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Black Hole

Lensing of space time around a black hole. At Oxford we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Lance Miller

Professor of Astrophysics

Research theme

  • Astronomy and astrophysics

Sub department

  • Astrophysics

Research groups

  • Beecroft Institute for Particle Astrophysics and Cosmology
  • Cosmology
  • Euclid
Lance.Miller@physics.ox.ac.uk
  • About
  • Publications

CFHTLenS: Improving the quality of photometric redshifts with precision photometry

Monthly Notices of the Royal Astronomical Society 421:3 (2012) 2355-2367

Authors:

H Hildebrandt, T Erben, K Kuijken, L van Waerbeke, C Heymans, J Coupon, J Benjamin, C Bonnett, L Fu, H Hoekstra, TD Kitching, Y Mellier, L Miller, M Velander, MJ Hudson, BTP Rowe, T Schrabback, E Semboloni, N Benítez

Abstract:

Here we present the results of various approaches to measure accurate colours and photometric redshifts (photo-z) from wide-field imaging data. We use data from the Canada-France-Hawaii Telescope Legacy Survey which have been re-processed by the Canada-France-Hawaii Telescope Lensing Survey (CFHTLenS) team in order to carry out a number of weak gravitational lensing studies. An emphasis is put on the correction of systematic effects in the photo-z arising from the different point spread functions (PSFs) in the five optical bands. Different ways of correcting these effects are discussed and the resulting photo-z accuracies are quantified by comparing the photo-z to large spectroscopic redshift (spec-z) data sets. Careful homogenization of the PSF between bands leads to increased overall accuracy of photo-z. The gain is particularly pronounced at fainter magnitudes where galaxies are smaller and flux measurements are affected more by PSF effects. We discuss ways of defining more secure subsamples of galaxies as well as a shape- and colour-based star-galaxy separation method, and we present redshift distributions for different magnitude limits. We also study possible re-calibrations of the photometric zero-points (ZPs) with the help of galaxies with known spec-z. We find that if PSF effects are properly taken into account, a re-calibration of the ZPs becomes much less important suggesting that previous such re-calibrations described in the literature could in fact be mostly corrections for PSF effects rather than corrections for real inaccuracies in the ZPs. The implications of this finding for future surveys like the Kilo Degree Survey (KiDS), Dark Energy Survey (DES), Large Synoptic Survey Telescope or Euclid are mixed. On the one hand, ZP re-calibrations with spec-z values might not be as accurate as previously thought. On the other hand, careful PSF homogenization might provide a way out and yield accurate, homogeneous photometry without the need for full spectroscopic coverage. This is the first paper in a series describing the technical aspects of CFHTLenS. © 2012 The Authors Monthly Notices of the Royal Astronomical Society © 2012 RAS.
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The impact of high spatial frequency atmospheric distortions on weak-lensing measurements

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 421:1 (2012) 381-389

Authors:

Catherine Heymans, Barnaby Rowe, Henk Hoekstra, Lance Miller, Thomas Erben, Thomas Kitching, Ludovic Van Waerbeke
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The impact of high spatial frequency atmospheric distortions on weak lensing measurements

ArXiv 1110.4913 (2011)

Authors:

Catherine Heymans, Barnaby Rowe, Henk Hoekstra, Lance Miller, Thomas Erben, Thomas Kitching, Ludovic Van Waerbeke

Abstract:

