39 results on '"R J McLure"'
Search Results
2. The VANDELS ESO public spectroscopic survey: observations and first data release
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Pentericci, L., Garilli, R. J. McLure B., Cucciati, O., Franzetti, P., Iovino, A., Amorin, R., Bolzonella, M., Bongiorno, A., Carnall, A. C., Castellano, M., Cimatti, A., Cirasuolo, M., Cullen, F., DeBarros, S., Dunlop, J. S., Elbaz, D., Finkelstein, S., Fontana, A., Fontanot, F., Fumana, M., Gargiulo, A., Guaita, L., Hartley, W., Jarvis, M., Juneau, S., Karman, W., Maccagni, D., Marchi, F., Marmol-Queralto, E., Nandra, K., Pompei, E., Pozzetti, L., Scodeggio, M., Sommariva, V., Talia, M., Almaini, O., Balestra, I., Bardelli, S., Bell, E. F., Bourne, N., Bowler, R. A. A., Brusa, M., Buitrago, F., Caputi, C., Cassata, P., Charlot, S., Citro, A., Cresci, G., Cristiani, S., Curtis-Lake, E., Dickinson, M., Faber, S. M., Fazio, G., Ferguson, H. C., Fiore, F., Franco, M., Fynbo, J. P. U., Galametz, A., Georgakakis, A., Giavalisco, M., Grazian, A., Hathi, N. P., Jung, I., Kim, S., Koekemoer, A. M., Khusanova, Y., Fèvre, O. Le, Lotz, J., Mannucci, F., Maltby, D., Matsuoka, K., McLeod, D., Mendez-Hernandez, H., Mendez-Abreu, J., Mignoli, M., Moresco, M., Mortlock, A., Nonino, M., Pannella, M., Papovich, C., Popesso, P., Rosario, D. J., Rosati, P., Salvato, M., Santini, P., Schaerer, D., Schreiber, C., Stark, D., Tasca, L. A. M., Thomas, R., Treu, T., Vanzella, E., Wild, V., Williams, C., Zamorani, G., and Zucca, E.
- Subjects
Astrophysics - Astrophysics of Galaxies - Abstract
This paper describes the observations and the first data release (DR1) of the ESO public spectroscopic survey "VANDELS, a deep VIMOS survey of the CANDELS CDFS and UDS fields". VANDELS' main targets are star-forming galaxies at 2.4
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- 2018
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3. The evolution of the galaxy UV luminosity function at redshifts z ≃ 8 – 15 from deep JWST and ground-based near-infrared imaging
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C T Donnan, D J McLeod, J S Dunlop, R J McLure, A C Carnall, R Begley, F Cullen, M L Hamadouche, R A A Bowler, D Magee, H J McCracken, B Milvang-Jensen, A Moneti, and T Targett
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- 2022
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4. Maximizing the power of deep extragalactic imaging surveys with the James Webb Space Telescope
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T W Kemp, J S Dunlop, R J McLure, C Schreiber, A C Carnall, and F Cullen
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- 2019
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5. Obscured star formation in bright z ≃ 7 Lyman-break galaxies
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R A A Bowler, N Bourne, J S Dunlop, R J McLure, and D J McLeod
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- 2018
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6. The ultraviolet continuum slopes (β) of galaxies at z ≃ 8 − 16 from JWST and ground-based near-infrared imaging
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Fergus Cullen, R J McLure, D J McLeod, J S Dunlop, C T Donnan, A C Carnall, R A A Bowler, R Begley, M L Hamadouche, and T M Stanton
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formation [galaxies] ,Space and Planetary Science ,starburst [galaxies] ,Astronomy and Astrophysics ,dark ages, reionization, first stars ,evolution [galaxies] ,high-redshift [galaxies] - Abstract
We study the rest-frame ultraviolet (UV) continuum slopes (β) of galaxies at redshifts 8 < z < 16 (〈z〉 = 10), using a combination of James Webb Space Telescope (JWST) ERO and ERS NIRCam imaging and ground-based near-infrared imaging of the COSMOS field. The combination of JWST and ground-based imaging provides a wide baseline in both redshift and absolute UV magnitude (−22.6 < MUV < −17.9), sufficient to allow a meaningful comparison to previous results at lower redshift. Using a power-law fitting technique, we find that our full sample (median MUV = −19.3 ± 1.3) returns an inverse-variance weighted mean value of 〈β〉 = −2.10 ± 0.05, with a corresponding median value of β = −2.29 ± 0.09. These values imply that the UV colours of galaxies at z > 8 are, on average, no bluer than the bluest galaxies in the local Universe (e.g., NGC 1705; β = −2.46). We find evidence for a β − MUV relation, such that brighter UV galaxies display redder UV slopes (dβ/dMUV=−0.17±0.05). Comparing to results at lower redshift, we find that the slope of our β − MUV relation is consistent with the slope observed at z ≃ 5 and that, at a given MUV, our 8 < z < 16 galaxies are bluer than their z ≃ 5 counterparts, with an inverse-variance weighted mean offset of 〈Δβ〉 = −0.38 ± 0.09. We do not find strong evidence that any objects in our sample display ultra-blue UV continuum slopes (i.e., β ≲ −3) that would require their UV emission to be dominated by ultra-young, dust-free stellar populations with high Lyman-continuum escape fractions. Comparing our results to the predictions of theoretical galaxy formation models, we find that the galaxies in our sample are consistent with the young, metal-poor and moderately dust-reddened galaxies expected at z > 8.
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- 2023
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7. A combined VANDELS and LEGA-C study: the evolution of quiescent galaxy size, stellar mass, and age from z = 0.6 to z = 1.3
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M L Hamadouche, A C Carnall, R J McLure, J S Dunlop, D J McLeod, F Cullen, R Begley, M Bolzonella, F Buitrago, M Castellano, O Cucciati, A Fontana, A Gargiulo, M Moresco, L Pozzetti, and G Zamorani
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Space and Planetary Science ,Astronomy and Astrophysics ,star formation [galaxies] ,evolution [galaxies] ,high-redshift [galaxies] - Abstract
We study the relationships between stellar mass, size, and age within the quiescent population, using two mass-complete spectroscopic samples with log10(M⋆/M⊙) > 10.3, taken from VANDELS at 1.0 < z < 1.3, and LEGA-C at 0.6 < z < 0.8. Using robust Dn4000 values, we demonstrate that the well-known ‘downsizing’ signature is already in place by z ≃ 1.1, with Dn4000 increasing by ≃ 0.1 across a ≃ 1 dex mass interval for both VANDELS and LEGA-C. We then proceed to investigate the evolution of the quiescent galaxy stellar mass–size relation from z ≃ 1.1 to z ≃ 0.7. We find the median size increases by a factor of 1.9 ± 0.1 at log10(M⋆/M⊙) = 10.5, and see tentative evidence for flattening of the relation, finding slopes of α = 0.72 ± 0.06 and α=0.56±0.04 for VANDELS and LEGA-C, respectively. We finally split our sample into galaxies above and below our fitted mass–size relations, to investigate how size and Dn4000 correlate. For LEGA-C, we see a clear difference, with larger galaxies found to have smaller Dn4000 at fixed stellar mass. Due to the faintness and smaller numbers of the VANDELS sample, we cannot confirm whether a similar relation exists at z ≃ 1.1. We consider whether differences in stellar age or metallicity are most likely to drive this size–Dn4000 relation, finding that any metallicity differences are unlikely to fully explain the observed offset, meaning smaller galaxies must be older than their larger counterparts. We find the observed evolution in size, mass, and Dn4000 across the ≃ 2 Gyr from z ∼ 1.1 to z ∼ 0.7 can be explained by a simple toy model in which VANDELS galaxies evolve passively whilst experiencing a series of minor mergers.
