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The WiggleZ Dark Energy Survey: joint measurements of the expansion and growth history at<i>z</i>&lt; 1

Chris BlakeCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaSarah BroughAustralian Astronomical Observatory; PO Box 296; Epping; NSW; 1710; AustraliaMatthew CollessAustralian Astronomical Observatory; PO Box 296; Epping; NSW; 1710; AustraliaCarlos ContrerasCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaWarrick CouchCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaScott CroomSydney Institute for Astronomy; School of Physics, University of Sydney; NSW; 2006; AustraliaDarren CrotonCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaTamara M. DavisSchool of Mathematics and Physics; University of Queensland; Brisbane; QLD; 4072; AustraliaMichael J. DrinkwaterSchool of Mathematics and Physics; University of Queensland; Brisbane; QLD; 4072; AustraliaKarl ForsterCalifornia Institute of Technology; MC 278-17, 1200 East California Boulevard; Pasadena; CA; 91125; USADavid GilbankSouth African Astronomical Observatory; PO Box 9; Observatory; 7935; South AfricaMike GladdersDepartment of Astronomy and Astrophysics; University of Chicago; 5640 South Ellis Avenue; Chicago; IL; 60637; USAKarl GlazebrookCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaBen JelliffeSydney Institute for Astronomy; School of Physics, University of Sydney; NSW; 2006; AustraliaRussell J. JurekAustralia Telescope National Facility; CSIRO; Epping; NSW; 1710; AustraliaI-hui LiCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaBarry MadoreObservatories of the Carnegie Institute of Washington; 813 Santa Barbara St.; Pasadena; CA; 91101; USAD. Christopher MartinCalifornia Institute of Technology; MC 278-17, 1200 East California Boulevard; Pasadena; CA; 91125; USAKevin PimbbletSchool of Physics; Monash University; Clayton; VIC; 3800; AustraliaGregory B. PooleCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaMichael PracySydney Institute for Astronomy; School of Physics, University of Sydney; NSW; 2006; AustraliaRob SharpEmily WisnioskiCentre for Astrophysics and Supercomputing; Swinburne University of Technology; PO Box 218; Hawthorn; VIC; 3122; AustraliaDavid WoodsDepartment of Physics and Astronomy; University of British Columbia; 6224 Agricultural Road; Vancouver; BC; V6T 1Z1; CanadaTed K. WyderCalifornia Institute of Technology; MC 278-17, 1200 East California Boulevard; Pasadena; CA; 91125; USAH. K. C. YeeDepartment of Astronomy and Astrophysics; University of Toronto; 50 St. George Street; Toronto; ON; M5S 3H4; Canada
2012en
ABI

Abstract

We perform a joint determination of the distance-redshift relation and cosmic expansion rate at redshifts z = 0.44, 0.6 and 0.73 by combining measurements of the baryon acoustic peak and Alcock-Paczynski distortion from galaxy clustering in the WiggleZ Dark Energy Survey, using a large ensemble of mock catalogues to calculate the covariance between the measurements. We find that D A(z) = (1205 ± 114, 1380 ± 95, 1534 ± 107)Mpc and H(z) = (82.6 ± 7.8, 87.9 ± 6.1, 97.3 ± 7.0)kms -1Mpc -1 at these three redshifts. Further combining our results with other baryon acoustic oscillation and distant supernovae data sets, we use a Monte Carlo Markov Chain technique to determine the evolution of the Hubble parameter H(z) as a stepwise function in nine redshift bins of width Δz = 0.1, also marginalizing over the spatial curvature. Our measurements of H(z), which have precision better than 7 per cent in most redshift bins, are consistent with the expansion history predicted by a cosmological constant dark energy model, in which the expansion rate accelerates at redshift z &lt; 0.7.

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