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R. G. Carlberg

Publications and source records attributed to R. G. Carlberg.

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Faint K Selected Galaxy Correlations and Clustering Evolution

Angular and spatial correlations are measured for K-band--selected galaxies, 248 having redshifts, 54 with z>1, in two patches of combined area 27 arcmin^2. The angular correlation for K<=21.5 mag is (theta/1.4+/-0.19 arcsec e^{+/-0.1})^{-0.8}. From the redshift sample we find that the real-space correlation, calculated with q_0=0.1, of M_K<=-23.5 mag galaxies (k-corrected) is ξ(r) = (r/2.9e^{+/-0.12}1/h Mpc)^{-1.8} at a mean z= 0.34, (r/2.0e^{+/-0.15}1/h Mpc)^{-1.8} at z= 0.62, (r/1.4e^{+/-0.15}1/h Mpc)^{-1.8} at z= 0.97, and (r/1.0e^{+/-0.2}1/h Mpc)^{-1.8} at z= 1.39, the last being a formal upper limit for a blue-biased sample. In general, these are more correlated than optically selected samples in the same redshift ranges. Over the interval 0.3<= z<=0.9 galaxies with red rest-frame colors, (U-K)_0>2 AB mag, have ξ(r)=(r/2.4e^{+/-0.14}1/h Mpc)^{-1.8} whereas bluer galaxies, which have a mean B of 23.7 mag and mean [OII] equivalent width W_{eq} = 41=Å, are very weakly correlated, with ξ(r)=(r/0.9e^{+/-0.22}1/h Mpc)^{-1.8}. For our measured growth rate of clustering, this blue population, if non-merging, can grow only into a low-redshift population less luminous than 0.4L_\ast. The cross-correlation of low- and high-luminosity galaxies at z=0.6 appears to have an excess in the correlation amplitude within 100/h kpc. The slow redshift evolution is consistent with these galaxies tracing the mass clustering in low density, Omega= 0.2, relatively unbiased, sigma_8=0.8, universe, but cannot yet exclude other possibilities.

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Redshift Evolution of Galaxy Cluster Densities

The number of rich galaxy clusters per unit volume is a strong function of Omega, the cosmological density parameter, and sigma_8, the linear extrapolation to z=0 of the density contrast in 8/h Mpc spheres. The CNOC cluster redshift survey provides a sample of clusters whose average mass profiles are accurately known, which enables a secure association between cluster numbers and the filtered density perturbation spectrum. We select from the CNOC cluster survey those EMSS clusters with bolometric L_x>=10^45 erg/s and a velocity dispersion exceeding 800 km/s in the redshift ranges 0.18-0.35 and 0.35-0.55. We compare the number density of these subsamples with similar samples at both high and low redshift. Using the Press-Schechter formalism and CDM style structure models, the density data are described with sigma_8=0.75+/-0.1 and Omega=0.4+/-0.2 (90% confidence). The cluster dynamical analysis gives Omega=0.2+/-0.1$ for which sigma_8=0.95+/-0.1 (90% confidence). The predicted cluster density evolution in an Ω=1 CDM model exceeds that observed by more than an order of magnitude.

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The Average Mass-to-Light Profile of Galaxy Clusters

The systematic errors in the virial mass-to-light ratio, M_v/L, of galaxy clusters as an estimator of the field M/L value are assessed. We overlay 14 clusters in redshift space to create an ensemble cluster which averages over substructure and asymmetries. The combined sample, including background, contains about 1150 galaxies, extending to a projected radius of about twice r_200. The radius r_200, defined as where the mean interior density is 200 times the critical density, is expected to contain the bulk of the virialized cluster mass. The dynamically derived M(r_200)/L(r_200) of the ensemble is 0.82+/-0.14 . The M_v/L overestimate is attributed to not taking into account the surface pressure term in the virial equation. Under the assumption that the velocity anisotropy parameter is in the range 0<=β<=2/3, the galaxy distribution accurately traces the mass profile beyond about the central 0.3r_200. There are no color or luminosity gradients in the galaxy population beyond 2r_200, but there is 0.11+/-0.05 mag fading in the r band luminosities between the field and cluster galaxies. We correct the cluster virial mass-to-light ratio, M_v/L=289+/-50 h\msun/\lsun (calculated assuming q_0=0.1), for the biases in M_v and mean luminosity to estimate the field M/L=213+/-59 h\msun/\lsun. With our self-consistently derived field luminosity density, j/ρ_c=1136+/-138 h\msun/\lsun (at z~1/3), the corrected M/L indicates Ω_0=0.19+/-0.06+/-0.04 (formal 1σrandom error and estimated potential systematic errors).

