Rigging dark halos: why is hierarchical galaxy formation consistent with the inside-out build-up of thin discs?

(2011)

Authors:

C Pichon, D Pogosyan, T Kimm, A Slyz, J Devriendt, Y Dubois

Galaxy and Mass Assembly (GAMA): survey diagnostics and core data release

\mnras 413 (2011) 971-995-971-995

Authors:

SP Driver, DT Hill, LS Kelvin, ASG Robotham, J Liske, P Norberg, IK Baldry, SP Bamford, AM Hopkins, J Loveday, JA Peacock, E Andrae, J Bland-Hawthorn, S Brough, MJI Brown, E Cameron, JHY Ching, M Colless, CJ Conselice, SM Croom, NJG Cross, R de Propris, S Dye, MJ Drinkwater, S Ellis, AW Graham, MW Grootes, M Gunawardhana, DH Jones, E van Kampen, C Maraston, RC Nichol, HR Parkinson, S Phillipps, K Pimbblet, CC Popescu, M Prescott, IG Roseboom, EM Sadler, AE Sansom, RG Sharp, DJB Smith, E Taylor, D Thomas, RJ Tuffs, D Wijesinghe, L Dunne, CS Frenk, MJ Jarvis, BF Madore, MJ Meyer, M Seibert, L Staveley-Smith, WJ Sutherland, SJ Warren

The evolution of radio sources in the UKIDSS-DXS-XMM-LSS field

\mnras 413 (2011) 1054-1060-1054-1060

Authors:

K McAlpine, MJ Jarvis

Galactic star formation in parsec-scale resolution simulations

Proceedings of the IAU (2011)

Authors:

LC Powell, F Bournaud, D Chapon, J Devriendt, A Slyz, R Teyssier

Abstract:

The interstellar medium (ISM) in galaxies is multiphase and cloudy, with stars forming in the very dense, cold gas found in Giant Molecular Clouds (GMCs). Simulating the evolution of an entire galaxy, however, is a computational problem which covers many orders of magnitude, so many simulations cannot reach densities high enough or temperatures low enough to resolve this multiphase nature. Therefore, the formation of GMCs is not captured and the resulting gas distribution is smooth, contrary to observations. We investigate how star formation (SF) proceeds in simulated galaxies when we obtain parsec-scale resolution and more successfully capture the multiphase ISM. Both major mergers and the accretion of cold gas via filaments are dominant contributors to a galaxy's total stellar budget and we examine SF at high resolution in both of these contexts.

Contemporaneous Chandra HETG and Suzaku X-ray observations of NGC 4051

Monthly Notices of the Royal Astronomical Society (2011)

Authors:

AP Lobban, JN Reeves, L Miller, TJ Turner, V Braito, SB Kraemer, DM Crenshaw

Abstract:

We present the results of a deep 300ks Chandra High Energy Transmission Grating (HETG) observation of the highly variable narrow-line Seyfert Type 1 galaxy NGC 4051. The HETG spectrum reveals 28 significant soft X-ray ionized lines in either emission or absorption; primarily originating from H-like and He-like K-shell transitions of O, Ne, Mg and Si (including higher order lines and strong forbidden emission lines from Ovii and Neix) plus high-ionization L-shell transitions from Fexvii to Fexxii and lower ionization inner-shell lines (e.g. Ovi). Modelling the data with xstar requires four distinct ionization zones for the gas, all outflowing with velocities < 1000kms -1 . A selection of the strongest emission/absorption lines appear to be resolved with full width at half-maximum (FWHM) of ∼600kms -1 . We also present the results from a quasi-simultaneous 350ks Suzaku observation of NGC 4051 where the X-ray Imaging Spectrometer (XIS) spectrum reveals strong evidence for blueshifted absorption lines at ∼6.8 and ∼7.1keV, consistent with previous findings. Modelling with xstar suggests that this is the signature of a highly ionized, high-velocity outflow (logξ= 4.1 +0.2 -0.1 ; v out ∼-0.02c) which potentially may have a significant effect on the host galaxy environment via feedback. Finally, we also simultaneously model the broad-band 2008 XIS+HXD (Hard X-ray Detector) Suzaku data with archival Suzaku data from 2005 when the source was observed to have entered an extended period of low flux in an attempt to analyse the cause of the long-term spectral variability. We find that we can account for this by allowing for large variations in the normalization of the intrinsic power-law component which may be interpreted as being due to significant changes in the covering fraction of a Compton-thick partial-coverer obscuring the central continuum emission. © 2011 The Authors. Monthly Notices of the Royal Astronomical Society © 2011 RAS.