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Monthly Notices of the Royal Astronomical Society | 2012

CFHTLenS: the Canada–France–Hawaii Telescope Lensing Survey

Catherine Heymans; Ludovic Van Waerbeke; Lance Miller; Thomas Erben; Hendrik Hildebrandt; Henk Hoekstra; Thomas D. Kitching; Y. Mellier; Patrick Simon; Christopher Bonnett; Jean Coupon; Liping Fu; Joachim Harnois-Déraps; Michael J. Hudson; Martin Kilbinger; K. Kuijken; Barnaby Rowe; Tim Schrabback; Elisabetta Semboloni; Edo van Uitert; Sanaz Vafaei; Malin Velander

We present the Canada–France–Hawaii Telescope Lensing Survey (CFHTLenS) that accurately determines a weak gravitational lensing signal from the full 154 deg^2 of deep multicolour data obtained by the CFHT Legacy Survey. Weak gravitational lensing by large-scale structure is widely recognized as one of the most powerful but technically challenging probes of cosmology. We outline the CFHTLenS analysis pipeline, describing how and why every step of the chain from the raw pixel data to the lensing shear and photometric redshift measurement has been revised and improved compared to previous analyses of a subset of the same data. We present a novel method to identify data which contributes a non-negligible contamination to our sample and quantify the required level of calibration for the survey. Through a series of cosmology-insensitive tests we demonstrate the robustness of the resulting cosmic shear signal, presenting a science-ready shear and photometric redshift catalogue for future exploitation.


Monthly Notices of the Royal Astronomical Society | 2000

The 2dF QSO Redshift Survey — I. The optical luminosity function of quasi-stellar objects

B. J. Boyle; T. Shanks; Scott M. Croom; Roger Smith; Lance Miller; N. S. Loaring; Catherine Heymans

We present a determination of the optical QSO luminosity function and its cosmological evolution with redshift for a sample of over 6000 QSOs identified primarily from the first observations of the 2dF QSO Redshift Survey (2QZ). For QSOs with -26<M_B<-23 and 0.35<z<2.3, we find that pure luminosity evolution (PLE) models provide an acceptable fit to the observed redshift dependence of the luminosity function. The luminosity function is best fit by a two-power-law function of the form. Exponential luminosity evolution models, both as a function of look-back time, and as a general second-order polynomial with redshift, were found to provide acceptable fits to the dataset comprising the 2QZ and the Large Bright Quasar Survey. Exponential evolution with look-back time is prefered for q_0=0.05, while the polynomial evolution model is prefered for q_0=0.5. The shape and evolution of the LF at low redshifts (z<0.5) and/or high luminosities, not currently well sampled by the 2dF QSO survey, may show departures from pure luminosity evolution, but the results presented here show that over a significant range of redshift, PLE is a good description of QSO evolution.


Monthly Notices of the Royal Astronomical Society | 2006

The Shear Testing Programme ¿ I. Weak lensing analysis of simulated ground-based observations

Catherine Heymans; Ludovic Van Waerbeke; David J. Bacon; Joel Bergé; G. M. Bernstein; Emmanuel Bertin; Sarah Bridle; Michael L. Brown; Douglas Clowe; Haakon Dahle; Thomas Erben; Meghan E. Gray; Marco Hetterscheidt; Henk Hoekstra; P. Hudelot; M. Jarvis; Konrad Kuijken; V. E. Margoniner; Richard Massey; Y. Mellier; Reiko Nakajima; Alexandre Refregier; Jason Rhodes; Tim Schrabback; David Michael Wittman

The Shear Testing Programme (STEP) is a collaborative project to improve the accuracy and reliability of all weak lensing measurements in preparation for the next generation of wide-field surveys. In this first STEP paper, we present the results of a blind analysis of simulated ground-based observations of relatively simple galaxy morphologies. The most successful methods are shown to achieve percent level accuracy. From the cosmic shear pipelines that have been used to constrain cosmology, we find weak lensing shear measured to an accuracy that is within the statistical errors of current weak lensing analyses, with shear measurements accurate to better than 7 per cent. The dominant source of measurement error is shown to arise from calibration uncertainties where the measured shear is over or underestimated by a constant multiplicative factor. This is of concern as calibration errors cannot be detected through standard diagnostic tests. The measured calibration errors appear to result from stellar contamination, false object detection, the shear measurement method itself, selection bias and/or the use of biased weights. Additive systematics (false detections of shear) resulting from residual point-spread function anisotropy are, in most cases, reduced to below an equivalent shear of 0.001, an order of magnitude below cosmic shear distortions on the scales probed by current surveys. Our results provide a snapshot view of the accuracy of current ground-based weak lensing methods and a benchmark upon which we can improve. To this end we provide descriptions of each method tested and include details of the eight different implementations of the commonly used Kaiser, Squires & Broadhurst method (KSB+) to aid the improvement of future KSB+ analyses.


