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The Astrophysical Journal | 2005

The Morphology-Density Relation in z ~ 1 Clusters

Marc Postman; Marijn Franx; N. J. G. Cross; B. Holden; Holland C. Ford; G. D. Illingworth; Tomotsugu Goto; R. Demarco; P. Rosati; John P. Blakeslee; K.-V. Tran; N. Benítez; M. Clampin; George F. Hartig; N. Homeier; D. R. Ardila; Frank Bartko; R. J. Bouwens; L. Bradley; T. J. Broadhurst; Robert A. Brown; Christopher J. Burrows; E. S. Cheng; Paul D. Feldman; David A. Golimowski; Caryl Gronwall; L. Infante; Randy A. Kimble; John E. Krist; Michael P. Lesser

We measure the morphology-density relation (MDR) and morphology-radius relation (MRR) for galaxies in seven z ~ 1 clusters that have been observed with the Advanced Camera for Surveys (ACS) on board the Hubble Space Telescope. Simulations and independent comparisons of our visually derived morphologies indicate that ACS allows one to distinguish between E, S0, and spiral morphologies down to z850 = 24, corresponding to L/L* = 0.21 and 0.30 at z = 0.83 and 1.24, respectively. We adopt density and radius estimation methods that match those used at lower redshift in order to study the evolution of the MDR and MRR. We detect a change in the MDR between 0.8 < z < 1.2 and that observed at z ~ 0, consistent with recent work; specifically, the growth in the bulge-dominated galaxy fraction, fE+S0, with increasing density proceeds less rapidly at z ~ 1 than it does at z ~ 0. At z ~ 1 and Σ ≥ 500 galaxies Mpc-2, we find fE+S0 = 0.72 ± 0.10. At z ~ 0, an E+S0 population fraction of this magnitude occurs at densities about 5 times smaller. The evolution in the MDR is confined to densities Σ 40 galaxies Mpc-2 and appears to be primarily due to a deficit of S0 galaxies and an excess of Sp+Irr galaxies relative to the local galaxy population. The fE-density relation exhibits no significant evolution between z = 1 and 0. We find mild evidence to suggest that the MDR is dependent on the bolometric X-ray luminosity of the intracluster medium. Implications for the evolution of the disk galaxy population in dense regions are discussed in the context of these observations.


Astrophysical Journal Supplement Series | 2004

FAINT GALAXIES IN DEEP ADVANCED CAMERA FOR SURVEYS OBSERVATIONS

N. Benítez; Holland C. Ford; R. J. Bouwens; Felipe Menanteau; John P. Blakeslee; Caryl Gronwall; G. D. Illingworth; Gerhardt R. Meurer; T. J. Broadhurst; Mark C. Clampin; Marijn Franx; George F. Hartig; D. Magee; Marco Sirianni; D. R. Ardila; Frank Bartko; Robert A. Brown; Christopher J. Burrows; E. S. Cheng; N. J. G. Cross; Paul D. Feldman; David A. Golimowski; L. Infante; Randy A. Kimble; John E. Krist; Michael P. Lesser; Z. Levay; Andre R. Martel; G. K. Miley; Marc Postman