High precision cosmology with weak gravitational lensing requires a precise measure of the Point Spread Function across the imaging data where the accuracy to which high spatial frequency variation can be modelled is limited by the stellar number density across the field. We analyse dense stellar fields imaged at the Canada-France-Hawaii Telescope to quantify the degree of high spatial frequency variation in ground-based imaging Point Spread Functions and compare our results to models of atmospheric turbulence. The data shows an anisotropic turbulence pattern with an orientation independent of the wind direction and wind speed. We find the amplitude of the high spatial frequencies to decrease with increasing exposure time as $t^{-1/2}$, and find a negligibly small atmospheric contribution to the Point Spread Function ellipticity variation for exposure times $t>180$ seconds. For future surveys analysing shorter exposure data, this anisotropic turbulence will need to be taken into account as the amplitude of the correlated atmospheric distortions becomes comparable to a cosmological lensing signal on scales less than $\sim 10$ arcminutes. This effect could be mitigated, however, by correlating galaxy shear measured on exposures imaged with a time separation greater than 50 seconds, for which we find the spatial turbulence patterns to be uncorrelated.
Details from ArXiV
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Euclid Definition Study Report

ArXiv 1110.3193 (2011)

Authors:

R Laureijs, J Amiaux, S Arduini, J-L Auguères, J Brinchmann, R Cole, M Cropper, C Dabin, L Duvet, A Ealet, B Garilli, P Gondoin, L Guzzo, J Hoar, H Hoekstra, R Holmes, T Kitching, T Maciaszek, Y Mellier, F Pasian, W Percival, J Rhodes, G Saavedra Criado, M Sauvage, R Scaramella, L Valenziano, S Warren, R Bender, F Castander, A Cimatti, O Le Fèvre, H Kurki-Suonio, M Levi, P Lilje, G Meylan, R Nichol, K Pedersen, V Popa, R Rebolo Lopez, H-W Rix, H Rottgering, W Zeilinger, F Grupp, P Hudelot, R Massey, M Meneghetti, L Miller, S Paltani, S Paulin-Henriksson, S Pires, C Saxton, T Schrabback, G Seidel, J Walsh, N Aghanim, L Amendola, J Bartlett, C Baccigalupi, J-P Beaulieu, K Benabed, J-G Cuby, D Elbaz, P Fosalba, G Gavazzi, A Helmi, I Hook, M Irwin, J-P Kneib, M Kunz, F Mannucci, L Moscardini, C Tao, R Teyssier, J Weller, G Zamorani, MR Zapatero Osorio, O Boulade, JJ Foumond, A Di Giorgio, P Guttridge, A James, M Kemp, J Martignac, A Spencer, D Walton, T Blümchen, C Bonoli, F Bortoletto, C Cerna, L Corcione, C Fabron, K Jahnke, S Ligori, F Madrid, L Martin, G Morgante, T Pamplona, E Prieto, M Riva, R Toledo, M Trifoglio, F Zerbi, F Abdalla, M Douspis, C Grenet, S Borgani, R Bouwens, F Courbin, J-M Delouis, P Dubath, A Fontana, M Frailis, A Grazian, J Koppenhöfer, O Mansutti, M Melchior, M Mignoli, J Mohr, C Neissner, K Noddle, M Poncet, M Scodeggio, S Serrano, N Shane, J-L Starck, C Surace, A Taylor, G Verdoes-Kleijn, C Vuerli, OR Williams, A Zacchei, B Altieri, I Escudero Sanz, R Kohley, T Oosterbroek, P Astier, D Bacon, S Bardelli, C Baugh, F Bellagamba, C Benoist, D Bianchi, A Biviano, E Branchini, C Carbone, V Cardone, D Clements, S Colombi, C Conselice, G Cresci, N Deacon, J Dunlop, C Fedeli, F Fontanot, P Franzetti, C Giocoli, J Garcia-Bellido, J Gow, A Heavens, P Hewett, C Heymans, A Holland, Z Huang, O Ilbert, B Joachimi, E Jennins, E Kerins, A Kiessling, D Kirk, R Kotak, O Krause, O Lahav, F van Leeuwen, J Lesgourgues, M Lombardi, M Magliocchetti, K Maguire, E Majerotto, R Maoli, F Marulli, S Maurogordato, H McCracken, R McLure, A Melchiorri, A Merson, M Moresco, M Nonino, P Norberg, J Peacock, R Pello, M Penny, V Pettorino, C Di Porto, L Pozzetti, C Quercellini, M Radovich, A Rassat, N Roche, S Ronayette, E Rossetti, B Sartoris, P Schneider, E Semboloni, S Serjeant, F Simpson, C Skordis, G Smadja, S Smartt, P Spano, S Spiro, M Sullivan, A Tilquin, R Trotta, L Verde, Y Wang, G Williger, G Zhao, J Zoubian, E Zucca