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The Luminosity Function of Field Galaxies in the CNOC1 Redshift Survey

We have computed the luminosity function for 389 field galaxies from the Canadian Network for Observational Cosmology cluster redshift survey (CNOC1), over redshifts z = 0.2-0.6. We find Schechter parameters M^* - 5 log h = -19.6 \pm 0.3 and α= -0.9 \pm 0.2 in rest-frame B_{AB}. We have also split our sample at the color of a redshifted but nonevolving Sbc galaxy, and find distinctly different luminosity functions for red and blue galaxies. Red galaxies have a shallow slope α\approx -0.4 and dominate the bright end of the luminosity function, while blue galaxies have a steep α\approx -1.4 and prevail at the faint end. Comparisons of the CNOC1 results to those from the Canada-France (CFRS) and Autofib redshift surveys show broad agreement among these independent samples, but there are also significant differences which will require larger samples to resolve. Also, in CNOC1 the red galaxy luminosity density stays about the same over the range z = 0.2-0.6, while the blue galaxy luminosity density increases steadily with redshift. These results are consistent with the trend of the luminosity density vs. redshift relations seen in the CFRS, though the normalizations of the luminosity densities appear to differ for blue galaxies. Comparison to the local luminosity function from the Las Campanas redshift survey (LCRS) shows that the luminosity density at z \approx 0.1 is only about half that seen at z \approx 0.4. A change in the luminosity function shape, particularly at the faint end, appears to be required to match the CNOC1 and LCRS luminosity functions, if galaxy evolution is the sole cause of the differences seen. However, it should be noted that the specific details of the construction of different surveys may complicate the comparison of results and so may need to be considered carefully.

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Close Pairs of Field Galaxies in the CNOC1 Redshift Survey

A redshift sample of 545 field galaxies is used to examine how the galaxy merger rate changes with redshift, and how mergers affect the observed properties of galaxies in close pairs. Close pairs are defined as those with projected separations less than 20 h^{-1} kpc. At a mean redshift of 0.33, it is found that 7.1 +/- 1.4 % of galaxies are in close physical pairs, compared to 4.3 +/- 0.4 % locally. The merger rate is estimated to change with redshift as (1+z)^{2.8 +/- 0.9}. These results are shown to be consistent with previous close pair studies, and provide one of the strongest constraints to date on the redshift dependence of the merger rate. As with earlier studies, no significant differences between the mean properties of paired and isolated galaxies are detected. However, using the subset of confirmed close physical pairs, those which appear to be undergoing interactions or mergers (based on their images) are found to have galaxies with strong emission lines and very blue rest-frame colors. In addition, these pairs have low relative velocities, increasing the likelihood that the galaxies will merge. We interpret this as the first clear evidence of merger-induced star formation occurring in field galaxies at this redshift.

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Galaxy Evolution in Abell 2390

The galaxy population in the intermediate-redshift ($z=0.228$) rich cluster Abell 2390 is investigated. We present velocities, colors, and morphological information for an exceptionally large sample of 323 galaxies (216 cluster members) in a 46$^\prime \times 7^\prime$ (6 $h^{-1}$ Mpc $\times$ 1 $h^{-1}$ Mpc) strip centered on the cD galaxy. This sample of confirmed cluster members is second only to that for the Coma cluster in terms of sample size and spatial coverage in the cluster rest frame, and is the first to trace the transition between a rich cluster and the field at intermediate redshift. The galaxy population in the cluster changes gradually from a very evolved, early-type population in the inner 0.4 \hmpc\ of the cluster to a progressively later-type population in the extensive outer envelope of the cluster from 1 to 3 \hmpc\/ in radius. Radial gradients in galaxy $g-r$ color, 4000 Å\/ break, H$δ$ and [O II] line strengths and morphology are seen in the cluster, and are investigated by comparing the data to models computed with the GISSEL spectral synthesis package. The results suggest that the cluster has been gradually built up by the infall of field galaxies over $\sim 8$ Gyr and that star formation has been truncated in infalling galaxies during the accretion process. The morphological composition of the cluster is shown to be consistent with such a scenario. If true for other clusters, infall-truncated star formation as seen in Abell 2390 may explain both the Butcher-Oemler effect and the large fraction of S0 galaxies in clusters. Only $\simlt$5\% of the galaxies observed in Abell 2390 exhibit evidence for star formation at levels stronger than those seen in typical late-type systems. This suggests that starbursts do not play a major role in driving cluster galaxy evolution at the redshift of

