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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

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
More details from the publisher

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.
More details from the publisher

Erratum: On the efficiency of production of the Fe Kα emission line in neutral matter

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 415:4 (2011) 3966-3967

Authors:

T Yaqoob, KD Murphy, L Miller, TJ Turner
More details from the publisher

X-ray reverberation in NLS1

ArXiv 1106.3648 (2011)

Authors:

L Miller, TJ Turner

Abstract:

Reverberation from scattering material around the black hole in active galactic nuclei is expected to produce a characteristic signature in a Fourier analysis of the time delays between directly-viewed continuum emission and the scattered light. Narrow-line Seyfert 1 galaxies (NLS1) are highly variable at X-ray energies, and are ideal candidates for the detection of X-ray reverberation. We show new analysis of a small sample of NLS1 that clearly shows the expected time-delay signature, providing strong evidence for the existence of a high covering fraction of scattering and absorbing material a few tens to hundreds of gravitational radii from the black hole. We also show that an alternative interpretation of time delays in the NLS1 1H0707-495, as arising about one gravitational radius from the black hole, is strongly disfavoured in an analysis of the energy-dependence of the time delays.
Details from ArXiV

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