Contamination of early-type galaxy alignments to galaxy lensing-CMB lensing cross-correlation

Monthly Notices of the Royal Astronomical Society 453:1 (2015) 682-689

Authors:

NE Chisari, J Dunkley, L Miller, R Allison

Abstract:

© 2015 The Authors. Galaxy shapes are subject to distortions due to the tidal field of the Universe. The crosscorrelation of galaxy lensing with the lensing of the cosmic microwave background (CMB) cannot easily be separated from the cross-correlation of galaxy intrinsic shapes with CMB lensing. Previous work suggested that the intrinsic alignment contamination can be 15 per cent of this cross-spectrum for the CFHT Stripe 82 (CS82) and Atacama Cosmology Telescope surveys. Here we re-examine these estimates using up-to-date observational constraints of intrinsic alignments at a redshift more similar to that of CS82 galaxies. We find an ≈ 10 per cent contamination of the cross-spectrum from red galaxies, with ≈ 3 per cent uncertainty due to uncertainties in the redshift distribution of source galaxies and the modelling of the spectral energy distribution. Blue galaxies are consistent with being unaligned, but could contaminate the cross-spectrum by an additional 9.5 per cent within current 95 per cent confidence levels. While our fiducial estimate of alignment contamination is similar to previous work, our work suggests that the relevance of alignments for CMB lensing-galaxy lensing cross-correlation remains largely unconstrained. Little information is currently available about alignments at z > 1.2. We consider the upper limiting case where all z > 1.2 galaxies are aligned with the same strength as low-redshift luminous red galaxies, finding as much as ≈ 60 per cent contamination.

The SAMI Pilot Survey: the fundamental and mass planes in three low-redshift clusters

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 451:3 (2015) 2723-2734

Authors:

Nicholas Scott, LMR Fogarty, Matt S Owers, Scott M Croom, Matthew Colless, Roger L Davies, S Brough, Michael B Pracy, Joss Bland-Hawthorn, D Heath Jones, JT Allen, Julia J Bryant, Luca Cortese, Michael Goodwin, Andrew W Green, Iraklis S Konstantopoulos, JS Lawrence, Samuel Richards, Rob Sharp

CFHTLenS: weak lensing calibrated scaling relations for low-mass clusters of galaxies

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 451:2 (2015) 1460-1481

Authors:

K Kettula, S Giodini, E van Uitert, H Hoekstra, A Finoguenov, M Lerchster, T Erben, C Heymans, H Hildebrandt, TD Kitching, A Mahdavi, Y Mellier, L Miller, M Mirkazemi, L Van Waerbeke, J Coupon, E Egami, L Fu, MJ Hudson, JP Kneib, K Kuijken, HJ McCracken, MJ Pereira, B Rowe, T Schrabback, M Tanaka, M Velander

The evolving relation between star-formation rate and stellar mass in the VIDEO Survey since z=3

Monthly Notices of the Royal Astronomical Society Oxford University Press 453:3 (2015) 2540-2557

Authors:

Russell Johnston, Mattia Vaccari, Matthew Jarvis, Matthew Smith, Elodie Giovannoli, Boris Häußler, Matthew Prescott

Abstract:

We investigate the star-formation rate (SFR) and stellar mass ($M_*$) relation of a star-forming (SF) galaxy sample in the XMM-LSS field to $z\sim 3.0$ using the near-infrared data from the VISTA Deep Extragalactic Observations (VIDEO) survey. Combining VIDEO with broad-band photometry, we use the SED fitting algorithm CIGALE to derive SFRs and $M_*$ and have adapted it to account for the full photometric redshift PDF uncertainty. Applying a SF selection using the D4000 index, we find evidence for strong evolution in the normalisation of the SFR-$M_*$ relation out to $z\sim 3$ and a roughly constant slope of (SFR $\propto M_*^{\alpha}$) $\alpha=0.69\pm0.02$ to $z\sim 1.7$. We find this increases close to unity toward $z\sim2.65$. Alternatively, if we apply a colour selection, we find a distinct turnover in the SFR-$M_*$ relation between $0.7\lesssim z\lesssim2.0$ at the high mass end, and suggest that this is due to an increased contamination from passive galaxies. We find evolution of the specific SFR $\propto(1+z)^{2.60}$ at $\log(M_*)\sim$10.5, out to $z\lesssim2.4$ with an observed flattening beyond $z\sim$ 2 with increased stellar mass. Comparing to a range of simulations we find the analytical scaling relation approaches, that invoke an equilibrium model, a good fit to our data, suggesting that a continual smooth accretion regulated by continual outflows may be a key driver in the overall growth of SFGs.

The faint radio source population at 15.7 GHz - II. Multi-wavelength properties

Monthly Notices Of The Royal Astronomical Society Oxford University Press 453:4 (2015) 4244-4263

Authors:

Imogen Whittam, Julia Riley, Dave Green, Matthew Jarvis, Mattia Vaccari

Abstract:

A complete, flux density limited sample of 96 faint ($> 0.5$ mJy) radio sources is selected from the 10C survey at 15.7 GHz in the Lockman Hole. We have matched this sample to a range of multi-wavelength catalogues, including SERVS, SWIRE, UKIDSS and optical data; multi-wavelength counterparts are found for 80 of the 96 sources and spectroscopic redshifts are available for 24 sources. Photometric reshifts are estimated for the sources with multi-wavelength data available; the median redshift of the sample is 0.91 with an interquartile range of 0.84. Radio-to-optical ratios show that at least 94 per cent of the sample are radio loud, indicating that the 10C sample is dominated by radio galaxies. This is in contrast to samples selected at lower frequencies, where radio-quiet AGN and starforming galaxies are present in significant numbers at these flux density levels. All six radio-quiet sources have rising radio spectra, suggesting that they are dominated by AGN emission. These results confirm the conclusions of Paper I that the faint, flat-spectrum sources which are found to dominate the 10C sample below $\sim 1$ mJy are the cores of radio galaxies. The properties of the 10C sample are compared to the SKADS Simulated Skies; a population of low-redshift starforming galaxies predicted by the simulation is not found in the observed sample.