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Evolution of galactic disks in clusters and the field at $0.1 < z < 0.6$ in the CNOC survey

Two-dimensional surface photometry is presented for a sample of 351 late-type galaxies with $0.12 < z < 0.65$. These objects are drawn from the Canadian Network for Observational Cosmology (CNOC) cluster survey and are either spectroscopically confirmed members of clusters at $z=0.23$ (64 galaxies), $0.43$ (45), and $0.55$ (36) or field galaxies with similar redshifts. Galaxies in the rich cluster Abell 2256 at $z=0.06$ were also analyzed with the same methods to provide a local reference point. At redshifts of (0.23, 0.43, 0.55) the disk surface brightness in cluster late-type galaxies is higher in the $B$-band by $Δμ_{0}(B) =(-0.58\pm 0.12,-1.22\pm 0.17,-0.97\pm 0.2$) mag, respectively, relative to the Freeman (1970) constant surface-brightness relation; whereas disks in cluster galaxies at $z=0.06$ are consistent with that relation. Field galaxies show a progressive disk-brightening with redshift that is consistent with that seen in the cluster population. Taken together with similar measurements of early-type galaxies (Schade et al. 1996a), these results suggest that the evolution of the field and cluster galaxy populations are similar, although we emphasize that our sample of cluster galaxies is dominated by objects at large distances (up to 3 Mpc) from the dense cluster core, so that the implications of these findings with respect to the Butcher-Oemler effect and the morphology-density relation will not be clear until an analysis of galaxy properties as a function of cluster-centric distance is completed.

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Evolution of Cluster and Field Ellipticals at $0.2 < z < 0.6$ in the CNOC Cluster Survey

Two-dimensional surface photometry has been done for 166 {\em early-type} galaxies (bulge/total luminosity $B/T>0.6$) in 3 fields of the Canadian Network for Observational Cosmology (CNOC) cluster survey. These galaxies are either spectroscopically confirmed members of clusters at $z=0.23$ (45 galaxies), $0.43$ (22), and $0.55$ (16) or field galaxies in the same redshift range. An additional 51 early-type galaxies in the rich cluster Abell 2256 at $z=0.06$ were analysed with the same technique. The resulting structural and surface brightness measurements show that, in the plane of absolute magnitude $M_{AB}(B)$ versus $\log R_e$ (half-light radius), the locus of cluster ellipticals shifts monotonically with redshift so that at redshifts of (0.23, 0.43, 0.55), galaxies of a given size are more luminous by ($-0.25\pm 0.10,-0.55\pm 0.12,-0.74\pm 0.21$) magnitudes with respect to the same relation measured at $z=0.06$ (adopting $q_\circ=0.5$). There is no evidence that early-type galaxies in the field evolve differently from those in clusters. If dynamical processes do not substantially modify the size-luminosity relation for early-type galaxies over the observed redshift range, then these galaxies have undergone significant luminosity evolution over the past half of the age of the universe. The amount of brightening is consistent with passive evolution models of old, single-burst stellar populations.

