The environment and characteristics of low-redshift galaxies detected by the Herschel-ATLAS

\mnras 418 (2011) 64-73-64-73

Authors:

A Dariush, L Cortese, S Eales, E Pascale, MWL Smith, L Dunne, S Dye, D Scott, R Auld, M Baes, J Bland-Hawthorn, S Buttiglione, A Cava, DL Clements, A Cooray, G Dezotti, S Driver, J Fritz, HL Gomez, A Hopkins, R Hopwood, RJ Ivison, MJ Jarvis, DH Jones, L Kelvin, HG Khosroshahi, J Liske, J Loveday, S Maddox, BF Madore, MJ Micha lowski, P Norberg, S Phillipps, M Pohlen, CC Popescu, M Prescott, E Rigby, A Robotham, G Rodighiero, M Seibert, DJB Smith, P Temi, RJ Tuffs, PP van der Werf

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.

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.

SWIFT observations of the Arp 147 ring galaxy system

Monthly Notices of the Royal Astronomical Society 417:2 (2011) 835-844

Authors:

L Fogarty, N Thatte, M Tecza, F Clarke, T Goodsall, R Houghton, G Salter, RL Davies, SA Kassin

Abstract:

We present observations of Arp 147, a galaxy system comprising a collisionally created ring galaxy and an early-type galaxy, using the Oxford SWIFT integral field spectrograph (IFS) at the 200-inch Hale telescope. We derive spatially resolved kinematics from the IFS data and use these to study the interaction between the two galaxies. We find the edge-to-edge expansion velocity of the ring is 225 ± 8kms-1, implying an upper limit on the time-scale for the collision of 50Myr. We also calculate that the angle of impact for the collision is between, where 0° would imply a perpendicular collision. The ring galaxy is strongly star forming with the star formation likely to have been triggered by the collision between the two galaxies. We also measure some key physical parameters in an integrated and spatially resolved manner for the ring galaxy. Using the observed B-I colours and the Hα equivalent widths, we conclude that two stellar components (a young and an old population) are required everywhere in the ring to simultaneously match both observed quantities. We are able to constrain the age range, light and mass fractions of the young star formation activity in the ring, finding a modest age range, a light fraction of less than a third, and a negligible (<1 per cent) mass fraction. We postulate that the redder colours observed in the south-east corner of the ring galaxy could correspond to the nuclear bulge of the original disc galaxy from which the ring was created, consistent with the stellar mass in the south-east quadrant being 30-50 per cent of the total. The ring appears to have been a typical disc galaxy prior to the encounter. The ring shows electron densities consistent with typical values for star-forming Hii regions. The eastern half of the ring exhibits a metallicity a factor of ~2 higher than the western half. The ionization parameter, measured across the ring, roughly follows the previously observed trend with metallicity. © 2011 The Authors Monthly Notices of the Royal Astronomical Society © 2011 RAS.

The ATLAS3D project - X. On the origin of the molecular and ionized gas in early-type galaxies

Monthly Notices of the Royal Astronomical Society 417:2 (2011) 882-899

Authors:

TA Davis, K Alatalo, M Sarzi, M Bureau, LM Young, L Blitz, P Serra, AF Crocker, D Krajnović, RM McDermid, M Bois, F Bournaud, M Cappellari, RL Davies, PA Duc, PT de Zeeuw, E Emsellem, S Khochfar, H Kuntschner, PY Lablanche, R Morganti, T Naab, T Oosterloo, N Scott, AM Weijmans

Abstract:

We make use of interferometric CO and Hi observations, and optical integral-field spectroscopy from the ATLAS3D survey, to probe the origin of the molecular and ionized interstellar medium (ISM) in local early-type galaxies. We find that 36 ± 5 per cent of our sample of fast-rotating early-type galaxies have their ionized gas kinematically misaligned with respect to the stars, setting a strong lower limit on the importance of externally acquired gas (e.g. from mergers and cold accretion). Slow rotators have a flat distribution of misalignments, indicating that the dominant source of gas is external. The molecular, ionized and atomic gas in all the detected galaxies are always kinematically aligned, even when they are misaligned from the stars, suggesting that all these three phases of the ISM share a common origin. In addition, we find that the origin of the cold and warm gas in fast-rotating early-type galaxies is strongly affected by environment, despite the molecular gas detection rate and mass fractions being fairly independent of group/cluster membership. Galaxies in dense groups and the Virgo cluster nearly always have their molecular gas kinematically aligned with the stellar kinematics, consistent with a purely internal origin (presumably stellar mass loss). In the field, however, kinematic misalignments between the stellar and gaseous components indicate that at least 42 ± 5 per cent of local fast-rotating early-type galaxies have their gas supplied from external sources. When one also considers evidence of accretion present in the galaxies' atomic gas distributions, ≳46 per cent of fast-rotating field ETGs are likely to have acquired a detectable amount of ISM from accretion and mergers. We discuss several scenarios which could explain the environmental dichotomy, including preprocessing in galaxy groups/cluster outskirts and the morphological transformation of spiral galaxies, but we find it difficult to simultaneously explain the kinematic misalignment difference and the constant detection rate. Furthermore, our results suggest that galaxy mass may be an important independent factor associated with the origin of the gas, with the most massive fast-rotating galaxies in our sample (MK≲-24mag; stellar mass of ≈8 × 1010 M⊙) always having kinematically aligned gas. This mass dependence appears to be independent of environment, suggesting it is caused by a separate physical mechanism. © 2011 The Authors Monthly Notices of the Royal Astronomical Society © 2011 RAS.