We present the analysis of the faint galaxy population in the Advanced Camera for Surveys (ACS) Early Release Observation fields VV 29 (UGC 10214) and NGC 4676. Here we attempt to thoroughly consider all aspects relevant for faint galaxy counting and photometry, developing methods which are based on public software and that are easily reproducible by other astronomers. Using simulations we determine the best SExtractor parameters for the detection of faint galaxies in deep HST observations, paying special attention to the issue of deblending, which significantly affects the normalization and shape of the number count distribution. We confirm, as claimed by Bernstein, Freedman and Madore (2002), that Kron-like magnitudes, such as the ones generated by SExtractor, can miss more than half of the light of faint galaxies, what dramatically affects the slope of the number counts. We present catalogs for the VV 29 and NGC 4676 fields with photometry in the g,V and I bands. We also show that combining the bayesian software BPZ with superb ACS data and new spectral templates enables us to estimate reliable photometric redshifts for a significant fraction of galaxies with as few as three filters. After correcting for selection effects, we measure slopes of 0.32+- 0.01 for 22 25.5 can be well approximated in all our filters by a passive luminosity evolution model based on the COMBO-17 luminosity function (\alpha=-1.5), with a strong merging rate following the prescription of Glazebrook et al. (1994), \phi^*\propto (1+Qz), with Q=4.We present the analysis of the faint galaxy population in the Advanced Camera for Surveys (ACS) Early Release Observation fields VV 29 (UGC 10214) and NGC 4676. These observations cover a total area of 26.3 arcmin 2 and have depths close to that of the Hubble Deep Fields in the deepest part of the VV 29 image, with 10 � detection limits for point sources of 27.8, 27.6, and 27.2 AB magnitudes in the g F475W , VF606W ,a ndIF814W bands, respectively. Measuring the faint galaxy number count distribution is a difficult task, with different groups arriving at widely varying results even on the same data set. Here we attempt to thoroughly consider all aspects relevant for faint galaxy counting and photometry, developing methods that are based on public software and that are easily reproducible by other astronomers. Using simulations we determine the best SExtractor parameters for the detection of faint galaxies in deep Hubble Space Telescope observations, paying special attention to the issue of deblending, which significantly affects the normalization and shape of the number count distribution. We confirm, as claimed by Bernstein, Freedman, & Madore, that Kron-like magnitudes, such as the ones generated by SExtractor, can miss more than half of the light offaint galaxies, what dramatically affects the slope of the number counts. We show how to correct for this effect, which depends sensitively not only on the characteristics of the observations, but also on the choice of SExtractor parameters. We present catalogs for the VV 29 and NGC 4676 fields with photometry in the F475W, F606W, and F814W bands. We also show that combining the Bayesian software BPZ with superb ACS data and new spectral templates enables us to estimate reliable photometric redshifts for a significant fraction of galaxies with as few as three filters. After correcting for selection effects, we measure slopes of 0:32 � 0:01for 22 25:5 can be well approximated in all our filters by a passive luminosity evolution model based on the COMBO-17 luminosity function (� ¼� 1:5), with a strong merging rate following the prescription of


Astronomical Telescopes and Instrumentation | 1998

Advanced camera for the Hubble Space Telescope

Holland C. Ford; Frank Bartko; Pierre Y. Bely; Tom Broadhurst; Christopher J. Burrows; Edward S. Cheng; Mark Clampin; James H. Crocker; Paul D. Feldman; David A. Golimowski; George F. Hartig; Garth D. Illingworth; Randy A. Kimble; Michael P. Lesser; George H. Miley; Susan G. Neff; Marc Postman; W. B. Sparks; Zlatan I. Tsvetanov; Richard L. White; Pamela C. Sullivan; Carolyn A. Krebs; Douglas B. Leviton; Tom La Jeunesse; William Burmester; Sherri Fike; Rich Johnson; Robert B. Slusher; Paul Volmer; Robert A. Woodruff

The Advanced Camera for the Hubble Space Telescope has three cameras. The first, the Wide Field Camera, will be a high- throughput, wide field, 4096 X 4096 pixel CCD optical and I-band camera that is half-critically sampled at 500 nm. The second, the High Resolution Camera (HRC), is a 1024 X 1024 pixel CCD camera that is critically sampled at 500 nm. The HRC has a 26 inch X 29 inch field of view and 29 percent throughput at 250 nm. The HRC optical path includes a coronagraph that will improve the HST contrast near bright objects by a factor of approximately 10 at 900 nm. The third camera, the solar-blind camera, is a far-UV, pulse-counting array that has a relatively high throughput over a 26 inch X 29 inch field of view. The advanced camera for surveys will increase HSTs capability for surveys and discovery by a factor of approximately 10 at 800 nm.