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- 2022
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8. The connection between stellar mass, age and quenching timescale in massive quiescent galaxies at $z \simeq 1$
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M L Hamadouche, A C Carnall, R J McLure, J S Dunlop, R Begley, F Cullen, D J McLeod, C T Donnan, and T M Stanton
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Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,FOS: Physical sciences ,Astronomy and Astrophysics ,star formation [galaxies] ,Astrophysics - Astrophysics of Galaxies ,evolution [galaxies] ,high-redshift [galaxies] - Abstract
We present a spectro-photometric study of a mass-complete sample of quiescent galaxies at $1.0 < z < 1.3$ with $\mathrm{log_{10}}(M_{\star}/\mathrm{M_{\odot}}) \geq 10.3$ drawn from the VANDELS survey, exploring the relationship between stellar mass, age and star-formation history. Within our sample of 114 galaxies, we derive a stellar-mass vs stellar-age relation with a slope of $1.20^{+0.28}_{-0.27}$ Gyr per decade in stellar mass. When combined with recent literature results, we find evidence that the slope of this relation remains consistent over the redshift interval $0, Comment: Accepted for publication in MNRAS, 11 pages, 6 figures
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- 2023
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9. A first look at the SMACS0723 JWST ERO:spectroscopic redshifts, stellar masses, and star-formation histories
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A C Carnall, R Begley, D J McLeod, M L Hamadouche, C T Donnan, R J McLure, J S Dunlop, B Milvang-Jensen, C L Bondestam, F Cullen, S M Jewell, and C L Pollock
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RELEASE ,astro-ph.GA ,IMAGES ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics - Astrophysics of Galaxies ,star formation [Galaxies] ,FORMATION RATES ,GALAXY ,high-redshift [Galaxies] ,RESOLUTION ,Space and Planetary Science ,ULTRA-DEEP FIELD ,LUMINOSITY FUNCTION ,Astrophysics of Galaxies (astro-ph.GA) ,distances and redshifts [Galaxies] ,POPULATION - Abstract
We present a first-look analysis of the JWST ERO data in the SMACS J0723.3-7327 cluster field. We begin by reporting 10 new spectroscopic redshifts from $\lambda_\mathrm{obs}=1.8-5.2\mu$m NIRSpec medium-resolution ($R=\lambda/\Delta\lambda = 1000$) data. These are determined via multiple high-SNR emission line detections, with 5 objects at $1 < z < 3$ displaying multiple rest-frame near-infrared Hydrogen Paschen lines, and 5 objects at $5 < z < 9$ displaying rest-frame optical Oxygen and Hydrogen Balmer lines. For the 5 higher-redshift galaxies we extract fluxes in 6 NIRCam bands spanning $\lambda_\mathrm{obs}=0.8-5\mu$m and perform spectral energy distribution fitting, in combination with existing HST photometry. The $7 < z < 9$ objects exhibit a U-shaped pattern across the F277W, F356W and F444W bands, indicating a Balmer break seen in emission (Balmer jump) and high-equivalent-width [O\,\textsc{iii}] emission. This indicates an extremely young stellar population, with the bulk of the current mass having formed within the past 10 Myr. We report robust stellar masses and mean stellar ages from our spectral fitting, with the four $z > 6$ galaxies exhibiting low stellar masses from log$_{10}(M_*/$M$_\odot)=7.1-8.2$ and correspondingly young mean stellar ages of only a few Myr. This work highlights the critical importance of combining large upcoming NIRCam surveys with NIRSpec follow-up to measure the spectroscopic redshifts necessary to robustly constrain physical parameters., Comment: 5 pages, 2 figures, 2 tables, accepted for publication in MNRAS Letters
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- 2023
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10. The abundance of $z \gtrsim 10$ galaxy candidates in the HUDF using deep JWST NIRCam medium-band imaging
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C T Donnan, D J McLeod, R J McLure, J S Dunlop, A C Carnall, F Cullen, and D Magee
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formation [galaxies] ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,FOS: Physical sciences ,Astronomy and Astrophysics ,high redshift [galaxies] ,Astrophysics - Astrophysics of Galaxies ,evolution [galaxies] - Abstract
We utilise JWST NIRCam medium-band imaging to search for extreme redshift ($z \geq 9.5$) galaxy candidates in the Hubble Ultra Deep Field (HUDF) and the additional pointing within the GOODS-South field provided by the second NIRCam module. Our search reveals 6 robust candidates, 3 of which have recently been spectroscopically confirmed. One of these 3 is the previously controversial $z \simeq 12$ galaxy candidate UDF-22980 which is now detected in five JWST NIRCam medium-band filters (F182M, F210M, F430M, F460M and F480M), efficiently excluding alternative low-redshift solutions and allowing us to now report a secure photometric redshift of $z = 11.6 \pm 0.2$. We also detect 2 galaxies at $z \geq 12.5$ including a newly-detected candidate in the imaging provided by the second NIRCam module (south-west of the HUDF) at $z = 12.6 \pm 0.6$. We determine the physical properties of the 6 galaxies by fitting the 14-band photometry with Bagpipes. We find stellar masses of $\log(M_{\star}/{\rm {M_{\odot}}}) \simeq 7.5 - 8.7$ and star-formation rates of $\log(\rm{SFR}/M_{\odot}^{-1} \rm{yr}^{-1}) \simeq 0.3 - 5.0$. Despite the relatively small cosmological volume covered by the HUDF itself and the second NIRCam module imaging, we find that the existence of these galaxies is fully consistent with the latest measurements of both the UV luminosity function and cosmic star-formation rate density at $z\simeq11$, supporting a gradual steady decline in the cosmic star-formation rate density out to at least $z\simeq15$., 8 pages, 4 figures, accepted for publication in MNRAS
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- 2022
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11. The evolution of the mass-metallicity relations from the VANDELS survey and the GAEA Semi-Analytic model
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Johan P. U. Fynbo, Pascale Hibon, Gabriella De Lucia, Filippo Mannucci, Ricardo Amorín, Margherita Talia, R. J. McLure, A. Calabrò, O. Cucciati, M. Castellano, Lucia Pozzetti, Angela Bongiorno, Nimish P. Hathi, Fergus Cullen, Fabio Fontanot, Anna Gallazzi, Michaela Hirschmann, Lizhi Xie, Laura Pentericci, Micol Bolzonella, Giovanni Cresci, Fontanot F., Calabro A., Talia M., Mannucci F., Castellano M., Cresci G., De Lucia G., Gallazzi A., Hirschmann M., Pentericci L., Xie L., Amorin R., Bolzonella M., Bongiorno A., Cucciati O., Cullen F., Fynbo J.P.U., Hathi N., Hibon P., McLure R.J., and Pozzetti L.
