arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2007.09008astro-ph.CO
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The Completed SDSS-IV extended Baryon Oscillation Spectroscopic Survey: measurement of the BAO and growth rate of structure of the emission line galaxy sample from the anisotropic power spectrum between redshift 0.6 and 1.1

Arnaud de Mattia, Vanina Ruhlmann-Kleider, Anand Raichoor, Ashley J. Ross, Amélie Tamone, Cheng Zhao, Shadab Alam, Santiago Avila, Etienne Burtin, Julian Bautis… 展开作者

Arnaud de Mattia, Vanina Ruhlmann-Kleider, Anand Raichoor, Ashley J. Ross, Amélie Tamone, Cheng Zhao, Shadab Alam, Santiago Avila, Etienne Burtin, Julian Bautista, Florian Beutler, Jonathan Brinkmann, Joel R. Brownstein, Michael J. Chapman, Chia-Hsun Chuang, Johan Comparat, Hélion du Mas des Bourboux, Kyle S. Dawson, Axel de la Macorra, Héctor Gil-Marín, Violeta Gonzalez-Perez, Claudio Gorgoni, Jiamin Hou, Hui Kong, Sicheng Lin, Seshadri Nadathur, Jeffrey A. Newman, Eva-Maria Mueller, Will J. Percival, Mehdi Rezaie, Graziano Rossi, Donald P. Schneider, Prabhakar Tiwari, M. Vivek, Yuting Wang, Gong-Bo Zhao

英文摘要:

We analyse the large-scale clustering in Fourier space of emission line galaxies (ELG) from the Data Release 16 of the Sloan Digital Sky Survey IV extended Baryon Oscillation Spectroscopic Survey. The ELG sample contains 173,736 galaxies covering 1,170 square degrees in the redshift range $0.6 < z < 1.1$. We perform a BAO measurement from the post-reconstruction power spectrum monopole, and study redshift space distortions (RSD) in the first three even multipoles. Photometric variations yield fluctuations of both the angular and radial survey selection functions. Those are directly inferred from data, imposing integral constraints which we model consistently. The full data set has only a weak preference for a BAO feature ($1.4σ$). At the effective redshift $z_{\rm eff} = 0.845$ we measure $D_{\rm V}(z_{\rm eff})/r_{\rm drag} = 18.33_{-0.62}^{+0.57}$, with $D_{\rm V}$ the volume-averaged distance and $r_{\rm drag}$ the comoving sound horizon at the drag epoch. In combination with the RSD measurement, at $z_{\rm eff} = 0.85$ we find $fσ_8(z_{\rm eff}) = 0.289_{-0.096}^{+0.085}$, with $f$ the growth rate of structure and $σ_8$ the normalisation of the linear power spectrum, $D_{\rm H}(z_{\rm eff})/r_{\rm drag} = 20.0_{-2.2}^{+2.4}$ and $D_{\rm M}(z_{\rm eff})/r_{\rm drag} = 19.17 \pm 0.99$ with $D_{\rm H}$ and $D_{\rm M}$ the Hubble and comoving angular distances, respectively. These results are in agreement with those obtained in configuration space, thus allowing a consensus measurement of $fσ_8(z_{\rm eff}) = 0.315 \pm 0.095$, $D_{\rm H}(z_{\rm eff})/r_{\rm drag} = 19.6_{-2.1}^{+2.2}$ and $D_{\rm M}(z_{\rm eff})/r_{\rm drag} = 19.5 \pm 1.0$. This measurement is consistent with a flat $Λ$CDM model with Planck parameters.

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