TY - JOUR
T1 - Seeing in the dark-II. cosmic shear in the sloan digital sky survey
AU - Huff, Eric M.
AU - Eifler, Tim
AU - Hirata, Christopher M.
AU - Mandelbaum, Rachel
AU - Schlegel, David
AU - Seljak, Uroš
PY - 2014/5
Y1 - 2014/5
N2 - Statistical weak lensing by large-scale structure-cosmic shear-is a promising cosmological tool, which has motivated the design of several large upcoming surveys. Here, we present a measurement of cosmic shear using co-added Sloan Digital Sky Survey (SDSS) imaging in 168 square degrees of the equatorial region, with r < 23.5 and i < 22.5, a source number density of 2.2 per arcmin2 and mean redshift of zmed = 0.52. These co-adds were generated using a new method described in the companion Paper I that was intended to minimize systematic errors in the lensing measurement due to coherent point spread function anisotropies that are otherwise prevalent in the SDSS imaging data.We present measurements of cosmic shear out to angular separations of 2°, along with systematics tests that (combined with those from Paper I on the catalogue generation) demonstrate that our results are dominated by statistical rather than systematic errors. Assuming a cosmological model corresponding to Wilkinson Microwave Anisotropy Probe 7(WMAP7) and allowing only the amplitude of matter fluctuations σ8 to vary, we find a best-fitting value of σ8 = 0.636+0.109 -0.154 (1σ); without systematic errors this would be σ8 = 0.636+0.099 -0.137 (1σ). Assuming a flatδcold dark matter model, the combined constraints with WMAP7 are σ8 = 0.784+0.028 -0.026(1σ)+0.055 -0.054(2σ) and ωmh2 = 0.1303+0.0047 -0.0048(1σ)+0.009 -0.009(2σ); the 2σ error ranges are, respectively, 14 and 17 per cent smaller than WMAP7 alone.
AB - Statistical weak lensing by large-scale structure-cosmic shear-is a promising cosmological tool, which has motivated the design of several large upcoming surveys. Here, we present a measurement of cosmic shear using co-added Sloan Digital Sky Survey (SDSS) imaging in 168 square degrees of the equatorial region, with r < 23.5 and i < 22.5, a source number density of 2.2 per arcmin2 and mean redshift of zmed = 0.52. These co-adds were generated using a new method described in the companion Paper I that was intended to minimize systematic errors in the lensing measurement due to coherent point spread function anisotropies that are otherwise prevalent in the SDSS imaging data.We present measurements of cosmic shear out to angular separations of 2°, along with systematics tests that (combined with those from Paper I on the catalogue generation) demonstrate that our results are dominated by statistical rather than systematic errors. Assuming a cosmological model corresponding to Wilkinson Microwave Anisotropy Probe 7(WMAP7) and allowing only the amplitude of matter fluctuations σ8 to vary, we find a best-fitting value of σ8 = 0.636+0.109 -0.154 (1σ); without systematic errors this would be σ8 = 0.636+0.099 -0.137 (1σ). Assuming a flatδcold dark matter model, the combined constraints with WMAP7 are σ8 = 0.784+0.028 -0.026(1σ)+0.055 -0.054(2σ) and ωmh2 = 0.1303+0.0047 -0.0048(1σ)+0.009 -0.009(2σ); the 2σ error ranges are, respectively, 14 and 17 per cent smaller than WMAP7 alone.
KW - Gravitational lensing
KW - Observations
KW - Weak-surveys-cosmology
UR - http://www.scopus.com/inward/record.url?scp=84899003867&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84899003867&partnerID=8YFLogxK
U2 - 10.1093/mnras/stu145
DO - 10.1093/mnras/stu145
M3 - Article
AN - SCOPUS:84899003867
VL - 440
SP - 1322
EP - 1344
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
SN - 0035-8711
IS - 2
ER -