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SPECTROSCOPIC SURVEY ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,formation [galaxies] ,Stellar mass ,Metallicity ,CONSISTENT ,FOS: Physical sciences ,Context (language use) ,Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,abundances [galaxies] ,STAR-FORMING GALAXIES ,SPECTRA ,galaxies: formation ,evolution [galaxies] ,Astrophysics::Galaxy Astrophysics ,Physics ,Star formation ,CANDELS ,Analytic model ,Astronomy and Astrophysics ,CHEMICAL ABUNDANCES ,Astrophysics - Astrophysics of Galaxies ,AGES ,Galaxy ,Redshift ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,STELLAR MASS ,galaxies: evolution ,NEBULAE ,galaxies: Abundance ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
In this work, we study the evolution of the mass-metallicity relations (MZRs) as predicted by the GAlaxy Evolution and Assembly (GAEA) semi-analytic model. We contrast these predictions with recent results from the VANDELS survey, that allows us to expand the accessible redshift range for the stellar MZR up to $z\sim3.5$. We complement our study by considering the evolution of the gas-phase MZR in the same redshift range. We show that GAEA is able to reproduce the observed evolution of the $z, 12 pages, 8 figures, MNRAS accepted, replaced to match the published version
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- 2021
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12. The discovery of rest-frame UV colour gradients and a diversity of dust morphologies in bright z ~ 7 Lyman-break galaxies
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R A A Bowler, F Cullen, R J McLure, J S Dunlop, and A Avison
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Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,Astrophysics::Solar and Stellar Astrophysics ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics::Earth and Planetary Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Astrophysics::Galaxy Astrophysics ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
We present deep ALMA dust continuum observations for a sample of luminous ($M_{\rm UV} < -22$) star-forming galaxies at $z \simeq 7$. We detect five of the six sources in the far-infrared (FIR), providing key constraints on the obscured star-formation rate (SFR) and the infrared-excess-$\beta$ (IRX-$\beta$) relation without the need for stacking. Despite the galaxies showing blue rest-frame UV slopes ($\beta \simeq -2$) we find that 35-75 percent of the total SFR is obscured. We find the IRX-$\beta$ relation derived for these $z \simeq 7$ sources is consistent with that found for local star-burst galaxies. Using our relatively high-resolution (FWHM $\simeq 0.7\,{\rm arcsec}$) observations we identify a diversity of dust morphologies in the sample. We find both compact emission that appears offset relative to the unobscured components and extended dust emission that is co-spatial with the rest-frame UV light. In the majority of the sources we detect strong rest-frame UV colour gradients (with up to $\Delta \beta \simeq 0.7$-$1.4$) as probed by the multi-band UltraVISTA ground-based data. The observed redder colours are spatially correlated with the location of the FIR detection. Our results show that even in bright Lyman-break galaxies at $z \simeq 7$ the peak of the star-formation is typically hosted by the fainter, redder, regions in the rest-frame UV, which have an obscured fraction of $f_{\rm obs} \ge 0.8$. As well as demonstrating the importance of dust obscured star-formation within the Epoch of Reionization, these observations provide an exciting taster of the rich spatially resolved datasets that will be obtained from JWST and high-resolution ALMA follow-up at these redshifts., Comment: 14 pages, 6 figures, 3 tables. Updated to MNRAS accepted version
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- 2021
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13. The VANDELS ESO public spectroscopic survey: observations and first data release
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O. Cucciati, Andrea Grazian, E. Zucca, Y. Khusanova, Emma Curtis-Lake, A. Iovino, Stéphane Charlot, R. J. McLure B. Garilli, James Dunlop, Adriana Gargiulo, Johan P. U. Fynbo, Alice Mortlock, Mara Salvato, E. Mármol-Queraltó, Nimish P. Hathi, Seock-Sam Kim, L. A. M. Tasca, Fabrizio Fiore, Italo Balestra, Kirpal Nandra, A. Georgakakis, Emanuela Pompei, D. Elbaz, Anton M. Koekemoer, S. L. Finkelstein, F. Marchi, M. Franco, Maurilio Pannella, Tommaso Treu, Audrey Galametz, Corentin Schreiber, H. Mendez-Hernandez, Andrea Cimatti, P. Popesso, M. Fumana, Giovanni G. Fazio, S. Cristiani, Angela Bongiorno, David J. Rosario, Laura Pentericci, Marco Castellano, Piero Rosati, Vivienne Wild, Giovanni Cresci, A. C. Carnall, C. Caputi, M. Giavalisco, Paolo Cassata, Lucia Pozzetti, Marcella Brusa, M. Bolzonella, R. C. Thomas, Margherita Talia, D. Maccagni, S. Bardelli, W. Karman, S. DeBarros, K. Matsuoka, H. C. Ferguson, Jennifer M. Lotz, F. Fontanot, Adriano Fontana, C. Papovich, W. G. Hartley, Michele Moresco, Eros Vanzella, David T. Maltby, Omar Almaini, S. Juneau, Rebecca A. A. Bowler, Daniel Schaerer, Daniel P. Stark, Nathan Bourne, S. M. Faber, D. J. McLeod, Ricardo Amorín, Michele Cirasuolo, P. Franzetti, Fernando Buitrago, O. Le Fevre, Annalisa Citro, Mario Nonino, Fergus Cullen, Intae Jung, G. Zamorani, Eric F. Bell, Lucia Guaita, Christina C. Williams, V. Sommariva, Marco Scodeggio, M. Mignoli, Matt J. Jarvis, Mark Dickinson, P. Santini, Jairo Méndez-Abreu, F. Mannucci, ITA, USA, GBR, FRA, DEU, INAF - Osservatorio Astronomico di Roma (OAR), Istituto Nazionale di Astrofisica (INAF), INAF - Osservatorio Astronomico di Milano (OAM), INAF - Osservatorio Astronomico di Bologna (OABO), INAF - Osservatorio Astronomico di Brera (OAB), Università di Bologna, Dipartimento di Astronomia, Università di Bologna [Bologna] (UNIBO), INAF - Osservatorio Astronomico di Bologna (OAB), Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7), CNR-INFM CRS-Soft, c/o Dipartimento di Fisica, CNR-INFM CRS-Soft, Centre for Astrophysics Research [Hatfield], University of Hertfordshire [Hatfield] (UH), INAF-IASF Milano, European Southern Observatory (ESO), University of Bologna, INAF - Osservatorio Astronomico di Trieste (OAT), Dipartimento di Fisica e Astronomia [Bologna], University of Groningen [Groningen], Laboratoire d'Astrophysique de Marseille (LAM), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Aix Marseille Université (AMU)-Centre National d'Études Spatiales [Toulouse] (CNES), Osservatorio Astronomico (INAF), NOAO, Max-Planck-Institut für Extraterrestrische Physik (MPE), Department of Astronomy [Amherst], University of Massachusetts [Amherst] (UMass Amherst), University of Massachusetts System (UMASS)-University of Massachusetts System (UMASS), INAF - Osservatorio Astrofisico di Arcetri (OAA), Space Telescope Science Institute (STSci), Department of computer science, Kyushu Institute of Technology, University of Texas-Pan American (UTPA), University of Texas-Pan, Excellence Cluster Universe, Technische Universität München [München] (TUM), Institut de recherche en astrophysique et planétologie (IRAP), Université