The Astronomical Journal | 2003

Hubble Space Telescope ACS Coronagraphic Imaging of the Circumstellar Disk around HD 141569A

Mark C. Clampin; John E. Krist; D. R. Ardila; David A. Golimowski; George F. Hartig; Holland C. Ford; G. D. Illingworth; Frank Bartko; N. Benítez; John P. Blakeslee; R. J. Bouwens; T. J. Broadhurst; Robert A. Brown; Christopher J. Burrows; E. S. Cheng; N. J. G. Cross; Paul D. Feldman; Marijn Franx; Caryl Gronwall; L. Infante; R. A. Kimble; Michael P. Lesser; Andre R. Martel; Felipe Menanteau; Gerhardt R. Meurer; G. K. Miley; Marc Postman; P. Rosati; Marco Sirianni; W. B. Sparks

Multicolor coronagraphic images of the circumstellar disk around HD 141569A have been obtained with the Hubble Space Telescope Advanced Camera for Surveys. The B, V, and I images show that the disks previously described multiple-ring structure is actually a continuous distribution of dust with a tightly wound spiral structure. Extending from the disk are two, more open spiral arms, one of which appears to reach the nearby binary star HD 141569BC. Diffuse dust is seen up to 1200 AU from HD 141569A. Although planets may exist in the inner region of the disk, tidal interaction with HD 141569BC seems more likely to be the cause of these phenomena. The disk appears redder than the star (B-V = 0.21 and V-I = 0.25), and its color is spatially uniform. A scattering asymmetry factor of g = 0.25–0.35 is derived. The azimuthal density distribution is asymmetric, varying by a factor of ~3 at some radii.


The Astrophysical Journal | 2003

STAR FORMATION AT z ~ 6: i-DROPOUTS IN THE ADVANCED CAMERA FOR SURVEYS GUARANTEED TIME OBSERVATION FIELDS

R. J. Bouwens; G. D. Illingworth; P. Rosati; C. Lidman; T. J. Broadhurst; Marijn Franx; Holland C. Ford; D. Magee; N. Benítez; John P. Blakeslee; Gerhardt R. Meurer; Mark C. Clampin; George F. Hartig; D. R. Ardila; Frank Bartko; Robert A. Brown; Christopher J. Burrows; E. S. Cheng; N. J. G. Cross; Paul D. Feldman; David A. Golimowski; Caryl Gronwall; Leopoldo Infante; Randy A. Kimble; J. E. Krist; Michael P. Lesser; Andre R. Martel; Felipe Menanteau; G. K. Miley; Marc Postman

Using an i - z dropout criterion, we determine the space density of z ~ 6 galaxies from two deep ACS GTO fields with deep optical-IR imaging. A total of 23 objects are found over 46 arcmin2, or ~0.5 ± 0.1 objects arcmin-2 down to zAB ~ 27.3 (6 σ), or a completeness-corrected ~0.5 ± 0.2 objects arcmin-2 down to zAB ~ 26.5 (including one probable z ~ 6 active galactic nucleus). Combining deep ISAAC data for our RDCS 1252-2927 field (JAB ~ 25.7 and Ks,AB ~ 25.0; 5 σ) and NICMOS data for the Hubble Deep Field-North (J110,AB and H160,AB ~ 27.3, 5 σ), we verify that these dropouts have relatively flat spectral slopes, as one would expect for star-forming objects at z ~ 6. Compared with the average-color (β = -1.3) U-dropout in the Steidel et al. z ~ 3 sample, i-dropouts in our sample range in luminosity from ~1.5L* (zAB ~ 25.6) to ~0.3L* (zAB ~ 27.3) with the exception of one very bright candidate at z850,AB ~ 24.2. The half-light radii vary from 009 to 021, or 0.5 kpc to 1.3 kpc. We derive the z ~ 6 rest-frame UV luminosity density (or star formation rate density) by using three different procedures. All three procedures use simulations based on a slightly lower redshift (z ~ 5) V606-dropout sample from Chandra Deep Field-South ACS images. First, we make a direct comparison of our findings with a no-evolution projection of this V-dropout sample, allowing us to automatically correct for the light lost at faint magnitudes or lower surface brightnesses. We find 23% ± 25% more i-dropouts than we predict, consistent with no strong evolution over this redshift range. Adopting previous results to z ~ 5, this works out to a mere 20% ± 29% drop in the luminosity density from z ~ 3 to z ~ 6. Second, we use the same V-dropout simulations to derive a detailed selection function for our i-dropout sample and compute the UV-luminosity density [(7.2 ± 2.5) × 1025 ergs s-1 Hz-1 Mpc-3 down to zAB ~ 27]. We find a 39% ± 21% drop over the same redshift range (z ~ 3-6), consistent with the first estimate. This is our preferred value and suggests a star formation rate of 0.0090 ± 0.0031 M☉ yr-1 Mpc-3 to zAB ~ 27, or ~0.036 ± 0.012 M☉ yr-1 Mpc-3 by extrapolating the luminosity function to the faint limit, assuming α = -1.6. Third, we follow a very similar procedure, except that we assume no incompleteness, and find a rest-frame continuum luminosity that is ~2-3 times lower than our other two determinations. This final estimate is to be taken as a lower limit and is important if there are modest changes in the colors or surface brightnesses from z ~ 5 to z ~ 6 (the other estimates assume no large changes in the intrinsic selectability of objects). We note that all three estimates are well within the canonical range of luminosity densities necessary for reionization of the universe at this epoch by star-forming galaxies.


