D. G. Bonfield
University of Hertfordshire
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Science | 2010
M. Negrello; R. Hopwood; G. De Zotti; A. Cooray; A. Verma; J. J. Bock; David T. Frayer; M. A. Gurwell; A. Omont; R. Neri; H. Dannerbauer; L. Leeuw; Elizabeth J. Barton; Jeff Cooke; S. Kim; E. da Cunha; G. Rodighiero; P. Cox; D. G. Bonfield; M. J. Jarvis; S. Serjeant; R. J. Ivison; Simon Dye; I. Aretxaga; David H. Hughes; E. Ibar; Frank Bertoldi; I. Valtchanov; Stephen Anthony Eales; Loretta Dunne
Through a Lens Brightly Astronomical sources detected in the submillimeter range are generally thought to be distant, dusty galaxies undergoing a vigorous burst of star formation. They can be detected because the dust absorbs the light from stars and reemits it at longer wavelengths. Their properties are still difficult to ascertain, however, because the combination of interference from dust and the low spatial resolution of submillimeter telescopes prevents further study at other wavelengths. Using data from the Herschel Space Telescope, Negrello et al. (p. 800) showed that by searching for the brightest sources in a wide enough area in the sky it was possible to detect gravitationally lensed submillimeter galaxies with nearly full efficiency. Gravitational lensing occurs when the light of an astronomical object is deflected by a foreground mass. This phenomenon increases the apparent brightness and angular size of the lensed objects, making it easier to study sources that would be otherwise too faint to probe. Data from the Herschel Space Observatory unveils distant, dusty galaxies invisible to optical telescopes. Gravitational lensing is a powerful astrophysical and cosmological probe and is particularly valuable at submillimeter wavelengths for the study of the statistical and individual properties of dusty star-forming galaxies. However, the identification of gravitational lenses is often time-intensive, involving the sifting of large volumes of imaging or spectroscopic data to find few candidates. We used early data from the Herschel Astrophysical Terahertz Large Area Survey to demonstrate that wide-area submillimeter surveys can simply and easily detect strong gravitational lensing events, with close to 100% efficiency.
The Astrophysical Journal | 2011
A. Lapi; Joaquin Gonzalez-Nuevo; Lulu Fan; A. Bressan; G. De Zotti; L. Danese; M. Negrello; Loretta Dunne; Stephen Anthony Eales; Steve Maddox; Robbie Richard Auld; M. Baes; D. G. Bonfield; S. Buttiglione; A. Cava; D. L. Clements; A. Cooray; Aliakbar Dariush; Simon Dye; J. Fritz; D. Herranz; R. Hopwood; E. Ibar; R. J. Ivison; M. J. Jarvis; S. Kaviraj; M. López-Caniego; M. Massardi; M. J. Michałowski; Enzo Pascale
Exploiting the Herschel Astrophysical Terahertz Large Area Survey Science Demonstration Phase survey data, we have determined the luminosity functions (LFs) at rest-frame wavelengths of 100 and 250 μm and at several redshifts z gsim 1, for bright submillimeter galaxies with star formation rates (SFRs) gsim 100 M ☉ yr–1. We find that the evolution of the comoving LF is strong up to z ≈ 2.5, and slows down at higher redshifts. From the LFs and the information on halo masses inferred from clustering analysis, we derived an average relation between SFR and halo mass (and its scatter). We also infer that the timescale of the main episode of dust-enshrouded star formation in massive halos (M H gsim 3 × 1012 M ☉) amounts to ~7 × 108 yr. Given the SFRs, which are in the range of 102-103 M ☉ yr–1, this timescale implies final stellar masses of the order of 1011-1012 M ☉. The corresponding stellar mass function matches the observed mass function of passively evolving galaxies at z gsim 1. The comparison of the statistics for submillimeter and UV-selected galaxies suggests that the dust-free, UV bright phase is gsim 102 times shorter than the submillimeter bright phase, implying that the dust must form soon after the onset of star formation. Using a single reference spectral energy distribution (SED; the one of the z ≈ 2.3 galaxy SMM J2135-0102), our simple physical model is able to reproduce not only the LFs at different redshifts >1 but also the counts at wavelengths ranging from 250 μm to ≈1 mm. Owing to the steepness of the counts and their relatively broad frequency range, this result suggests that the dispersion of submillimeter SEDs of z > 1 galaxies around the reference one is rather small.