Toulouse III - Paul Sabatier (UT3), Université Fédérale Toulouse Midi-Pyrénées-Université Fédérale Toulouse Midi-Pyrénées-Observatoire Midi-Pyrénées (OMP), Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS), California Institute of Technology (CALTECH), Alma Mater Studiorum Università di Bologna [Bologna] (UNIBO), National Optical Astronomy Observatory (NOAO), Technische Universität Munchen - Université Technique de Munich [Munich, Allemagne] (TUM), Institut national des sciences de l'Univers (INSU - CNRS)-Université Toulouse III - Paul Sabatier (UT3), Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Université Fédérale Toulouse Midi-Pyrénées-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Centre National de la Recherche Scientifique (CNRS), University of St Andrews. School of Physics and Astronomy, Astrophysique Interprétation Modélisation (AIM (UMR7158 / UMR_E_9005 / UM_112)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), University of Bologna/Università di Bologna, Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS), Kyushu Institute of Technology (Kyutech), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS), Astronomy, Pentericci, L., McLure, R. J., Garilli, B., Cucciati, O., Franzetti, P., Iovino, A., Amorin, R., Bolzonella, M., Bongiorno, A., Carnall, A. C., Castellano, M., Cimatti, A., Cirasuolo, M., Cullen, F., De Barros, S., Dunlop, J. S., Elbaz, D., Finkelstein, S. L., Fontana, A., Fontanot, F., Fumana, M., Gargiulo, A., Guaita, L., Hartley, W. G., Jarvis, M. J., Juneau, S., Karman, W., Maccagni, D., Marchi, F., Marmol-Queralto, E., Nandra, K., Pompei, E., Pozzetti, L., Scodeggio, M., Sommariva, V., Talia, M., Almaini, O., Balestra, I., Bardelli, S., Bell, E. F., Bourne, N., Bowler, R. A. A., Brusa, M., Buitrago, F., Caputi, K. I., Cassata, P., Charlot, S., Citro, A., Cresci, G., Cristiani, S., Curtis-Lake, E., Dickinson, M., Fazio, G. G., Ferguson, H. C., Fiore, F., Franco, M., Fynbo, J. P. U., Galametz, A., Georgakakis, A., Giavalisco, M., Grazian, A., Hathi, N. P., Jung, I., Kim, S., Koekemoer, A. M., Khusanova, Y., Le Fèvre, O., Lotz, J. M., Mannucci, F., Maltby, D. T., Matsuoka, K., McLeod, D. J., Mendez-Hernandez, H., Mendez-Abreu, J., Mignoli, M., Moresco, M., Mortlock, A., Nonino, M., Pannella, M., Papovich, C., Popesso, P., Rosario, D. P., Salvato, M., Santini, P., Schaerer, D., Schreiber, C., Stark, D. P., Tasca, L. A. M., Thomas, R., Treu, T., Vanzella, E., Wild, V., Williams, C. C., Zamorani, G., Zucca, E., Amorin Barbieri, Ricardo [0000-0001-5758-1000], and Apollo - University of Cambridge Repository
- Subjects
media_common.quotation_subject ,REDSHIFT ,Galaxies: fundamental parameter ,FOS: Physical sciences ,Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,01 natural sciences ,surveys ,galaxies: high-redshift ,0103 physical sciences ,Galaxy formation and evolution ,fundamental parameters [galaxies] ,QB Astronomy ,Survey ,Galaxies: evolution ,Galaxies: fundamental parameters ,Galaxies: general ,Galaxies: high-redshift ,Surveys ,Astronomy and Astrophysics ,Space and Planetary Science ,010303 astronomy & astrophysics ,Spectrograph ,evolution [galaxies] ,QC ,ComputingMilieux_MISCELLANEOUS ,Astrophysics::Galaxy Astrophysics ,media_common ,QB ,Physics ,[SDU.ASTR]Sciences of the Universe [physics]/Astrophysics [astro-ph] ,010308 nuclear & particles physics ,galaxies: fundamental parameters ,3rd-DAS ,Astronomy and Astrophysic ,galaxies: general ,Astrophysics - Astrophysics of Galaxies ,Galaxy ,Redshift ,Universe ,Data set ,GALAXIES ,QC Physics ,Sky ,[SDU]Sciences of the Universe [physics] ,Astrophysics of Galaxies (astro-ph.GA) ,VIMOS ,galaxies: evolution ,high-redshift [galaxies] ,Data reduction ,general [galaxies] - Abstract
This paper describes the observations and the first data release (DR1) of the ESO public spectroscopic survey "VANDELS, a deep VIMOS survey of the CANDELS CDFS and UDS fields". VANDELS' main targets are star-forming galaxies at 2.4, Comment: Submitted to A&A
- Published
- 2018
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14. Candels observations of the structural properties of cluster galaxies at z = 1.62
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Duncan Farrah, Dale D. Kocevski, James Dunlop, Boris Häußler, Christopher N. A. Willmer, Yicheng Guo, Steven L. Finkelstein, J. A. Newman, C. J. Conselice, A. van der Wel, R. J. McLure, Jennifer M. Lotz, S. M. Faber, Elizabeth J. McGrath, Anton M. Koekemoer, Avishai Dekel, H. C. Ferguson, R. Bassett, I. Momcheva, G. Rudnick, Daniel H. McIntosh, Kim-Vy Tran, David C. Koo, Keely Finkelstein, Casey Papovich, Eric F. Bell, Stijn Wuyts, and Ben Weiner
- Subjects
SIMILAR-TO 2 ,Field (physics) ,Stellar mass ,Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,HIGH-REDSHIFT GALAXIES ,PASSIVELY EVOLVING GALAXIES ,(XMM-LSS02182-05102) ,cD ,ELLIPTIC GALAXIES ,evolution ,Cluster (physics) ,COLOR-MAGNITUDE RELATION ,STAR-FORMING GALAXIES ,clusters: general [galaxies] ,EXTRAGALACTIC LEGACY SURVEY ,Astrophysics::Galaxy Astrophysics ,[galaxies] ,Physics ,COSMIC cancer database ,clusters: individual [galaxies] ,Star formation ,Astronomy and Astrophysics ,HUBBLE-SPACE-TELESCOPE ,Galaxy ,Redshift ,MASSIVE ,ULTRA-DEEP-FIELD ,Physics and Astronomy ,Space and Planetary Science ,structure [galaxies] ,Wide Field Camera 3 ,MORPHOLOGY-DENSITY RELATION ,elliptical and lenticular [galaxies] ,high-redshift [galaxies] - Abstract
We discuss the structural and morphological properties of galaxies in a z = 1.62 proto-cluster using near-IR imaging data from Hubble Space Telescope Wide Field Camera 3 data of the Cosmic Assembly Near-IR Deep Extragalactic Legacy Survey (CANDELS). The cluster galaxies exhibit a clear color-morphology relation: galaxies with colors of quiescent stellar populations generally have morphologies consistent with spheroids, and galaxies with colors consistent with ongoing star formation have disk-like and irregular morphologies. The size distribution of the quiescent cluster galaxies shows a deficit of compact (≲ 1 kpc), massive galaxies compared to CANDELS field galaxies at z = 1.6. As a result, the cluster quiescent galaxies have larger average effective sizes compared to field galaxies at fixed mass at greater than 90% significance. Combined with data from the literature, the size evolution of quiescent cluster galaxies is relatively slow from z ≃ 1.6 to the present, growing as (1 + z)-0.6 ± 0.1. If this result is generalizable, then it implies that physical processes associated with the denser cluster region seem to have caused accelerated size growth in quiescent galaxies prior to z = 1.6 and slower subsequent growth at z < 1.6 compared to galaxies in the lower density field. The quiescent cluster galaxies at z = 1.6 have higher ellipticities compared to lower redshift samples at fixed mass, and their surface-brightness profiles suggest that they contain extended stellar disks. We argue that the cluster galaxies require dissipationless (i.e., gas-poor or "dry") mergers to reorganize the disk material and to match the relations for ellipticity, stellar mass, size, and color of early-type galaxies in z < 1 clusters. © © 2012. The American Astronomical Society. All rights reserved..
