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dc.contributor.authorReid, B. A.
dc.contributor.authorSamushia, L.
dc.contributor.authorWhite, M.
dc.contributor.authorPercival, W. J.
dc.contributor.authorManera, M.
dc.contributor.authorPadmanabhan, N.
dc.contributor.authorRoss, A. J.
dc.contributor.authorSánchez, A. G.
dc.contributor.authorBailey, S.
dc.contributor.authorBizyaev, D.
dc.contributor.authorBolton, A. S.
dc.contributor.authorBrewington, H.
dc.contributor.authorBrinkmann, J.
dc.contributor.authorBrownstein, J. R.
dc.contributor.authorCuesta, A. J.
dc.contributor.authorEisenstein, D. J.
dc.contributor.authorGunn, J. E.
dc.contributor.authorHonscheid, K.
dc.contributor.authorMalanushenko, E.
dc.contributor.authorMalanushenko, V.
dc.contributor.authorMaraston, C.
dc.contributor.authorMcBride, C. K.
dc.contributor.authorMuna, D.
dc.contributor.authorNichol, R. C.
dc.contributor.authorOravetz, D.
dc.contributor.authorPan, K.
dc.contributor.authorde Putter, R.
dc.contributor.authorRoe, N. A.
dc.contributor.authorRoss, N. P.
dc.contributor.authorSchlegel, D. J.
dc.contributor.authorSchneider, D. P.
dc.contributor.authorSeo, H.-J.
dc.contributor.authorShelden, A.
dc.contributor.authorSheldon, E. S.
dc.contributor.authorSimmons, A.
dc.contributor.authorSkibba, R. A.
dc.contributor.authorSnedden, S.
dc.contributor.authorSwanson, M. E. C.
dc.contributor.authorThomas, D.
dc.contributor.authorTinker, J.
dc.contributor.authorTojeiro, R.
dc.contributor.authorVerde, L.
dc.contributor.authorWake, D. A.
dc.contributor.authorWeaver, B. A.
dc.contributor.authorWeinberg, D. H.
dc.contributor.authorZehavi, I.
dc.contributor.authorZhao, G.-B.
dc.date.accessioned2018-10-16T14:30:18Z
dc.date.available2018-10-16T14:30:18Z
dc.date.issued2012-11-11
dc.identifier.citationReid , B A , Samushia , L , White , M , Percival , W J , Manera , M , Padmanabhan , N , Ross , A J , Sánchez , A G , Bailey , S , Bizyaev , D , Bolton , A S , Brewington , H , Brinkmann , J , Brownstein , J R , Cuesta , A J , Eisenstein , D J , Gunn , J E , Honscheid , K , Malanushenko , E , Malanushenko , V , Maraston , C , McBride , C K , Muna , D , Nichol , R C , Oravetz , D , Pan , K , de Putter , R , Roe , N A , Ross , N P , Schlegel , D J , Schneider , D P , Seo , H-J , Shelden , A , Sheldon , E S , Simmons , A , Skibba , R A , Snedden , S , Swanson , M E C , Thomas , D , Tinker , J , Tojeiro , R , Verde , L , Wake , D A , Weaver , B A , Weinberg , D H , Zehavi , I & Zhao , G-B 2012 , ' The clustering of galaxies in the SDSS-III Baryon Oscillation Spectroscopic Survey : measurements of the growth of structure and expansion rate at z = 0.57 from anisotropic clustering ' , Monthly Notices of the Royal Astronomical Society , vol. 426 , pp. 2719-2737 . https://doi.org/10.1111/j.1365-2966.2012.21779.xen
dc.identifier.issn0035-8711
dc.identifier.otherPURE: 252559298
dc.identifier.otherPURE UUID: 5743ac5b-892f-47af-b167-998e911dc404
dc.identifier.otherBibtex: urn:16dbdeec90c735ad19a06a00a84bf3c4
dc.identifier.otherScopus: 84867858872
dc.identifier.urihttps://hdl.handle.net/10023/16241
dc.description.abstractWe analyse the anisotropic clustering of massive galaxies from the Sloan Digital Sky Survey III Baryon Oscillation Spectroscopic Survey (BOSS) Data Release 9 (DR9) sample, which consists of 264 283 galaxies in the redshift range 0.43 < z < 0.7 spanning 3275 deg2. Both peculiar velocities and errors in the assumed redshift–distance relation (‘Alcock–Paczynski effect’) generate correlations between clustering amplitude and orientation with respect to the line of sight. Together with the sharp baryon acoustic oscillation (BAO) standard ruler, our measurements of the broad-band shape of the monopole and quadrupole correlation functions simultaneously constrain the comoving angular diameter distance (2190 ± 61 Mpc) to z = 0.57, the Hubble expansion rate at z = 0.57 (92.4 ± 4.5 km s−1 Mpc−1) and the growth rate of structure at that same redshift (dσ8/d ln a = 0.43 ± 0.069). Our analysis provides the best current direct determination of both DA and H in galaxy clustering data using this technique. If we further assume a Λcold dark matter expansion history, our growth constraint tightens to dσ8/d ln a = 0.415 ± 0.034. In combination with the cosmic microwave background, our measurements of DA, H and dσ8/d ln a all separately require dark energy at z > 0.57, and when combined imply ΩΛ = 0.74 ± 0.016, independent of the Universe's evolution at z < 0.57. All of these constraints assume scale-independent linear growth, and assume general relativity to compute both 퓞 (10 per cent) non-linear model corrections and our errors. In our companion paper, Samushia et al., we explore further cosmological implications of these observations.
dc.format.extent19
dc.language.isoeng
dc.relation.ispartofMonthly Notices of the Royal Astronomical Societyen
dc.rights© 2012 The Authors, Monthly Notices of the Royal Astronomical Society © 2012 RAS. This work has been made available online in accordance with the publisher’s policies. This is the final published version of the work, which was originally published at https://doi.org/10.1111/j.1365-2966.2012.21779.xen
dc.subjectGalaxies: haloesen
dc.subjectGalaxies: statisticsen
dc.subjectCosmological parametersen
dc.subjectLarge-scale structure of the Universeen
dc.subjectQB Astronomyen
dc.subjectQC Physicsen
dc.subject.lccQBen
dc.subject.lccQCen
dc.titleThe clustering of galaxies in the SDSS-III Baryon Oscillation Spectroscopic Survey : measurements of the growth of structure and expansion rate at z = 0.57 from anisotropic clusteringen
dc.typeJournal articleen
dc.description.versionPublisher PDFen
dc.contributor.institutionUniversity of St Andrews. School of Physics and Astronomyen
dc.identifier.doihttps://doi.org/10.1111/j.1365-2966.2012.21779.x
dc.description.statusPeer revieweden


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