Monthly Notices of the Royal Astronomical Society | 2012
D. J. B. Smith; Loretta Dunne; E. da Cunha; K. Rowlands; Steve Maddox; Haley Louise Gomez; D. G. Bonfield; S. Charlot; Simon P. Driver; Cristina Popescu; Richard J. Tuffs; James Dunlop; M. J. Jarvis; N. Seymour; M. Symeonidis; M. Baes; N. Bourne; D. L. Clements; A. Cooray; G. De Zotti; Simon Dye; Stephen Anthony Eales; D. Scott; A. Verma; P. van der Werf; E. Andrae; R. Auld; S. Buttiglione; A. Cava; A. Dariush
We present a pan-chromatic analysis of an unprecedented sample of 1402 250 μm selected galaxies at z < 0.5 () from the Herschel-ATLAS survey. We complement our Herschel 100–500 μm data with UV–K-band photometry from the Galaxy And Mass Assembly (GAMA) survey and apply the magphys energy-balance technique to produce pan-chromatic spectral energy distributions (SEDs) for a representative sample of 250 μm selected galaxies spanning the most recent 5 Gyr of cosmic history. We derive estimates of physical parameters, including star formation rates, stellar masses, dust masses and infrared (IR) luminosities. The typical H-ATLAS galaxy at z < 0.5 has a far-infrared luminosity in the range 1010–1012 L⊙ (SFR: 1–50 M⊙ yr−1) and thus is broadly representative of normal star-forming galaxies over this redshift range. We show that 250 μm selected galaxies contain a larger mass of dust at a given IR luminosity or star formation rate than previous samples selected at 60 μm from the IRAS. We derive typical SEDs for H-ATLAS galaxies, and show that the emergent SED shape is most sensitive to specific star formation rate. The optical–UV SEDs also become more reddened due to dust at higher redshifts. Our template SEDs are significantly cooler than existing IR templates. They may therefore be most appropriate for inferring total IR luminosities from moderate redshift sub-millimetre selected samples and for inclusion in models of the lower redshift sub-millimetre galaxy populations.
arXiv: Cosmology and Nongalactic Astrophysics | 2010
D. J. B. Smith; Loretta Dunne; Stephen J. Maddox; S. Eales; D. G. Bonfield; M. J. Jarvis; William J. Sutherland; S. Fleuren; E. Rigby; M. A. Thompson; Ivan K. Baldry; Steven P. Bamford; S. Buttiglione; A. Cava; D. L. Clements; A. Cooray; Scott M. Croom; A. Dariush; G. De Zotti; Simon P. Driver; J. S. Dunlop; J. Fritz; D. T. Hill; Andrew M. Hopkins; R. Hopwood; E. Ibar; R. J. Ivison; D. H. Jones; Lee S. Kelvin; L. Leeuw
We present a technique to identify optical counterparts of 250-μm-selected sources from the Herschel–ATLAS survey. Of the 6621 250 μm > 32-mJy sources in our science demonstration catalogue we find that ∼60 per cent have counterparts brighter than r = 22.4 mag in the Sloan Digital Sky Survey. Applying a likelihood ratio technique we are able to identify 2423 of the counterparts with a reliability R > 0.8. This is approximately 37 per cent of the full 250-μm catalogue. We have estimated photometric redshifts for each of these 2423 reliable counterparts, while 1099 also have spectroscopic redshifts collated from several different sources, including the GAMA survey. We estimate the completeness of identifying counterparts as a function of redshift, and present evidence that 250-μm-selected Herschel–ATLAS galaxies have a bimodal redshift distribution. Those with reliable optical identifications have a redshift distribution peaking at z ≈ 0.25 ± 0.05, while submillimetre colours suggest that a significant fraction with no counterpart above the r-band limit have z > 1. We also suggest a method for selecting populations of strongly lensed high-redshift galaxies. Our identifications are matched to UV–NIR photometry from the GAMA survey, and these data are available as part of the Herschel–ATLAS public data release.
