby Abell Cluster Survey (ENACS) in combination with the Cosmos Galaxy Catalogue, to investigate the existence of a Fundamental Plane (FP) for rich clusters of galaxies. The 20 clusters with the most regular projected galaxy distributions appear to define a quite narrow FP, which is similar to the FP found by Schaeffer et al., who used other clusters. Our cluster FP appears to be different from that of ellipticals, as well as from the virial prediction. The latter fact may have several physical explanations, or a combination thereof. If M/L varies with L this will change the FP slope away from the virial slope. Differences in dynamical structure between clusters will also produce deviations from the virial FP. In view of the long virialization time-scales in all but the very central parts of galaxy clusters, the deviation of the cluster FP from the virial expectation may also result from clusters not being totally virialized. The scatter of the observations around the cluster FP is fairly small. An important part of the observed scatter is likely to be intrinsic. If this intrinsic spread were due exclusively to deviations from the Hubble flow it would imply cluster peculiar velocities of at most about 1000 km.s-1.

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arXiv1996

The ESO Nearby Abell Cluster Survey. III. Distribution and Kinematics of Emission-Line Galaxies

We have studied the frequency of occurrence, the kinematics and the spatial distribution of Emission-Line Galaxies (ELG) in clusters in the ESO Nearby Abell Cluster Survey (ENACS). More than 90% of the ELG are spirals, but the ELG represent only 30% of all spirals. The true ELG fraction in clusters is 0.10; this is consistent with that in the field (0.21) as a result of differences in morphological mix. The average ELG fraction decreases with increasing velocity dispersion of the cluster. Only 1/5 of the clusters shows a significant difference in the average velocities of the ELG and the other (non-ELG) galaxies; in a similar fraction of the clusters significant differences in velocity dispersion are seen. Yet, the velocity dispersion of the ELG is, on average, 20% larger than that of the non-ELG. This larger velocity dispersion is largely intrinsic, i.e. it is not likely to be the result of velocity offsets of the ELG. The surface density of the ELG is significantly less peaked towards the centre than that of the non-ELG. The ELG are distributed fairly smoothly within the cluster with at most 25% in compact substructures. The distribution and kinematics of the ELG yield virial mass estimates that, on average, are 50% higher than those based on the non-ELG. This probably means that the ELG are on more radial orbits than the non-ELG. All observed properties of the ELG are consistent with most of them being on their first approach of the high-density cluster core.

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arXiv1995

The Kinematics of Emission-Line Galaxies in Clusters from ENACS

Summary - By using the data from the ESO Nearby Abell Cluster Survey (ENACS), we have studied the properties of emission-line galaxies (ELG) in clusters. The fraction of ELG in clusters is 16~\%; this fraction is slightly dependent on the cluster velocity dispersion, being larger for ``colder'' systems. ELG tend to occur more frequently than other cluster galaxies in substructures. However, only a minor cluster fraction has an ELG population with a mean velocity significantly different from that of the overall cluster population. The velocity distribution of cluster ELG is broader than that of the other cluster galaxies, which translates in a larger observed velocity dispersion. The velocity distribution for ELG in the inner cluster regions suggests that ELG are on mostly radial orbits.

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arXiv1995

The ESO Nearby Abell Cluster Survey. I. Description of the Dataset and Definition of Physical Systems

Summary - We describe the results of the ESO Key-programme on `Structure and Dynamics of Rich Galaxy Clusters' (or ENACS). The final database contains a total of 5634 galaxies in the directions of 107 clusters from the ACO catalogue with richness $R\ge 1$ and mean redshifts $z \le 0.1$. Of the 5634 redshifts, 4465 are based on absorption lines only, 583 on emission lines only and 586 on both. The overall reliability of the 5634 accepted redshifts is 0.98. For 5615 galaxies an $R_{25}$ magnitude was obtained. We discuss various methods for defining the compact, physically relevant systems in the 107 `pencil-beam' surveys. We have chosen to apply a fixed velocity gap of 1000 km/s to separate galaxies that do not form part of the same system. With this gap size, systems are not broken up into sub-systems, and field galaxies are hardly linked to the systems. We present the mean redshifts of the 220 systems (with at least 4 members) identified in the 107 pencil beam surveys. On average, about 75~\% of the 5634 galaxies are in the largest system found in the direction of the rich Abell cluster candidate. Half of the 25~\% of galaxies outside the largest system belong to a secondary system along the same line of sight. For about 90~\% of the nearby rich Abell cluster candidates studied here we find a redshift system that either contains more than half of the total number of redshifts, or that has at least two times as many redshifts as the next largest system.