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The Two-Point Correlation Function at Redshift 1/3

We present the results of a study of the two-point correlation function for a sample of field galaxies taken from the CNOCI cluster survey. The sample consists of 144 galaxies within a contiguous region of space subtending 225 square arcminutes. The objects have r-band magnitudes 17.0 < r < 21.7 and redshifts 0.21 < z < 0.53. The median redshift of the sample is 0.36. The real space correlation function is found to be consistent with a power law ξ(r) = (r/r_0)^-1.7 with r_0 = 2.1 +0.6/-0.3 (Ω_0=1), or r_0 = 2.5 +0.7/-0.4 (Ω_0=0.2). Uncertainties are estimated using the bias-corrected bootstrap resampling method, with 300 resamplings. This low correlation length implies strong evolution since z~0.36 has occurred in either the correlation function or the luminosity function; if the observed correlation function is modeled as ξ(r,z) = ξ(r,0) * (1+z)^-(3+ε) with ξ(r,0) = (r/5.1 h^-1Mpc)^-1.7, then ε= 0.8 +1.0/-1.3. Comparison of the redshift space and real space correlation function indicates that the one-dimensional pairwise peculiar velocity dispersion σat z~0.36 is weakly inconsistent with 770 km s^-1, the value predicted by the Cosmic Virial Theorem if Ω_0=1. The observed correlation function is, however, consistent with σ=400 km s^-1, the value expected if Ω_0=0.2.

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Sinking Satellites and Tilting Disk Galaxies

The infall of a satellite galaxy onto a galactic disk generally brings in angular momentum that is not aligned with the axis of the disk. The main dynamical issues addressed are what fraction of the orbital angular momentum of the satellite and the associated energy is added to the disk, as opposed to being left in the halo, and whether the absorbed fraction is added coherently or thermalized in the disk. By employing fully self-consistent disk+halo+satellite N-body simulations, we study the particular case of the satellite and main halo having similar density profiles, with internal velocities having the ``cosmological'' scaling $σ\propto M^{1/3}$. We find that most of the orbital angular momentum of the infalling satellite is left in the tidally stripped satellite remnants, with only $2\%$, $6\%$ and $9\%$ of the orbital angular momentum being transferred to disks and halos for $10\%$, $20\%$ and $30\%$ disk-mass satellites respectively. Because the disks are tilted by the infall of $10\%$, $20\%$ and $30\%$ disk-mass satellites by angles of $(2.9\pm0.3)^\circ$, $(6.3\pm0.1)^\circ$ and $(9.7\pm0.2)^\circ$ respectively, the kinetic energy associated with the vertical motion in the initial coordinate frame of the three disks is respectively increased by $(6\pm3)\%$, $(26\pm3)\%$ and $(51\pm5)\%$ whereas the corresponding disk thermal energy associated with the vertical random motion in the tilted coordinate frame is only increased by $(4\pm3)\%$, $(6\pm2)\%$ and $(10\pm2)\%$, respectively. Under our initial conditions, a satellite having up to 20\% of the disk mass would produce little observable thickening whereas a 30\% disk-mass satellite produces little observable thickening inside the half-mass radius of the disk but great damage beyond the half-mass radius.

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Mergers and Galaxy Evolution (Sept94 Ringberg Workshop)

Galaxy merging is the late time manifestation of the galaxy formation process and likely significantly effects $z<1$ galaxies. A ``maximum reasonable rate'' model for merging finds a $\sim2$ mag K band increase in the luminosities of dwarf galaxies so that they contribute significantly to the faint counts, with spirals and ellipticals being far less affected. The median $K$ and $I$ redshifts stabilize (and even decrease slightly) at $z\simeq0.6$ beyond I=21 or K=19. The B redshifts continue to rise (although strongly dependent on the UV spectral evolution). Such rapid merging predicts that at $z=1$ the characteristic galaxy mass is reduced to $\sim30\%$ of the $z=0$ value. To rule out this model requires good sampling beyond $z=1$. A theoretical complication for even a minimal merger rate, which reduces $z=1$ masses to 2/3 of current epoch values, is that infall of a single satellite having 10\% of a disk's mass may destroy thin disks. Using completely self-consistent n-body simulations, we show that the primary response of a disk to ``cosmological'' satellites up to 20\% of the disk mass is to {\em tilt} the disk with a temporary warping.

