Cosmological implications of baryon acoustic oscillation measurements

É. Aubourg(Centre National de la Recherche Scientifique), S. Bailey(Lawrence Berkeley National Laboratory), Julian Bautista(Centre National de la Recherche Scientifique), Florian Beutler(Lawrence Berkeley National Laboratory), Vaishali Bhardwaj(Lawrence Berkeley National Laboratory), Dmitry Bizyaev, Michael R. Blanton(New York University), Michael Blomqvist(University of California, Irvine), A. Bolton(University of Utah), Jo Bovy(Institute for Advanced Study), H. Brewington, J. Brinkmann, Joel R. Brownstein(University of Utah), A. Burden(University of Portsmouth), Nicolás G. Busca(Centre National de la Recherche Scientifique), W. Carithers(Lawrence Berkeley National Laboratory), Chia-Hsun Chuang(Universidad Autónoma de Madrid), Johan Comparat(Universidad Autónoma de Madrid), Rupert A. C. Croft(University of Oxford), Antonio J. Cuesta(Whitney Museum of American Art), Kyle Dawson(University of Utah), Timothée Delubac(École Polytechnique Fédérale de Lausanne), Daniel J. Eisenstein(Center for Astrophysics Harvard & Smithsonian), Andreu Font-Ribera(Lawrence Berkeley National Laboratory), Jian Ge(University of Florida), J.M. Le Goff(Commissariat à l'Énergie Atomique et aux Énergies Alternatives), Satya Gontcho A Gontcho(Universitat de Barcelona), J. Richard Gott(Princeton University), James E. Gunn(Princeton University), Hong Guo(University of Utah), Julien Guy(Centre National de la Recherche Scientifique), J.–Ch. Hamilton(Centre National de la Recherche Scientifique), Shirley Ho(Carnegie Mellon University), Klaus Honscheid(The Ohio State University), Cullan Howlett(University of Portsmouth), D. Kirkby(University of California, Irvine), Francisco-Shu Kitaura(Leibniz Institute for Astrophysics Potsdam), Jean‐Paul Kneib(Centre National de la Recherche Scientifique), Khee‐Gan Lee(Max Planck Institute for Astronomy), Dan Long, Robert H. Lupton(Princeton University), M. Vargas-Magaña(Centre National de la Recherche Scientifique), Viktor Malanushenko, Elena Malanushenko, Marc Manera(University College London), Claudia Maraston(University of Portsmouth), Daniel Margala(University of California, Irvine), Cameron K. McBride(Center for Astrophysics Harvard & Smithsonian), Jordi Miralda‐Escudé(Institució Catalana de Recerca i Estudis Avançats), Adam D. Myers(University of Wyoming), Robert C. Nichol(University of Portsmouth), P. Noterdaeme(Centre National de la Recherche Scientifique), Sebastián E. Nuza(Leibniz Institute for Astrophysics Potsdam), Matthew D. Olmstead(University of Utah), Daniel Oravetz, Isabelle Pâris(Trieste Astronomical Observatory), Nikhil Padmanabhan(Whitney Museum of American Art), N. Palanque‐Delabrouille(Lawrence Berkeley National Laboratory), Kaike Pan, Marcos Pellejero-Ibáñez(Universidad de La Laguna), Will J. Percival(University of Portsmouth), Patrick Petitjean(Centre National de la Recherche Scientifique), Matthew M. Pieri(Centre National de la Recherche Scientifique), Francisco Prada(Consejo Superior de Investigaciones Científicas), Beth Reid(Lawrence Berkeley National Laboratory), James Rich(Commissariat à l'Énergie Atomique et aux Énergies Alternatives), Natalie A. Roe(Lawrence Berkeley National Laboratory), Ashley J. Ross(The Ohio State University), Nicholas P. Ross(Drexel University), Graziano Rossi(Commissariat à l'Énergie Atomique et aux Énergies Alternatives), J. A. Rubiño-Martín(Universidad de La Laguna), Ariel G. Sánchez(Max Planck Institute for Extraterrestrial Physics), Lado Samushia(Ilia State University), R. Génova-Santos(Instituto de Astrofísica de Canarias), Claudia G. Scóccola(Instituto de Astrofísica de Canarias), David J. Schlegel(Lawrence Berkeley National Laboratory), Donald P. Schneider(Pennsylvania State University), Hee‐Jong Seo(Ohio University), Erin Sheldon(Brookhaven National Laboratory), Audrey Simmons, Ramin Skibba(University of California San Diego), Anže Slosar(Brookhaven National Laboratory), Michael A. Strauss(Princeton University), D. Thomas(University of Portsmouth), Jeremy L. Tinker(New York University), Rita Tojeiro(University of Portsmouth), J. Alberto Vázquez(Brookhaven National Laboratory), Matteo Viel(Istituto Nazionale di Fisica Nucleare), David A. Wake(University of Wisconsin–Madison), Benjamin A. Weaver(New York University), David H. Weinberg(The Ohio State University), W. M. Wood‐Vasey(University of Pittsburgh), Christophe Yèche(Commissariat à l'Énergie Atomique et aux Énergies Alternatives), Idit Zehavi(Case Western Reserve University), Gong‐Bo Zhao(National Astronomical Observatories)
Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology
December 14, 2015
Cited by 739Open Access
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Abstract