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- 2016
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15. A remarkably high fraction of strong Lyα emitters amongst luminous redshift 6.0 < z < 6.5 Lyman-break galaxies in the UKIDSS Ultra-Deep Survey
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R. J. McLure, Omar Almaini, H. J. Pearce, E. J. Bradshaw, W. G. Hartley, M. Cirasuolo, Daniel Stark, Sylvie Foucaud, Emma Curtis-Lake, James Dunlop, and Robert Chuter
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Physics ,High rate ,010308 nuclear & particles physics ,Continuum (design consultancy) ,Astronomy and Astrophysics ,Astrophysics ,01 natural sciences ,Redshift ,Galaxy ,Luminosity ,Space and Planetary Science ,0103 physical sciences ,010303 astronomy & astrophysics ,Photometric redshift - Abstract
We present spectroscopic confirmation of ten highly luminous (L >= 2L*) Lyman alpha emitters in the redshift range 6.01 = 6 Lyman break galaxies (LBGs) selected from an area of 0.25 square degrees within the UKIDSS Ultra-deep Survey (UDS). Overall, our high rate of spectroscopic confirmation (>= 71%) and low rate of contamination provides a strong vindication of the photometric redshift analysis used to define the original sample. By considering star-formation rate estimates based on the Ly_alpha and UV continuum luminosity we conclude that our sample is consistent with a Ly_alpha escape fraction of ~25%. Moreover, after careful consideration of the potential uncertainties and biases, we find that 40%-50% of our sample of L >= 2L* galaxies at 6.0 = 25 Angs), a fraction which is a factor of ~2 higher than previously reported for L =2 L*) LBGs shows a similarly sharp increase to that observed in their lower-luminosity (L
- Published
- 2012
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16. A critical analysis of the ultraviolet continuum slopes (β) of high-redshift galaxies: no evidence (yet) for extreme stellar populations at z > 6
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R. J. McLure, James Dunlop, Richard S. Ellis, L. de Ravel, Daniel Stark, Brant Robertson, and M. Cirasuolo
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Physics ,education.field_of_study ,010308 nuclear & particles physics ,Continuum (design consultancy) ,Population ,Astronomy and Astrophysics ,Astrophysics ,01 natural sciences ,Galaxy ,Redshift ,Luminosity ,Space and Planetary Science ,0103 physical sciences ,Beta (velocity) ,Extreme value theory ,education ,010303 astronomy & astrophysics ,Noise (radio) - Abstract
It has recently been reported that the faintest galaxies at z~6-7 display extremely blue UV continuum slopes, with a UV power-law index beta ~ -3. Such slopes are bluer than previously reported for any other galaxy population, and imply extinction-free, young, very low-metallicity stellar populations with a high ionizing photon escape fraction. Here we undertake a critical study of the evidence for such extreme values of beta, combining three new WFC3/IR-selected samples of galaxies spanning ~2 decades in UV luminosity over the redshift range z~4.5-8. We explore the impact of inclusion/exclusion of less robust high-z candidates, and use the varying depths of the samples to explore the effects of noise and selection bias. Simple data-consistency arguments suggest that artificially blue average values of beta can result when the analysis is extended into the deepest ~ 0.5-mag bin of these WFC3/IR-selected samples, regardless of the actual luminosity or z range probed. By confining attention to robust, well-detected high-z galaxy candidates, we find that the average value of beta is consistent with -2.05 +/- 0.10 for z=5-7, and -22 < M_UV < -18. We create and analyse a set of simulations which demonstrate that a bias towards artifically low/blue average values of beta is indeed expected when the UV slope analysis is extended towards the source detection threshold, and conclude that there is as yet no clear evidence for UV slopes significantly bluer than beta ~ -2, the typical value displayed by the bluest star-forming galaxies at more modest z. A robust measurement of beta for the faintest galaxies at z~7-8 remains a key observational goal, as it provides a fundamental test for high escape fractions from a potentially abundant source of reionizing photons. This goal is achievable with HST, but requires still deeper WFC3/IR imaging in the HUDF.
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- 2011
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17. Environments of active galactic nuclei at z < 1.5 in the UKIDSS Ultra-Deep Survey
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Omar Almaini, E. J. Bradshaw, James Dunlop, W. G. Hartley, M. Cirasuolo, R. J. McLure, Chris Simpson, Robert Chuter, and C. J. Conselice
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Physics ,education.field_of_study ,010308 nuclear & particles physics ,Infrared ,Astrophysics::High Energy Astrophysical Phenomena ,media_common.quotation_subject ,Population ,Astronomy ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,01 natural sciences ,Galaxy ,Redshift ,Universe ,Space and Planetary Science ,0103 physical sciences ,Density field ,education ,010303 astronomy & astrophysics ,Astrophysics::Galaxy Astrophysics ,media_common - Abstract
We investigate the environments of both X-ray and radio-loud AGN within the UKIDSS Ultra-deep Survey (UDS) using deep infrared selection to sample the galaxy density field in the redshift range 1.0 ~ 10^13 M_sun. A closer look at the small-scale environments of the AGN reveals that the neighbouring galaxies of radio-loud AGN have U-B colours more skewed towards the `green-valley' and the red sequence, whereas the neighbours of X-ray AGN show no difference to the general galaxy population. This suggests that although both AGN types live in overdense environments, the radio-loud AGN may be preferentially located in more evolved cluster cores, in a similar environment to low-powered radio AGN in the local Universe.