Astronomy and Astrophysics | 2008

Very weak lensing in the CFHTLS wide: cosmology from cosmic shear in the linear regime ,

Liping Fu; Elisabetta Semboloni; Henk Hoekstra; Martin Kilbinger; L. van Waerbeke; I. Tereno; Y. Mellier; Catherine Heymans; J. Coupon; K. Benabed; Jonathan Benjamin; E. Bertin; Olivier Doré; Michael J. Hudson; O. Ilbert; R. Maoli; C. Marmo; H. J. McCracken; Brice Ménard

Aims. We present an exploration of weak lensing by large-scale structure in the linear regime, using the third-year (T0003) CFHTLS Wide data release. Our results place tight constraints on the scaling of the amplitude of the matter power spectrum σ8 with the matter density Ωm. Methods. Spanning 57 square degrees to i � = 24.5 over three independent fields, the unprecedented contiguous area of this survey permits high signal-to-noise measurements of two-point shear statistics from 1 arcmin to 4 degrees. Understanding systematic errors in our analysis is vital in interpreting the results. We therefore demonstrate the percent-level accuracy of our method using STEP simulations, an E/B-mode decomposition of the data, and the star-galaxy cross correlation function. We also present a thorough analysis of the galaxy redshift distribution using redshift data from the CFHTLS T0003 Deep fields that probe the same spatial regions as the Wide fields. Results. We find σ8(Ωm/0.25) 0.64 = 0.785 ± 0.043 using the aperture-mass statistic for the full range of angular scales for an assumed flat cosmology, in excellent agreement with WMAP3 constraints. The largest physical scale probed by our analysis is 85 Mpc, assuming a mean redshift of lenses of 0.5 and a ΛCDM cosmology. This allows for the first time to constrain cosmology using only cosmic shear measurements in the linear regime. Using only angular scales θ> 85 arcmin, we find σ8(Ωm/0.25) 0.53 lin = 0.837 ± 0.084, which agree with the results from our full analysis. Combining our results with data from WMAP3, we find Ωm = 0.248 ± 0.019 and σ8 = 0.771 ± 0.029.


Monthly Notices of the Royal Astronomical Society | 2013

CFHTLenS tomographic weak lensing cosmological parameter constraints: Mitigating the impact of intrinsic galaxy alignments

Catherine Heymans; Emma Grocutt; Alan Heavens; Martin Kilbinger; Thomas D. Kitching; Fergus Simpson; Jonathan Benjamin; Thomas Erben; Hendrik Hildebrandt; Henk Hoekstra; Y. Mellier; Lance Miller; Ludovic Van Waerbeke; Michael L. Brown; Jean Coupon; Liping Fu; Joachim Harnois-Déraps; Michael J. Hudson; Konrad Kuijken; Barnaby Rowe; Tim Schrabback; Elisabetta Semboloni; Sanaz Vafaei; Malin Velander

We present a finely-binned tomographic weak lensing analysis of the Canada-FranceHawaii Telescope Lensing Survey, CFHTLenS, mitigating contamination to the signal from the presence of intrinsic galaxy alignments via the simultaneous fit of a cosmological model and an intrinsic alignment model. CFHTLenS spans 154 square degrees in five optical bands, with accurate shear and photometric redshifts for a galaxy sample with a median redshift of zm = 0:70. We estimate the 21 sets of cosmic shear correlation functions associated with six redshift bins, each spanning the angular range of 1:5 < < 35 arcmin. We combine this CFHTLenS data with auxiliary cosmological probes: the cosmic microwave background with data from WMAP7, baryon acoustic oscillations with data from BOSS, and a prior on the Hubble constant from the HST distance ladder. This leads to constraints on the normalisation of the matter power spectrum 8 = 0:799 0:015 and the matter density parameter m = 0:271 0:010 for a flat CDM cosmology. For a flat wCDM cosmology we constrain the dark energy equation of state parameter w = 1:02 0:09. We also provide constraints for curved CDM and wCDM cosmologies. We find the intrinsic alignment contamination to be galaxy-type dependent with a significant intrinsic alignment signal found for early-type galaxies, in contrast to the late-type galaxy sample for which the intrinsic alignment signal is found to be consistent with zero.