The Astronomical Journal | 2005

HUBBLE SPACE TELESCOPE ADVANCED CAMERA FOR SURVEYS CORONAGRAPHIC IMAGING OF THE AU MICROSCOPII DEBRIS DISK

John E. Krist; D. R. Ardila; David A. Golimowski; M. Clampin; Holland C. Ford; G. D. Illingworth; George F. Hartig; Frank Bartko; N. Benítez; John P. Blakeslee; R. J. Bouwens; L. Bradley; T. J. Broadhurst; Robert A. Brown; Christopher J. Burrows; E. S. Cheng; N. J. G. Cross; R. Demarco; Paul D. Feldman; Marijn Franx; Tomotsugu Goto; Caryl Gronwall; B. Holden; N. Homeier; L. Infante; Randy A. Kimble; Michael P. Lesser; Andre R. Martel; S. Mei; Felipe Menanteau

We present Hubble Space Telescope Advanced Camera for Surveys multicolor coronagraphic images of the recently discovered edge-on debris disk around the nearby (� 10 pc) M dwarf AU Microscopii. The disk is seen between r ¼ 0B75 and 15 00 (7.5–150 AU) from the star. It has a thin midplane with a projected FWHM thickness of 2.5–3.5 AU within r < 50 AU of the star that increases to 6.5–9 AU at r � 75 AU. The disk’s radial brightness profile is generally flat forr < 15 AU, then decreases gradually (I / r � 1:8 )o ut tor � 43 AU, beyond which it falls rapidly (I / r � 4:7 ). Within 50 AU the midplane is straight and aligned with the star, and beyond that it deviates by � 3 � , resulting in a bowed appearance that was also seen in ground-based images. Three-dimensional modeling of the disk shows that the inner region (r < 50 AU) is inclined to the line of sight by less than 1 � and the outer disk by � 3 � . The inclination of the outer disk and moderate forward scattering (g � 0:4) can explain the apparentbow. The intrinsic, deprojected FWHM thickness is 1.5–10 AU, increasing with radius. The models indicate that the disk is clear of dust within � 12 AU of the star, in general agreement with the previous prediction of 17 AU based on the infrared spectral energy distribution. The disk is blue, being 60% brighter at B than I relative to the star. One possible explanation for this is that there is a surplus of very small grains compared with other imaged debris disks that have more neutral or red colors. This may be due to the low radiation pressure exerted by the late-type star. Observations at two epochs show that an extended source seen along the midplane is a background galaxy.