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- 2011
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18. Galaxies at z= 6-9 from the WFC3/IR imaging of the Hubble Ultra Deep Field
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Anton M. Koekemoer, James Dunlop, Elena Sabbi, R. J. McLure, Richard S. Ellis, Daniel Stark, M. Cirasuolo, and T. A. Targett
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Physics ,education.field_of_study ,010308 nuclear & particles physics ,Star formation ,Population ,Astronomy ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Hubble Ultra-Deep Field ,01 natural sciences ,Galaxy ,Redshift ,Luminosity ,Space and Planetary Science ,0103 physical sciences ,education ,010303 astronomy & astrophysics ,Astrophysics::Galaxy Astrophysics ,Photometric redshift ,Luminosity function (astronomy) - Abstract
We present the results of a systematic search for galaxies in the redshift range z = 6 - 9, within the new, deep, near-infrared imaging of the Hubble Ultra Deep Field provided by the Wide Field Camera 3 (WFC3) on HST. We have performed full SED fitting to the optical+infrared photometry of all high-redshift galaxy candidates detected at greater than 5-sigma in at least one of the WFC3/IR broad-band filters. After rejection of contaminants, the result is a sample of 49 galaxies with primary redshift solutions z > 5.9. Our sample, selected without recourse to specific colour cuts, re-selects all but the faintest one of the 16 z-drops selected by Oesch et al. (2009), recovers all 5 of the Y-drops reported by Bouwens et al. (2009), and adds a further 29 galaxy candidates, of which 12 lie beyond z = 6.3, and 4 lie beyond z = 7. We also present confidence intervals on our photometric redshift estimates, and caution that acceptable low-redshift (z 6.3, and for all 8 galaxy candidates at z > 7.5. Nevertheless, the very highest redshift candidates appear to be strongly clustered in the field. We derive new estimates of the ultraviolet galaxy luminosity function at z = 7 and z = 8. Where our results are most robust, at a characteristic luminosity M(1500) ~ -19.5 (AB), we find that the comoving number density of galaxies declines by a factor of ~ 2.5 between z = 6 and z = 7, and by a further factor of ~ 2 by z = 8. These results suggest that it is difficult for the observed population of high-redshift star-forming galaxies to achieve reionisation by z ~ 6 without a significant contribution from galaxies well below the detection limits, plus alterations in the escape fraction of ionising photons and/or continued vigorous star formation at z > 15.
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- 2010
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19. Discovery of the galaxy counterpart of HDF 850.1, the brightest submillimetre source in theHubble Deep Field
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J. S. Dunlop, R. J. McLure, T. Yamada, M. Kajisawa, J. A. Peacock, R. G. Mann, D. H. Hughes, I. Aretxaga, T. W. B. Muxlow, A. M. S. Richards, M. Dickinson, R. J. Ivison, G. P. Smith, I. Smail, S. Serjeant, O. Almaini, and A. Lawrence
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Physics ,education.field_of_study ,COSMIC cancer database ,Hubble Deep Field ,Population ,Astronomy and Astrophysics ,Astrophysics ,Galaxy ,Redshift ,law.invention ,Telescope ,Gravitational lens ,Space and Planetary Science ,law ,Elliptical galaxy ,education - Abstract
Despite extensive observational efforts, the brightest sub-mm source in the Hubble Deep Field, HDF850.1, has failed to yield a convincing optical/infrared identifica- tion almost 4 years after its discovery. This failure is all the more notable given the availability of supporting multi-frequency data of unparalleled depth, and sub-arcsec positional accuracy for the sub-mm/mm source. Consequently, HDF850.1 has become a test case of the possibility that the most violently star-forming objects in the universe are too red and/or distant to be seen in the deepest optical images. Here we report the discovery of the host galaxy of HDF850.1. This object has been revealed by careful analysis of a new, deep Kimage of the HDF obtained with the Subaru 8.2-m telescope. Its reality is confirmed by a similar analysis of the HST NICMOS F160W image of the same region. This object is extremely faint (K ≃ 23.5), clumpy (on sub-arcsec scales) and very red (I − K > 5.2; H − K = 1.4 ± 0.35). The likelihood that it is the correct identification is strongly reinforced by a reanalysis of the combined MERLIN+VLA 1.4-GHz map of the field which provides a new radio detection of HDF850.1 only 0.1arcsec from the new near-infrared counterpart, and with sufficient positional accuracy to exclude all previously considered alternative optical candidates. We have calculated new confidence limits on the estimated redshift of HDF850.1 in the light of the new radio detection, and find z = 4.1±0.5. We have also determined the scale-length, and hence estimated the mass of the apparently nearby (0.5arcsec distant) z ≃ 1 elliptical galaxy 3-586.0. From this we calculate that the flux density of HDF850.1 has been boosted by a factor of ≃ 3 through gravitational lensing by this intervening elliptical, consistent with predictions that a small but significant fraction of blank-field sub-mm sources are lensed by foreground galaxies. We discuss the wider implications of these results for the sub-mm population and cosmic star-formation history.
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- 2004
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20. Erratum: Evolution of star formation in the UKIDSS Ultra Deep Survey Field - I. Luminosity functions and cosmic star formation rate out to z = 1.6
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Phil A. James, Masami Ouchi, Yoshiaki Ono, P. N. Best, James Dunlop, Charles E. Simpson, R. J. McLure, Alyssa B. Drake, Chris A. Collins, D. J. B. Smith, Ivan K. Baldry, Gavin Dalton, David Bonfield, and Matt J. Jarvis
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Physics ,010308 nuclear & particles physics ,Star formation ,Astronomy ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Redshift survey ,01 natural sciences ,Redshift ,Galaxy ,Cosmology ,Photometry (optics) ,Space and Planetary Science ,0103 physical sciences ,Emission spectrum ,Subaru Telescope ,010303 astronomy & astrophysics ,Astrophysics::Galaxy Astrophysics - Abstract
We present new results on the cosmic star formation history in the Subaru/XMM–Newton Deep Survey (SXDS)–Ultra Deep Survey (UDS) field out to z = 1.6. We compile narrowband data from the Subaru Telescope and the Visible and Infrared Survey Telescope for Astronomy (VISTA) in conjunction with broad-band data from the SXDS and UDS, to make a selection of 5725 emission-line galaxies in 12 redshift slices, spanning 10 Gyr of cosmic time. We determine photometric redshifts for the sample using 11-band photometry, and use a spectroscopically confirmed subset to fine tune the resultant redshift distribution. We use the maximum-likelihood technique to determine luminosity functions in each redshift slice and model the selection effects inherent in any narrow-band selection statistically, to obviate the retrospective corrections ordinarily required. The deep narrow-band data are sensitive to very low star formation rates (SFRs), and allow an accurate evaluation of the faint end slope of the Schechter function, α. We find that α is particularly sensitive to the assumed faintest broad-band magnitude of a galaxy capable of hosting an emission line, and propose that this limit should be empirically motivated. For this analysis, we base our threshold on the limiting observed equivalent widths of emission lines in the local Universe. We compute the characteristic SFR of galaxies in each redshift slice, and the integrated SFR density, ρSFR. We find our results to be in good agreement with the literature and parametrize the evolution of the SFR density as ρSFR ∝ (1 + z)4.58 confirming a steep decline in star formation activity since z ∼ 1.6. Key words: surveys – galaxies: evolution – galaxies: formation – galaxies: high-redshift – galaxies: star formation – cosmology: observations.