Astronomy and Astrophysics | 2010
A. Amblard; A. Cooray; Paolo Serra; P. Temi; Elizabeth J. Barton; M. Negrello; Robbie Richard Auld; M. Baes; Ivan K. Baldry; Steven P. Bamford; A. W. Blain; J. J. Bock; D. G. Bonfield; D. Burgarella; S. Buttiglione; E. Cameron; A. Cava; D. L. Clements; Scott M. Croom; Aliakbar Dariush; G. De Zotti; Simon P. Driver; James Dunlop; Loretta Dunne; Simon Dye; Stephen Anthony Eales; David T. Frayer; J. Fritz; Jonathan P. Gardner; J. González-Nuevo
We present colour-colour diagrams of detected sources in the Herschel-ATLAS science demonstration field from 100 to 500 mu m using both PACS and SPIRE. We fit isothermal modified black bodies to the spectral energy distribution (SED) to extract the dust temperature of sources with counterparts in Galaxy And Mass Assembly (GAMA) or SDSS surveys with either a spectroscopic or a photometric redshift. For a subsample of 330 sources detected in at least three FIR bands with a significance greater than 3 sigma, we find an average dust temperature of (28 +/- 8) K. For sources with no known redshift, we populate the colour-colour diagram with a large number of SEDs generated with a broad range of dust temperatures and emissivity parameters, and compare to colours of observed sources to establish the redshift distribution of this sample. For another subsample of 1686 sources with fluxes above 35 mJy at 350 mu m and detected at 250 and 500 mu m with a significance greater than 3s, we find an average redshift of 2.2 +/- 0.6.
Monthly Notices of the Royal Astronomical Society | 2011
D. J. B. Smith; Loretta Dunne; Steve Maddox; Stephen Anthony Eales; D. G. Bonfield; M. J. Jarvis; W. Sutherland; S. Fleuren; E. Rigby; M. A. Thompson; Ivan K. Baldry; Steven P. Bamford; S. Buttiglione; A. Cava; D. L. Clements; A. Cooray; Scott M. Croom; Aliakbar Dariush; G. De Zotti; Simon P. Driver; James Dunlop; J. Fritz; D. T. Hill; Andrew M. Hopkins; R. Hopwood; E. Ibar; R. J. Ivison; D. H. Jones; Lee S. Kelvin; L. Leeuw
We present a technique to identify optical counterparts of 250-μm-selected sources from the Herschel–ATLAS survey. Of the 6621 250 μm > 32-mJy sources in our science demonstration catalogue we find that ∼60 per cent have counterparts brighter than r = 22.4 mag in the Sloan Digital Sky Survey. Applying a likelihood ratio technique we are able to identify 2423 of the counterparts with a reliability R > 0.8. This is approximately 37 per cent of the full 250-μm catalogue. We have estimated photometric redshifts for each of these 2423 reliable counterparts, while 1099 also have spectroscopic redshifts collated from several different sources, including the GAMA survey. We estimate the completeness of identifying counterparts as a function of redshift, and present evidence that 250-μm-selected Herschel–ATLAS galaxies have a bimodal redshift distribution. Those with reliable optical identifications have a redshift distribution peaking at z ≈ 0.25 ± 0.05, while submillimetre colours suggest that a significant fraction with no counterpart above the r-band limit have z > 1. We also suggest a method for selecting populations of strongly lensed high-redshift galaxies. Our identifications are matched to UV–NIR photometry from the GAMA survey, and these data are available as part of the Herschel–ATLAS public data release.
