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

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Kilbinger, Martin, Fu, Liping, Heymans, Catherine, Simpson, Fergus, Benjamin, Jonathan, Erben, Thomas, Harnois-Déraps, Joachim, Hoekstra, Henk, Hildebrandt, Hendrik, Kitching, Thomas D., Mellier, Yannick, Miller, Lance, Van Waerbeke, Ludovic, Benabed, Karim, Bonnett, Christopher, Coupon, Jean, Hudson, Michael J., Kuijken, Konrad, Rowe, Barnaby, Schrabback, Tim, Semboloni, Elisabetta, Vafaei, Sanaz, Velander, Malin·2013·Monthly Notices of the Royal Astronomical Society

Abstract

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 deg2 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 σ8 scaled with the total matter density Ωm. For a flat Λcold dark matter (ΛCDM) model we obtain σ8(Ωm/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 Ωm = 0.283 ± 0.010 and σ8 = 0.813 ± 0.014. In the case of a curved wCDM universe, we obtain Ωm = 0.27 ± 0.03, σ8 = 0.83 ± 0.04, w0 = −1.10 ± 0.15 and ΩK = 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.

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Metadata

Authors
Kilbinger, M., Fu, L., Heymans, C., Simpson, F., Benjamin, J., Erben, T., Harnois-Déraps, J., Hoekstra, H., Hildebrandt, H., Kitching, T. D., Mellier, Y., Miller, L., Van Waerbeke, L., Benabed, K., Bonnett, C., Coupon, J., Hudson, M. J., Kuijken, K., Rowe, B., Schrabback, T., Semboloni, E., Vafaei, S., & Velander, M.
Venue
Monthly Notices of the Royal Astronomical Society
Published
2013-02-09
Volume
430
Issue
3
Pages
2200-2220
ISSN
  • 0035-8711 (ISSN-L)
  • 1365-2966
OpenAlex
W2042266745
Cited by
349
References
113
FWCI
33.18
Type
journal article
Language
en
Open access
bronze

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The paper
Kilbinger, M., Fu, L., Heymans, C., Simpson, F., Benjamin, J., Erben, T., Harnois-Déraps, J., Hoekstra, H., Hildebrandt, H., Kitching, T. D., Mellier, Y., Miller, L., Van Waerbeke, L., Benabed, K., Bonnett, C., Coupon, J., Hudson, M. J., Kuijken, K., Rowe, B., . . . Velander, M. (2013). CFHTLenS: combined probe cosmological model comparison using 2D weak gravitational lensing. Monthly Notices of the Royal Astronomical Society. https://doi.org/10.1093/mnras/stt041

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