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- 2015
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21. A mass threshold in the number density of passive galaxies at
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V. Sommariva, A. Fontana, A. Lamastra, P. Santini, J. S. Dunlop, M. Nonino, M. Castellano, H. Ferguson, R. J. McLure, A. Galametz, M. Giavalisco, A. Grazian, Y. Lu, N. Menci, A. Merson, D. Paris, L. Pentericci, R. Somerville, T. Targett, and A. M. Koekemoer
- Published
- 2014
22. Constraints on the star-formation rate of
- Author
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M. Castellano, V. Sommariva, A. Fontana, L. Pentericci, P. Santini, A. Grazian, R. Amorin, J. L. Donley, J. S. Dunlop, H. C. Ferguson, F. Fiore, A. Galametz, E. Giallongo, Y. Guo, K.-H. Huang, A. Koekemoer, R. Maiolino, R. J. McLure, D. Paris, D. Schaerer, P. Troncoso, and E. Vanzella
- Published
- 2014
23. The bright end of the galaxy luminosity function at z\xfd=7: before the onset of mass quenching?
- Author
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R. A. A. Bowler, J. S. Dunlop, R. J. McLure, A. B. Rogers, H. J. McCracken, B. Milvang-Jensen, H. Furusawa, J. P. U. Fynbo, Y. Taniguchi, J. Afonso, M. N. Bremer, and O. Le Fevre
- Published
- 2014
24. The cluster environments of powerful radio-loud and radio-quiet active galactic nuclei
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R. J. McLure and J. S. Dunlop
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Physics ,education.field_of_study ,Active galactic nucleus ,Radio galaxy ,Astrophysics::High Energy Astrophysical Phenomena ,Population ,Significant difference ,Astronomy and Astrophysics ,Quasar ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Amplitude ,Space and Planetary Science ,QUIET ,Cluster (physics) ,education ,Astrophysics::Galaxy Astrophysics - Abstract
The spatial clustering amplitude (B_{gq}) is determined for a sample of 44 powerful AGN at z~0.2. No significant difference is detected in the richness of the cluster environments of the radio-loud and radio-quiet sub-samples, both of which typically inhabit environments as rich as Abell Class ~0. Comparison with radio luminosity-matched samples from Hill & Lilly (1991) and Wold et al. (2000a) suggests that there is no epoch-dependent change in environment richness out to at least z>=0.5 for either radio galaxies or radio quasars. Comparison with the APM cluster survey shows that, contrary to current folklore, powerful AGN do not avoid rich clusters, but rather display a spread in cluster environment which is perfectly consistent with being drawn at random from the massive elliptical population. Finally, we argue that virtually all Abell class ~0 clusters contained an active galaxy during the epoch of peak quasar activity at z~2.5.
- Published
- 2001
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25. A mass threshold in the number density of passive galaxies at z$\sim$2
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V. Sommariva, A. Fontana, A. Lamastra, P. Santini, J. S. Dunlop, M. Nonino, M. Castellano, H. Ferguson, R. J. McLure, A. Galametz, M. Giavalisco, A. Grazian, Y. Lu, N. Menci, A. Merson, D. Paris, L. Pentericci, R. Somerville, T. Targett, and A. M. Koekemoer
- Subjects
Physics ,Number density ,Stellar mass ,Field (physics) ,Star formation ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics ,Function (mathematics) ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Galaxy ,Redshift ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,Galaxy formation and evolution ,Astrophysics::Solar and Stellar Astrophysics ,10. No inequality ,Astrophysics::Galaxy Astrophysics - Abstract
The process that quenched star formation in galaxies at intermediate and high redshift is still the subject of considerable debate. One way to investigate this puzzling issue is to study the number density of quiescent galaxies at z~2, and its dependence on mass. Here we present the results of a new study based on very deep Ks-band imaging (with the HAWK-I instrument on the VLT) of two HST CANDELS fields (the UKIDSS Ultra-deep survey (UDS) field and GOODS-South). The new HAWK-I data (taken as part of the HUGS VLT Large Program) reach detection limits of Ks>26 (AB mag). We select a sample of passively-evolving galaxies in the redshift range 1.422 is real. This has enabled us to establish unambiguously that the number counts of quiescent galaxies at z~2 flatten and slightly decline at magnitudes fainter than Ks~22(AB mag.). We show that this trend corresponds to a stellar mass threshold $M_*10^{10.8}\,{\rm M_{\odot}}$ below which the mechanism that halts the star formation in high-redshift galaxies seems to be inefficient. Finally we compare the observed pBzK number counts with those of quiescent galaxies extracted from four different semi-analytic models. We find that none of the models provides a statistically acceptable description of the number density of quiescent galaxies at these redshifts. We conclude that the mass function of quiescent galaxies as a function of redshift continues to present a key and demanding challenge for proposed models of galaxy formation and evolution., Comment: Accepted for publication on Astronomy and Astrophysics
- Published
- 2014
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26. The unbiased measurement of ultraviolet spectral slopes in low-luminosity galaxies at z \xfd 7
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A. B. Rogers, R. J. McLure, and J. S. Dunlop
- Published
- 2013
27. The ages, masses and star formation rates of spectroscopically confirmed z \xa0 6 galaxies in CANDELS
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E. Curtis-Lake, R. J. McLure, J. S. Dunlop, M. Schenker, A. B. Rogers, T. Targett, M. Cirasuolo, O. Almaini, M. L. N. Ashby, E. J. Bradshaw, S. L. Finkelstein, M. Dickinson, R. S. Ellis, S. M. Faber, G. G. Fazio, H. C. Ferguson, A. Fontana, N. A. Grogin, W. G. Hartley, D. D. Kocevski, A. M. Koekemoer, K. Lai, B. E. Robertson, E. Vanzella, and S. P. Willner
- Published
- 2013
28. Star formation in luminous quasar host galaxies at z = 1-2
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D. J. E. Floyd, J. S. Dunlop, M. J. Kukula, M. J. I. Brown, R. J. McLure, S. A. Baum, and C. P. O'Dea
- Published
- 2013
29. Discovery of bright
- Author
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R. A. A. Bowler, J. S. Dunlop, R. J. McLure, H. J. McCracken, B. Milvang-Jensen, H. Furusawa, J. P. U. Fynbo, O. Le Fxe8vre, J. Holt, Y. Ideue, Y. Ihara, A. B. Rogers, and Y. Taniguchi
- Published
- 2012
30. The size-luminosity relation at
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A. Grazian, M. Castellano, A. Fontana, L. Pentericci, J. S. Dunlop, R. J. McLure, A. M. Koekemoer, M. E. Dickinson, S. M. Faber, H. C. Ferguson, A. Galametz, M. Giavalisco, N. A. Grogin, N. P. Hathi, D. D. Kocevski, K. Lai, J. A. Newman, and E. Vanzella
- Published
- 2012
31. CANDELS OBSERVATIONS OF THE STRUCTURAL PROPERTIES OF CLUSTER GALAXIES AT
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C. Papovich, R. Bassett, J. M. Lotz, A. van der Wel, K.-V Tran, S. L. Finkelstein, E. F. Bell, C. J. Conselice, A. Dekel, J. S. Dunlop, Yicheng Guo, S. M. Faber, D. Farrah, H. C. Ferguson, K. D. Finkelstein, B. Hxe4ussler, D. D. Kocevski, A. M. Koekemoer, D. C. Koo, E. J. McGrath, R. J. McLure, D. H. McIntosh, I. Momcheva, J. A. Newman, G. Rudnick, B. Weiner, C. N. A. Willmer, and S. Wuyts