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Velocity Bias in MS1224+20

Velocity bias offers a single parameter ($b_v$) description of the likely segregation of mass and light in a galaxy cluster. The relation between the projected mass profile and the light profile, normalized by the virial $M/L$, is presented as a function of $b_v\equivσ_\ell/σ_ρ$, the ratio of the RMS velocity dispersions of the galaxies and the underlying dark matter. The light distribution does not trace the mass at any radius within the cluster. At the apparent harmonic radius the gravitational mass can exceed the virial mass calculated from the light by about a factor of 2 (or more). The data for the MS1224+20 cluster, covering nearly a decade in radius, are well described by a velocity bias value of $b_v=0.85\pm0.05$, comparable to the n-body estimate of $b_v=0.8\pm0.1$. This particular value will remain tentative until more data are available.

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Testing the Least Action Principle in an Omega_0=1 Universe

The least action principle (LAP) is a dynamically rigorous method for deriving the history of galaxy orbits. In particular it is an Omega_0 test, predicting current epoch galaxy velocities as a function of position and of the cosmological background. It is most usefully applied to in--falling structures, such as the local group, where its application indicates that the preferred cosmological model is Omega_0 = 0.1 and h=0.75 (h is the Hubble parameter in units of 100 Km s^-1 Mpc^-1). The method assumes that all the mass acts as if it were distributed as the visible galaxies. We test the reliability of the LAP to Local Group-like systems extracted from Omega_0=1 N--body simulations. While the orbits of the galaxies are qualitatively well reconstructed, the LAP systematically underestimates the mass of the system. This failure is attributed to the presence of extended halos weakly clustered around visible galaxies which prevent a large fraction of the group mass from being detected by the LAP technique. We conclude that the LAP method cannot rule out an Omega_0=1 value on the Local Group scale. Better constraints on Omega_0 may be obtained by applying this technique to in--falling systems, such as clusters, containing objects with separations large compared to galaxy sizes.

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Velocity Bias in Clusters

Hierarchical gravitational clustering creates galaxies that usually do not fully share the dynamical history of an average particle in the mass field. In particular, galaxy tracers identified in numerical simulations can have individual velocity dispersions in virialized regions a factor \bvs\ lower than the dark matter. The field average of the pairwise velocity dispersion depends on the statistical weighting of collapsed regions, so that the tracer pairwise dispersion is a different factor, \bvp, times the density field value. A model of a cool equilibrium tracer population demonstrates that mass to light segregation is very sensitive to single particle velocity bias. For the $ϕ=-GM/(r+a)$ potential a $\bvs=0.9$ tracer indicates a virial mass about a factor of 5 low. The likely value of \bvs\ is estimated and the simple equilibrium model is tested for applicability using a $10^6$ particle simulation of the formation of a single cluster from cosmological initial conditions. From this simulation, the value of \bvs\ is estimated as $0.8\pm0.1$. The pairwise velocity dispersion bias, \bvp, which is equal to \bvs\ augmented with any anti-bias of galaxies against high velocity dispersion clusters. The value of \bvp\ is estimated to be 15\% less than \bvs, consequently $\bvp=0.6^{+0.2}_{-0.1}$. Comparison of cluster mass and luminosity profiles at large radii is a test for the existence of single particle velocity bias. [compressed postscript file cluster.ps.Z via anonymous ftp from orca.astro.washington.edu in ~ftp/pub/hpcc, or carlberg@astro.washington.edu]

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Lensing from the Light-Traces-Mass Map of MS1224+20

The MS1224+20 cluster of galaxies is a high luminosity X-ray source at z=0.325. To compare the lensing mass to the virial mass we have completed a uniform, high precision redshift survey over a field of $7\arcm\times9\arcm$, obtaining 75 redshifts. The velocity dispersion of 30 cluster galaxies is $775$ \kms\ and the projected harmonic radius is 0.32 \hmpc. The virial mass is $2.1\times 10^{14} h^{-1} \msun$. Correcting for faint cluster galaxies without redshifts and allowing for a modest evolution in the galaxy luminosity function gives a current epoch mass-to-light ratio $M/L_V(0)=255h \msun/\lsun$. The same field contains a $z=0.225$ cluster with $σ_v\simeq 500$ \kms, and a group at $z=0.412$ with $σ_v\simeq 400$ \kms. The clusters' gravitational field induces image ellipticities that are calculated from the light-traces-mass density distribution and compared to the observed average tangential distortions from Fahlman \et (1994). Between 1.5 and 3 virial radii, the observed lensing distortions are $4\pm2$ times stronger than the light-traces-mass model and the virial M/L predict.

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