Abstract:

Euclid is a space-based survey mission from the European Space Agency designed to understand the origin of the Universe's accelerating expansion. It will use cosmological probes to investigate the nature of dark energy, dark matter and gravity by tracking their observational signatures on the geometry of the universe and on the cosmic history of structure formation. The mission is optimised for two independent primary cosmological probes: Weak gravitational Lensing (WL) and Baryonic Acoustic Oscillations (BAO). The Euclid payload consists of a 1.2 m Korsch telescope designed to provide a large field of view. It carries two instruments with a common field-of-view of ~0.54 deg2: the visual imager (VIS) and the near infrared instrument (NISP) which contains a slitless spectrometer and a three bands photometer. The Euclid wide survey will cover 15,000 deg2 of the extragalactic sky and is complemented by two 20 deg2 deep fields. For WL, Euclid measures the shapes of 30-40 resolved galaxies per arcmin2 in one broad visible R+I+Z band (550-920 nm). The photometric redshifts for these galaxies reach a precision of dz/(1+z) < 0.05. They are derived from three additional Euclid NIR bands (Y, J, H in the range 0.92-2.0 micron), complemented by ground based photometry in visible bands derived from public data or through engaged collaborations. The BAO are determined from a spectroscopic survey with a redshift accuracy dz/(1+z) =0.001. The slitless spectrometer, with spectral resolution ~250, predominantly detects Ha emission line galaxies. Euclid is a Medium Class mission of the ESA Cosmic Vision 2015-2025 programme, with a foreseen launch date in 2019. This report (also known as the Euclid Red Book) describes the outcome of the Phase A study.
Details from ArXiV
Details from ORA

The environment and redshift dependence of accretion on to dark matter haloes and subhaloes

Monthly Notices of the Royal Astronomical Society 417:1 (2011) 666-680

Authors:

H Tillson, L Miller, J Devriendt

Abstract:

A dark-matter-only Horizon Project simulation is used to investigate the environment and redshift dependences of accretion on to both haloes and subhaloes. These objects grow in the simulation via mergers and via accretion of diffuse non-halo material, and we measure the combined signal from these two modes of accretion. It is found that the halo accretion rate varies less strongly with redshift than predicted by the Extended Press-Schechter formalism and is dominated by minor merger and diffuse accretion events at z= 0, for all haloes. These latter growth mechanisms may be able to drive the radio-mode feedback hypothesised for recent galaxy-formation models, and have both the correct accretion rate and the form of cosmological evolution. The low-redshift subhalo accretors in the simulation form a mass-selected subsample safely above the mass resolution limit that reside in the outer regions of their host, with ∼70 per cent beyond their host's virial radius, where they are probably not being significantly stripped of mass. These subhaloes accrete, on average, at higher rates than haloes at low redshift and we argue that this is due to their enhanced clustering at small scales. At cluster scales, the mass accretion rate on to haloes and subhaloes at low redshift is found to be only weakly dependent on environment, and we confirm that at z∼ 2 haloes accrete independently of their environment at all scales, as reported by other authors. By comparing our results with an observational study of black hole growth, we support previous suggestions that at z > 1, dark matter haloes and their associated central black holes grew coevally, but show that by the present-day, dark matter haloes could be accreting at fractional rates that are up to a factor of 3 - 4 higher than their associated black holes. © 2011 The Authors Monthly Notices of the Royal Astronomical Society © 2011 RAS.
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