- Published
- 2012
32. THE NATURE OF EXTREMELY RED
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K. I. Caputi, J. S. Dunlop, R. J. McLure, J.-S. Huang, G. G. Fazio, M. L. N. Ashby, M. Castellano, A. Fontana, M. Cirasuolo, O. Almaini, E. F. Bell, M. Dickinson, J. L. Donley, S. M. Faber, H. C. Ferguson, M. Giavalisco, N. A. Grogin, D. D. Kocevski, A. M. Koekemoer, D. C. Koo, K. Lai, J. A. Newman, and R. S. Somerville
- Published
- 2012
33. The stellar mass function of the most-massive galaxies at 3 \u2264z < 5 in the UKIDSS Ultra Deep Survey
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K. I. Caputi, M. Cirasuolo, J. S. Dunlop, R. J. McLure, D. Farrah, and O. Almaini
- Published
- 2011
34. A
- Author
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C. Papovich, I. Momcheva, C. N. A. Willmer, K. D. Finkelstein, S. L. Finkelstein, K.-V. Tran, M. Brodwin, J. S. Dunlop, D. Farrah, S. A. Khan, J. Lotz, P. McCarthy, R. J. McLure, M. Rieke, G. Rudnick, S. Sivanandam, F. Pacaud, and M. Pierre
- Published
- 2010
35. The environments of active galactic nuclei at 3.6 μm
- Author
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R. J. McLure, Martin J. Hardcastle, Jamie Stevens, Evanthia Hatziminaoglou, Gordon T. Richards, J. T. Falder, Matt J. Jarvis, M. J. Page, and Mark Lacy
- Subjects
Physics ,Active galactic nucleus ,Stellar population ,Radio galaxy ,Astrophysics::High Energy Astrophysical Phenomena ,Astronomy and Astrophysics ,Quasar ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Radius ,Galaxy merger ,Galaxy ,Luminosity ,Space and Planetary Science ,Astrophysics::Galaxy Astrophysics - Abstract
We present an analysis of a large sample of AGN environments at z~1 using stacked Spitzer data at 3.6um. The sample contains type-1 and type-2 AGN in the form of quasars and radio galaxies, and spans a large range in both optical and radio luminosity. We find, on average, that 2 to 3 massive galaxies containing a substantial evolved stellar population lie within a 200-300 kpc radius of the AGN, constituting a >8-sigma excess relative to the field. Secondly, we find evidence for the environmental source density to increase with the radio luminosity of AGN, but not with black-hole mass. This is shown first by dividing the AGN into their classical AGN types, where we see more significant over-densities in the fields of the radio-loud AGN. If instead we dispense with the classical AGN definitions, we find that the source over-density as a function of radio luminosity for all our AGN exhibits a positive correlation. One interpretation of this result is that the Mpc-scale environment is in some way influencing the radio emission that we observe from AGN. This could be explained by the confinement of radio jets in dense environments leading to enhanced radio emission or, alternatively, may be linked to more rapid black-hole spin brought on by galaxy mergers.
- Published
- 2010
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36. A new measurement of the evolving near-infrared galaxy luminosity function out to
- Author
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M. Cirasuolo, R. J. McLure, J. S. Dunlop, O. Almaini, S. Foucaud, and C. Simpson
- Published
- 2010
37. Six more quasars at redshift 6 discovered by the Canada-France High-z Quasar Survey
- Author
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J. Willott P. Delorme C. Reylé L. Albert J. Bergeron D. Crampton X. Delfosse T. Forveille J. B. Hutchings R. J. Mclure A. Omont D. Schade, C., Univers, Transport, Interfaces, Nanostructures, Atmosphère et environnement, Molécules (UMR 6213) (UTINAM), Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Université de Franche-Comté (UFC), Université Bourgogne Franche-Comté [COMUE] (UBFC)-Université Bourgogne Franche-Comté [COMUE] (UBFC), Université de Franche-Comté (UFC), and Université Bourgogne Franche-Comté [COMUE] (UBFC)-Université Bourgogne Franche-Comté [COMUE] (UBFC)-Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)
- Subjects
ComputingMilieux_MISCELLANEOUS - Abstract
International audience
- Published
- 2009
38. A Sample of Radio Galaxies Spanning Three Decades in Radio Luminosity – An Overview
- Author
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Matt J. Jarvis, R. J. McLure, Chris J. Willott, Ewan Mitchell, Steve Rawlings, G. J. Hill, and James S. Dunlop
- Subjects
Luminous infrared galaxy ,Physics ,X-shaped radio galaxy ,Radio galaxy ,Astronomy ,Quasar ,Astrophysics ,Sample (graphics) ,Luminosity function (astronomy) ,Luminosity - Abstract
Multiwavelength mapping of galaxy formation and evolution, 13-16 October 2003, Venice, Italy
- Published
- 2006
- Full Text
- View/download PDF
39. VLA AND ALMA IMAGING OF INTENSE GALAXY-WIDE STAR FORMATION IN z ∼ 2 GALAXIES.
- Author
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W. Rujopakarn, J. S. Dunlop, G. H. Rieke, R. J. Ivison, A. Cibinel, K. Nyland, P. Jagannathan, J. D. Silverman, D. M. Alexander, A. D. Biggs, S. Bhatnagar, D. R. Ballantyne, M. Dickinson, D. Elbaz, J. E. Geach, C. C. Hayward, A. Kirkpatrick, R. J. McLure, M. J. Michałowski, and N. A. Miller
- Subjects
STELLAR evolution ,TIDAL stripping (Astrophysics) ,GALACTIC nuclei ,GALACTIC center ,SOLAR system ,MILKY Way - Abstract
We present ≃0.″4 resolution extinction-independent distributions of star formation and dust in 11 star-forming galaxies (SFGs) at z = 1.3–3.0. These galaxies are selected from sensitive blank-field surveys of the 2′ × 2′ Hubble Ultra-Deep Field at λ = 5 cm and 1.3 mm using the Karl G. Jansky Very Large Array and Atacama Large Millimeter/submillimeter Array. They have star formation rates (SFRs), stellar masses, and dust properties representative of massive main-sequence SFGs at z ∼ 2. Morphological classification performed on spatially resolved stellar mass maps indicates a mixture of disk and morphologically disturbed systems; half of the sample harbor X-ray active galactic nuclei (AGNs), thereby representing a diversity of z ∼ 2 SFGs undergoing vigorous mass assembly. We find that their intense star formation most frequently occurs at the location of stellar-mass concentration and extends over an area comparable to their stellar-mass distribution, with a median diameter of 4.2 ± 1.8 kpc. This provides direct evidence of galaxy-wide star formation in distant blank-field-selected main-sequence SFGs. The typical galactic-average SFR surface density is 2.5 M
⊙ yr−1 kpc−2 , sufficiently high to drive outflows. In X-ray-selected AGN where radio emission is enhanced over the level associated with star formation, the radio excess pinpoints the AGNs, which are found to be cospatial with star formation. The median extinction-independent size of main-sequence SFGs is two times larger than those of bright submillimeter galaxies, whose SFRs are 3–8 times larger, providing a constraint on the characteristic SFR (∼300 M⊙ yr−1 ) above which a significant population of more compact SFGs appears to emerge. [ABSTRACT FROM AUTHOR]- Published
- 2016
- Full Text
- View/download PDF
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