The Astrophysical Journal | 2003

ADVANCED CAMERA FOR SURVEYS OBSERVATIONS OF YOUNG STAR CLUSTERS IN THE INTERACTING GALAXY UGC 10214

Hien D. Tran; Marco Sirianni; Holland C. Ford; G. D. Illingworth; Mark C. Clampin; George F. Hartig; Robert H. Becker; Richard L. White; Frank Bartko; N. Benítez; John P. Blakeslee; R. J. Bouwens; T. J. Broadhurst; Robert A. Brown; Christopher J. Burrows; E. S. Cheng; N. J. G. Cross; Paul D. Feldman; Marijn Franx; David A. Golimowski; Caryl Gronwall; Leopoldo Infante; Randy A. Kimble; John E. Krist; Michael P. Lesser; D. Magee; Andre R. Martel; Wm. J. McCann; Gerhardt R. Meurer; George H. Miley

We present the first Advanced Camera for Surveys (ACS) observations of young star clusters in the colliding/merging galaxy UGC 10214. The observations were made as part of the Early Release Observation (ERO) program for the newly installed ACS during service mission SM3B for the Hubble Space Telescope (HST). Many young star clusters can be identified in the tails of UGC 10214, with ages ranging from � 3t o 10 Myr. The extreme blue VI (F606WF814W) colors of the star clusters found in the tail of UGC 10214 can only be explained if strong emission lines are included with a young stellar population. This has been confirmed by our Keck spectroscopy of some of these bright blue stellar knots. The most luminous and largest of these blue knots has an absolute magnitude of MV ¼� 14:45, with a half-light radius of 161 pc, and if it is a single star clus- ter, it would qualify as a super star cluster (SSC). Alternatively, it could be a superposition of multiple scaled OB associations or clusters. With an estimated age of � 4 -5 Myr, its derived mass is less than 1:3 � 10 6 M� . Thus, the young stellar knot is unbound and will not evolve into a normal globular cluster. The bright blue clus- ters and associations are much younger than the dynamical age of the tail, providing strong evidence that star formation occurs in the tail long after it was ejected. UGC 10214 provides a nearby example of processes that contributed to the formation of halos and intracluster media in the distant and younger universe. Subject heading: galaxies: individual (Arp 188, UGC 10214, VV 29) — galaxies: star clusters


Nature | 2004

A large population of ‘Lyman-break’ galaxies in a protocluster at redshift z ≈ 4.1

George K. Miley; Roderik Overzier; Zlatan I. Tsvetanov; R. J. Bouwens; N. Benítez; John P. Blakeslee; Holland C. Ford; Garth D. Illingworth; Marc Postman; P. Rosati; Mark C. Clampin; George F. Hartig; A. Zirm; Huub Röttgering; B. P. Venemans; D. R. Ardila; Frank Bartko; T. J. Broadhurst; Robert A. Brown; Chris Burrows; E. S. Cheng; N. J. G. Cross; Carlos De Breuck; Paul D. Feldman; Marijn Franx; David A. Golimowski; Caryl Gronwall; Leopoldo Infante; Andre R. Martel; Felipe Menanteau

The most massive galaxies and the richest clusters are believed to have emerged from regions with the largest enhancements of mass density relative to the surrounding space. Distant radio galaxies may pinpoint the locations of the ancestors of rich clusters, because they are massive systems associated with ‘overdensities’ of galaxies that are bright in the Lyman-α line of hydrogen. A powerful technique for detecting high-redshift galaxies is to search for the characteristic ‘Lyman break’ feature in the galaxy colour, at wavelengths just shortwards of Lyα, which is due to absorption of radiation from the galaxy by the intervening intergalactic medium. Here we report multicolour imaging of the most distant candidate protocluster, TN J1338–1942 at a redshift z ≈ 4.1. We find a large number of objects with the characteristic colours of galaxies at that redshift, and we show that this excess is concentrated around the targeted dominant radio galaxy. Our data therefore indicate that TN J1338–1942 is indeed the most distant cluster progenitor of a rich local cluster, and that galaxy clusters began forming when the Universe was only ten per cent of its present age.