Monthly Notices of the Royal Astronomical Society | 2007

The shear testing programme 2 : factors affecting high-precision weak-lensing analyses.

Richard Massey; Catherine Heymans; Joel Bergé; G. M. Bernstein; Sarah Bridle; Douglas Clowe; H. Dahle; Richard S. Ellis; Thomas Erben; Marco Hetterscheidt; F. William High; Christopher M. Hirata; Henk Hoekstra; P. Hudelot; M. Jarvis; David E. Johnston; Konrad Kuijken; V. E. Margoniner; Rachel Mandelbaum; Y. Mellier; Reiko Nakajima; Stephane Paulin-Henriksson; Molly S. Peeples; Chris Roat; Alexandre Refregier; Jason Rhodes; Tim Schrabback; Mischa Schirmer; Uros Seljak; Elisabetta Semboloni

The Shear Testing Programme (STEP) is a collaborative project to improve the accuracy and reliability of weak-lensing measurement, in preparation for the next generation of wide-field surveys. We review 16 current and emerging shear-measurement methods in a common language, and assess their performance by running them (blindly) on simulated images that contain a known shear signal. We determine the common features of algorithms that most successfully recover the input parameters. A desirable goal would be the combination of their best elements into one ultimate shear-measurement method. In this analysis, we achieve previously unattained discriminatory precision via a combination of more extensive simulations and pairs of galaxy images that have been rotated with respect to each other. That removes the otherwise overwhelming noise from their intrinsic ellipticities. Finally, the robustness of our simulation approach is confirmed by testing the relative calibration of methods on real data. Weak-lensing measurements have improved since the first STEP paper. Several methods now consistently achieve better than 2 per cent precision, and are still being developed. However, we can now distinguish all methods from perfect performance. Our main concern continues to be the potential for a multiplicative shear calibration bias: not least because this cannot be internally calibrated with real data. We determine which galaxy populations are responsible for bias and, by adjusting the simulated observing conditions, we also investigate the effects of instrumental and atmospheric parameters. The simulated point spread functions are not allowed to vary spatially, to avoid additional confusion from interpolation errors. We have isolated several previously unrecognized aspects of galaxy shape measurement, in which focused development could provide further progress towards the sub-per cent level of precision desired for future surveys. These areas include the suitable treatment of image pixellization and galaxy morphology evolution. Ignoring the former effect affects the measurement of shear in different directions, leading to an overall underestimation of shear and hence the amplitude of the matter power spectrum. Ignoring the second effect could affect the calibration of shear estimators as a function of galaxy redshift, and the evolution of the lensing signal, which will be vital to measure parameters including the dark energy equation of state.


Monthly Notices of the Royal Astronomical Society | 2013

CFHTLenS: the Canada-France-Hawaii Telescope Lensing Survey - imaging data and catalogue products

Thomas Erben; Hendrik Hildebrandt; L. Miller; L. van Waerbeke; Catherine Heymans; Henk Hoekstra; T. D. Kitching; Y. Mellier; Jonathan Benjamin; Chris Blake; Christopher Bonnett; O. Cordes; Jean Coupon; Liping Fu; R. Gavazzi; Bryan R. Gillis; E. Grocutt; Stephen Gwyn; K. Holhjem; M. J. Hudson; M. Kilbinger; K. Kuijken; Martha Milkeraitis; Barnaby Rowe; Tim Schrabback; Elisabetta Semboloni; Patrick Simon; M. Smit; O. Toader; Sanaz Vafaei