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arXiv1995

The ESO Nearby Abell Cluster Survey. II. The Distribution of Velocity Dispersions of Rich Galaxy Clusters

Summary - By combining the 5634 redshifts from the ESO Nearby Abell Cluster Survey (the ENACS) with another 1000 redshifts from the literature we are able to study the distribution of velocity dispersions for a volume-limited sample of 128 $R_{\rm ACO} \geq 1$ clusters, out to a redshift $z=0.1$, in a solid angle of 2.55 sr centered on the South Galactic Pole. In deriving velocity dispersions we apply a new, physically motivated method for removing fore- and background galaxies. We discuss in detail the completeness of the cluster sample for which we derive the distribution of cluster velocity dispersions. The large apparent spread between velocity dispersion and richness must be largely intrinsic. A consequence of the very broad relation between richness and velocity dispersion is that all cluster samples complete in richness are biased against low dispersions. For the richness limit of our sample this bias operates below about 800 km/sec. Above 800 km/s, our distribution of global velocity dispersions is free from systematic errors and biases, and agrees very well with the most recent determination of the distribution of cluster X-ray temperatures. Therefore, we conclude that X-ray temperature and velocity dispersion distributions statistically measure the same cluster property. We stress the need for model predictions that produce exactly the same information as provided by the observations, for a sample of model clusters with a richness limit that mimics that of the sample of observed clusters.

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arXiv1995

The Kinematics of Emission-Line Galaxies in Clusters from ENACS

By using the ENACS data, we have studied the properties of emission-line galaxies (ELG) in clusters. The fraction of ELG in clusters is 16~%; this fraction is slightly dependent on the cluster velocity dispersion, being larger for ``colder'' systems. ELG tend to occur more frequently than other cluster galaxies in substructures. However, only a minor cluster fraction has an ELG population with a mean velocity significantly different from that of the overall cluster population. The velocity distribution of cluster ELG is broader than that of the other cluster galaxies, which translates in a larger observed velocity dispersion. The velocity distribution for ELG in the inner cluster regions suggests that ELG are on mostly radial orbits.

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arXiv1994

The Shapes of Galaxy Clusters

We have reanalyzed a data set of 99 low redshift ($ z < 0.1 $) Abell clusters and determined their shapes. For this, three different measures are used. We use Monte-Carlo simulations to investigate the errors in the methods. The corrected distribution of cluster ellipticities shows a peak at $ ε\sim 0.4 $ and extends to $ ε\sim 0.8 $. The results are self-consistent, i.e., with the corrected distribution over projected cluster shapes we can reconstruct the observed distribution and the observed relation between the number of galaxies in a cluster and its ellipticity. It is shown that the richer clusters are intrinsically more nearly spherical than the poorer ones. The corrected distribution of cluster shapes is more consistent with a prolate population than with an oblate population. We compare the corrected true distribution of (projected) ellipticities with predictions from N-body simulations. For this, we use a catalogue of 75 N-body simulated clusters (van Kampen 1994) which assume a CDM spectrum with $ Ω= 1.0 $. The simulations include a recipe for galaxy formation and merging. 'Observing' these simulated clusters produces an ellipticity distribution that extends to much higher $ ε$ and that has too few nearly spherical clusters. Preliminary results of simulations of the formation of clusters in an $ Ω= 0.2 $ universe suggest that, on average, clusters are more nearly spherical in this case.

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