The Astrophysical Journal | 2003

DISCOVERY OF TWO DISTANT TYPE IA SUPERNOVAE IN THE HUBBLE DEEP FIELD NORTH WITH THE ADVANCED CAMERA FOR SURVEYS

John P. Blakeslee; Zlatan I. Tsvetanov; Adam G. Riess; Holland C. Ford; Garth D. Illingworth; D. Magee; John L. Tonry; N. Benítez; Mark C. Clampin; George F. Hartig; Gerhardt R. Meurer; Marco Sirianni; D. R. Ardila; Frank Bartko; R. J. Bouwens; T. J. Broadhurst; N. J. G. Cross; Paul D. Feldman; Marijn Franx; David A. Golimowski; Caryl Gronwall; Randy A. Kimble; John E. Krist; Andre R. Martel; Felipe Menanteau; George H. Miley; Marc Postman; P. Rosati; W. B. Sparks; Louis-Gregory Strolger

We present observations of the rst two supernovae discovered with the recently installed Advanced Camera for Surveys (ACS) on the Hubble Space Telescope (HST). The supernovae were found in Wide Field Camera images of the Hubble Deep Field North taken with the F775W, F850LP, and G800L optical elements as part of the ACS guaranteed time observation program. Spectra extracted from the ACS G800L grism exposures conrm that the objects are Type Ia supernovae (SNe Ia) at redshifts z = 0 47 and z = 0 95. Follow-up HST observations have been conducted with ACS in F775W and F850LP and with NICMOS in the near-infrared F110W bandpass, yielding a total of 9 ux measurements in the 3 bandpasses over a period of 50 days in the observed frame. We discuss many of the important issues in doing accurate photometry with the ACS. We analyze the multi-band light curves using two different tting methods to calibrate the supernovae luminosities and place them on the SNe Ia Hubble diagram. The resulting distances are consistent with the redshift-distance relation of the accelerating universe model, although evolving intergalactic grey dust remains as a less likely possibility. The relative ease with which these SNe Ia were found, conrmed, and monitored demonstrates the potential ACS holds for revolutionizing the eld of high-redshift SNe Ia, and therefore of testing the accelerating universe cosmology and constraining the iepoch of deceleration.i Subject headings: cosmology: observations o supernovae: general o supernovae: individual (SN 2002dc, SN 2002dd)


The Astrophysical Journal | 2005

The Transformation of Cluster Galaxies at Intermediate Redshift

N. Homeier; R. Demarco; P. Rosati; Marc Postman; John P. Blakeslee; R. J. Bouwens; L. Bradley; Holland C. Ford; Tomotsugu Goto; Caryl Gronwall; B. Holden; M. J. Jee; Andre R. Martel; Simona Mei; Felipe Menanteau; A. Zirm; M. Clampin; George F. Hartig; G. D. Illingworth; D. R. Ardila; Frank Bartko; N. Benítez; T. J. Broadhurst; Robert A. Brown; Christopher J. Burrows; E. S. Cheng; N. J. G. Cross; Paul D. Feldman; Marijn Franx; David A. Golimowski

We combine imaging data from the Advanced Camera for Surveys (ACS) with VLT/FORS optical spectroscopy to study the properties of star-forming galaxies in the z = 0.837 cluster Cl 0152-1357. We have morphological information for 24 star-forming cluster galaxies, which range in morphology from late-type and irregular to compact early-type galaxies. We find that while most star-forming galaxies have r625 - i775 colors bluer than 1.0, eight are in the red cluster sequence. Among the star-forming cluster population, we find five compact early-type galaxies that have properties consistent with their identification as progenitors of dwarf elliptical galaxies. The spatial distribution of the star-forming cluster members is nonuniform. We find none within R ~ 500 Mpc of the cluster center, which is highly suggestive of an intracluster medium interaction. We derive star formation rates from [O II] λ3727 line fluxes and use these to compare the global star formation rate of Cl 0152-1357 to other clusters at low and intermediate redshifts. We find a tentative correlation between integrated star formation rates and TX, in the sense that hotter clusters have lower integrated star formation rates. Additional data from clusters with low X-ray temperatures are needed to confirm this trend. We do not find a significant correlation with redshift, suggesting that evolution is either weak or absent between z = 0.2 and 0.8.

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George F. Hartig

Space Telescope Science Institute

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Holland C. Ford

Space Telescope Science Institute

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Marijn Franx

Kapteyn Astronomical Institute

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Caryl Gronwall

Pennsylvania State University

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Christopher J. Burrows

Space Telescope Science Institute

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Robert A. Brown

Space Telescope Science Institute

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