Monthly Notices of the Royal Astronomical Society | 2010
A. Finoguenov; M. G. Watson; M. Tanaka; Chris Simpson; Michele Cirasuolo; James Dunlop; J. A. Peacock; D. Farrah; Masayuki Akiyama; Yoshihiro Ueda; Vernesa Smolčić; G. C. Stewart; Steve Rawlings; C. van Breukelen; Omar Almaini; Lee Clewley; D. G. Bonfield; M. J. Jarvis; J. M. Barr; S. Foucaud; Ross J. McLure; K. Sekiguchi; E. Egami
We present the results of a search for galaxy clusters in the Subaru–XMM Deep Field (SXDF). We reach a depth for a total cluster flux in the 0.5–2 keV band of 2 × 10^(−15) erg cm^(−2) s^(−1) over one of the widest XMM–Newton contiguous raster surveys, covering an area of 1.3 deg^2. Cluster candidates are identified through a wavelet detection of extended X-ray emission. The red-sequence technique allows us to identify 57 cluster candidates. We report on the progress with the cluster spectroscopic follow-up and derive their properties based on the X-ray luminosity and cluster scaling relations. In addition, three sources are identified as X-ray counterparts of radio lobes, and in three further sources, an X-ray counterpart of the radio lobes provides a significant fraction of the total flux of the source. In the area covered by near-infrared data, our identification success rate achieves 86 per cent. We detect a number of radio galaxies within our groups, and for a luminosity-limited sample of radio galaxies we compute halo occupation statistics using a marked cluster mass function. We compare the cluster detection statistics in the SXDF with that in the literature and provide the modelling using the concordance cosmology combined with current knowledge of the X-ray cluster properties. The joint cluster log(N) − log(S) is overpredicted by the model, and an agreement can be achieved through a reduction of the concordance σ_8 value by 5 per cent. Having considered the dn/dz and the X-ray luminosity function of clusters, we conclude that to pin down the origin of disagreement a much wider (50 deg^2) survey is needed.
Monthly Notices of the Royal Astronomical Society | 2013
M. J. Jarvis; D. G. Bonfield; Victoria Bruce; J. E. Geach; Kim McAlpine; Ross J. McLure; E. Gonzalez-Solares; M. J. Irwin; J. Lewis; A. Küpcü Yoldas; S. Andreon; N. J. G. Cross; James P. Emerson; Gavin Dalton; James Dunlop; S. T. Hodgkin; Fèvre O. Le; Marios Karouzos; Klaus Meisenheimer; Seb Oliver; Steve Rawlings; Chris Simpson; Ian Smail; D. J. B. Smith; M. Sullivan; W. Sutherland; Sarah White; Jonathan Zwart
In this paper we describe the first data release of the the Visible and Infrared Survey Telescope for Astronomy (VISTA) Deep Extragalactic Observations (VIDEO) survey. VIDEO is a ~12degree^2 survey in the near-infrared Z,Y,J,H and K_s bands, specifically designed to enable the evolution of galaxies and large structures to be traced as a function of both epoch and environment from the present day out to z=4, and active galactic nuclei (AGN) and the most massive galaxies up to and into the epoch of reionization. With its depth and area, VIDEO will be able to fully explore the period in the Universe where AGN and starburst activity were at their peak and the first galaxy clusters were beginning to virialize. VIDEO therefore offers a unique data set with which to investigate the interplay between AGN, starbursts and environment, and the role of feedback at a time when it was potentially most crucial. We provide data over the VIDEO-XMM3 tile, which also covers the Canada-France-Hawaii-Telescope Legacy Survey Deep-1 field (CFHTLS-D1). The released VIDEO data reach a 5-sigma AB-magnitude depth of Z=25.7, Y=24.5, J=24.4, H=24.1 and K_s=23.8 in 2 arcsec diameter apertures (the full depth of Y=24.6 will be reached within the full integration time in future releases). The data are compared to previous surveys over this field and we find good astrometric agreement with the Two-Micron All Sky Survey, and source counts in agreement with the recently released UltraVISTA survey data. The addition of the VIDEO data to the CFHTLS-D1 optical data increases the accuracy of photometric redshifts and significantly reduces the fraction of catastrophic outliers over the redshift range 0