We present data products from the Canada–France–Hawaii Telescope Lensing Survey (CFHTLenS). CFHTLenS is based on the Wide component of the Canada–France–Hawaii Telescope Legacy Survey (CFHTLS). It encompasses 154 deg^2 of deep, optical, high-quality, sub-arcsecond imaging data in the five optical filters u*g′r′i′z′. The scientific aims of the CFHTLenS team are weak gravitational lensing studies supported by photometric redshift estimates for the galaxies. This paper presents our data processing of the complete CFHTLenS data set. We were able to obtain a data set with very good image quality and high-quality astrometric and photometric calibration. Our external astrometric accuracy is between 60 and 70 mas with respect to Sloan Digital Sky Survey (SDSS) data, and the internal alignment in all filters is around 30 mas. Our average photometric calibration shows a dispersion of the order of 0.01–0.03 mag for g′r′i′z′ and about 0.04 mag for u* with respect to SDSS sources down to i_(SDSS) ≤ 21. We demonstrate in accompanying papers that our data meet necessary requirements to fully exploit the survey for weak gravitational lensing analyses in connection with photometric redshift studies. In the spirit of the CFHTLS, all our data products are released to the astronomical community via the Canadian Astronomy Data Centre at http://www.cadc-ccda.hia-iha.nrc-cnrc.gc.ca/community/CFHTLens/query.html. We give a description and how-to manuals of the public products which include image pixel data, source catalogues with photometric redshift estimates and all relevant quantities to perform weak lensing studies.


Monthly Notices of the Royal Astronomical Society | 2013

CFHTLenS: Combined probe cosmological model comparison using 2D weak gravitational lensing

Martin Kilbinger; Liping Fu; Catherine Heymans; Fergus Simpson; Jonathan Benjamin; Thomas Erben; Joachim Harnois-Déraps; Henk Hoekstra; Hendrik Hildebrandt; Thomas D. Kitching; Y. Mellier; Lance Miller; Ludovic Van Waerbeke; K. Benabed; Christopher Bonnett; Jean Coupon; Michael J. Hudson; Konrad Kuijken; Barnaby Rowe; Tim Schrabback; Elisabetta Semboloni; Sanaz Vafaei; Malin Velander

We present cosmological constraints from 2D weak gravitational lensing by the large-scale structure in the Canada–France–Hawaii Telescope Lensing Survey (CFHTLenS) which spans 154 deg^2 in five optical bands. Using accurate photometric redshifts and measured shapes for 4.2 million galaxies between redshifts of 0.2 and 1.3, we compute the 2D cosmic shear correlation function over angular scales ranging between 0.8 and 350 arcmin. Using non-linear models of the dark-matter power spectrum, we constrain cosmological parameters by exploring the parameter space with Population Monte Carlo sampling. The best constraints from lensing alone are obtained for the small-scale density-fluctuations amplitude σ_8 scaled with the total matter density Ωm. For a flat Λcold dark matter (ΛCDM) model we obtain σ_8(Ω_m/0.27)0.6 = 0.79 ± 0.03. We combine the CFHTLenS data with 7-year Wilkinson Microwave Anisotropy Probe (WMAP7), baryonic acoustic oscillations (BAO): SDSS-III (BOSS) and a Hubble Space Telescope distance-ladder prior on the Hubble constant to get joint constraints. For a flat ΛCDM model, we find Ω_m = 0.283 ± 0.010 and σ_8 = 0.813 ± 0.014. In the case of a curved wCDM universe, we obtain Ω_m = 0.27 ± 0.03, σ_8 = 0.83 ± 0.04, w0 = −1.10 ± 0.15 and Ω_K = 0.006^(+0.006)_(− 0.004). We calculate the Bayesian evidence to compare flat and curved ΛCDM and dark-energy CDM models. From the combination of all four probes, we find models with curvature to be at moderately disfavoured with respect to the flat case. A simple dark-energy model is indistinguishable from ΛCDM. Our results therefore do not necessitate any deviations from the standard cosmological model.