We derive constraints on cosmological parameters and tests of dark energy models from the combination of baryon acoustic oscillation (BAO) measurements with cosmic microwave background (CMB) data and a recent reanalysis of Type Ia supernova (SN) data. In particular, we take advantage of high-precision BAO measurements from galaxy clustering and the Lyman-$\ensuremath{\alpha}$ forest (LyaF) in the SDSS-III Baryon Oscillation Spectroscopic Survey (BOSS). Treating the BAO scale as an uncalibrated standard ruler, BAO data alone yield a high confidence detection of dark energy; in combination with the CMB angular acoustic scale they further imply a nearly flat universe. Adding the CMB-calibrated physical scale of the sound horizon, the combination of BAO and SN data into an ``inverse distance ladder'' yields a measurement of ${H}_{0}=67.3\ifmmode\pm\else\textpm\fi{}1.1\text{ }\text{ }\mathrm{km}\text{ }{\mathrm{s}}^{\ensuremath{-}1}\text{ }{\mathrm{Mpc}}^{\ensuremath{-}1}$, with 1.7% precision. This measurement assumes standard prerecombination physics but is insensitive to assumptions about dark energy or space curvature, so agreement with CMB-based estimates that assume a flat $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ cosmology is an important corroboration of this minimal cosmological model. For constant dark energy ($\mathrm{\ensuremath{\Lambda}}$), our $\mathrm{BAO}+\mathrm{SN}+\mathrm{CMB}$ combination yields matter density ${\mathrm{\ensuremath{\Omega}}}_{m}=0.301\ifmmode\pm\else\textpm\fi{}0.008$ and curvature ${\mathrm{\ensuremath{\Omega}}}_{k}=\ensuremath{-}0.003\ifmmode\pm\else\textpm\fi{}0.003$. When we allow more general forms of evolving dark energy, the $\mathrm{BAO}+\mathrm{SN}+\mathrm{CMB}$ parameter constraints are always consistent with flat $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ values at $\ensuremath{\approx}1\ensuremath{\sigma}$. While the overall ${\ensuremath{\chi}}^{2}$ of model fits is satisfactory, the LyaF BAO measurements are in moderate ($2--2.5\ensuremath{\sigma}$) tension with model predictions. Models with early dark energy that tracks the dominant energy component at high redshift remain consistent with our expansion history constraints, and they yield a higher ${H}_{0}$ and lower matter clustering amplitude, improving agreement with some low redshift observations. Expansion history alone yields an upper limit on the summed mass of neutrino species, $\ensuremath{\sum}{m}_{\ensuremath{\nu}}<0.56\text{ }\text{ }\mathrm{eV}$ (95% confidence), improving to $\ensuremath{\sum}{m}_{\ensuremath{\nu}}<0.25\text{ }\text{ }\mathrm{eV}$ if we include the lensing signal in the Planck CMB power spectrum. In a flat $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ model that allows extra relativistic species, our data combination yields ${N}_{\mathrm{eff}}=3.43\ifmmode\pm\else\textpm\fi{}0.26$; while the LyaF BAO data prefer higher ${N}_{\mathrm{eff}}$ when excluding galaxy BAO, the galaxy BAO alone favor ${N}_{\mathrm{eff}}\ensuremath{\approx}3$. When structure growth is extrapolated forward from the CMB to low redshift, standard dark energy models constrained by our data predict a level of matter clustering that is high compared to most, but not all, observational estimates.


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