Astronomy and Astrophysics | 2010
M. Baes; J. Fritz; Dimitri A. Gadotti; D. J. B. Smith; Loretta Dunne; E. da Cunha; A. Amblard; Robbie Richard Auld; G. J. Bendo; D. G. Bonfield; D. Burgarella; S. Buttiglione; A. Cava; D. L. Clements; A. Cooray; Aliakbar Dariush; G. De Zotti; Simon Dye; Stephen Anthony Eales; David T. Frayer; J. González-Nuevo; D. Herranz; E. Ibar; R. J. Ivison; G. Lagache; L. Leeuw; M. López-Caniego; M. J. Jarvis; Steve Maddox; M. Negrello
We use Herschel PACS and SPIRE observations of the edge-on spiral galaxy UGC4754, taken as part of the H-ATLAS SDP observations, to investigate the dust energy balance in this galaxy. We build detailed SKIRT radiative models based on SDSS and UKIDSS maps and use these models to predict the far-infrared emission. We find that our radiative transfer model underestimates the observed FIR emission by a factor of two to three. Similar discrepancies have been found for other edge-on spiral galaxies based on IRAS, ISO, and SCUBA data. Thanks to the good sampling of the SED at FIR wavelengths, we can rule out an underestimation of the FIR emissivity as the cause for this discrepancy. Instead we support highly obscured star formation that contributes little to the optical extinction as a more probable explanation.
The Astrophysical Journal | 2012
R. Lupu; K. S. Scott; James E. Aguirre; I. Aretxaga; Robbie Richard Auld; Elizabeth J. Barton; A. Beelen; Frank Bertoldi; J. J. Bock; D. G. Bonfield; C. M. Bradford; S. Buttiglione; A. Cava; D. L. Clements; Jeff Cooke; A. Cooray; H. Dannerbauer; A. Dariush; G. De Zotti; Loretta Dunne; S. Dye; Stephen Anthony Eales; David T. Frayer; J. Fritz; J. Glenn; David H. Hughes; E. Ibar; R. J. Ivison; M. J. Jarvis; J. Kamenetzky
We present new observations from Z-Spec, a broadband 185-305 GHz spectrometer, of five submillimeter bright lensed sources selected from the Herschel-Astrophysical Terahertz Large Area Survey science demonstration phase catalog. We construct a redshift-finding algorithm using combinations of the signal to noise of all the lines falling in the Z-Spec bandpass to determine redshifts with high confidence, even in cases where the signal to noise in individual lines is low. We measure the dust continuum in all sources and secure CO redshifts for four out of five (z ~ 1.5-3). In one source, SDP.17, we tentatively identify two independent redshifts and a water line, confirmed at z = 2.308. Our sources have properties characteristic of dusty starburst galaxies, with magnification-corrected star formation rates of 10^(2–3) M_☉ yr^(–1). Lower limits for the dust masses (~a few 10^8 M_☉) and spatial extents (~1 kpc equivalent radius) are derived from the continuum spectral energy distributions, corresponding to dust temperatures between 54 and 69 K. In the local thermodynamic equilibrium (LTE) approximation, we derive relatively low CO excitation temperatures (≲100 K) and optical depths (τ ≲ 1). Performing a non-LTE excitation analysis using RADEX, we find that the CO lines measured by Z-Spec (from J = 4 → 3 to 10 → 9, depending on the galaxy) localize the best solutions to either a high-temperature/low-density region or a low/temperature/high-density region near the LTE solution, with the optical depth varying accordingly. Observations of additional CO lines, CO(1-0) in particular, are needed to constrain the non-LTE models.