Monthly Notices of the Royal Astronomical Society | 2013

Bayesian galaxy shape measurement for weak lensing surveys - III. Application to the Canada-France-Hawaii Telescope Lensing Survey

L. Miller; Catherine Heymans; T. D. Kitching; L. van Waerbeke; Thomas Erben; Hendrik Hildebrandt; Henk Hoekstra; Y. Mellier; Barnaby Rowe; Jean Coupon; J. P. Dietrich; Liping Fu; Joachim Harnois-Déraps; M. J. Hudson; M. Kilbinger; K. Kuijken; Tim Schrabback; Elisabetta Semboloni; Sanaz Vafaei; Malin Velander

A likelihood-based method for measuring weak gravitational lensing shear in deep galaxy surveys is described and applied to the Canada–France–Hawaii Telescope (CFHT) Lensing Survey (CFHTLenS). CFHTLenS comprises 154 deg^2 of multi-colour optical data from the CFHT Legacy Survey, with lensing measurements being made in the i′ band to a depth i′_(AB) < 24.7, for galaxies with signal-to-noise ratio ν_(SN) ≳ 10. The method is based on the lensfit algorithm described in earlier papers, but here we describe a full analysis pipeline that takes into account the properties of real surveys. The method creates pixel-based models of the varying point spread function (PSF) in individual image exposures. It fits PSF-convolved two-component (disc plus bulge) models to measure the ellipticity of each galaxy, with Bayesian marginalization over model nuisance parameters of galaxy position, size, brightness and bulge fraction. The method allows optimal joint measurement of multiple, dithered image exposures, taking into account imaging distortion and the alignment of the multiple measurements. We discuss the effects of noise bias on the likelihood distribution of galaxy ellipticity. Two sets of image simulations that mirror the observed properties of CFHTLenS have been created to establish the methods accuracy and to derive an empirical correction for the effects of noise bias.


The Astrophysical Journal | 2010

A weak lensing study of X-ray groups in the cosmos survey: form and evolution of the mass-luminosity relation

Alexie Leauthaud; Alexis Finoguenov; Jean-Paul Kneib; James E. Taylor; Richard Massey; Jason Rhodes; O. Ilbert; Kevin Bundy; Jeremy L. Tinker; Matthew R. George; P. Capak; Anton M. Koekemoer; David E. Johnston; Yu-Ying Zhang; N. Cappelluti; Richard S. Ellis; M. Elvis; S. Giodini; Catherine Heymans; Oliver Le Fevre; S. J. Lilly; H. J. McCracken; Y. Mellier; Alexandre Refregier; M. Salvato; N. Z. Scoville; George F. Smoot; M. Tanaka; Ludovic Van Waerbeke; M. Wolk

Measurements of X-ray scaling laws are critical for improving cosmological constraints derived with the halo mass function and for understanding the physical processes that govern the heating and cooling of the intracluster medium. In this paper, we use a sample of 206 X-ray-selected galaxy groups to investigate the scaling relation between X-ray luminosity (L_X) and halo mass (M_(200)) where M_(200) is derived via stacked weak gravitational lensing. This work draws upon a broad array of multi-wavelength COSMOS observations including 1.64 degrees^2 of contiguous imaging with the Advanced Camera for Surveys to a limiting magnitude of I_(F814W) = 26.5 and deep XMM-Newton/Chandra imaging to a limiting flux of 1.0 × 10^(–15) erg cm6(–2) s^(–1) in the 0.5-2 keV band. The combined depth of these two data sets allows us to probe the lensing signals of X-ray-detected structures at both higher redshifts and lower masses than previously explored. Weak lensing profiles and halo masses are derived for nine sub-samples, narrowly binned in luminosity and redshift. The COSMOS data alone are well fit by a power law, M_(200) (L_X)^α, with a slope of α = 0.66 ± 0.14. These results significantly extend the dynamic range for which the halo masses of X-ray-selected structures have been measured with weak gravitational lensing. As a result, tight constraints are obtained for the slope of the M-L_X relation. The combination of our group data with previously published cluster data demonstrates that the M-L_X relation is well described by a single power law, α = 0.64 ± 0.03, over two decades in mass, M_(200) ~ 10^(13.5)-10^(15.5) h^(–1)_72 M_☉. These results are inconsistent at the 3.7σ level with the self-similar prediction of α = 0.75. We examine the redshift dependence of the M-L_X relation and find little evidence for evolution beyond the rate predicted by self-similarity from z ~ 0.25 to z ~ 0.

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Marco Barden

University of Innsbruck

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Daniel H. McIntosh

University of Missouri–Kansas City

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Shardha Jogee

University of Texas at Austin

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