Back to Search Start Over

HI constraints from the cross-correlation of eBOSS galaxies and Green Bank Telescope intensity maps

Authors :
Wolz, Laura
Pourtsidou, Alkistis
Masui, Kiyoshi W.
Chang, Tzu-Ching
Bautista, Julian E.
Mueller, Eva-Maria
Avila, Santiago
Bacon, David
Percival, Will J.
Cunnington, Steven
Anderson, Chris
Chen, Xuelei
Kneib, Jean-Paul
Li, Yi-Chao
Liao, Yu-Wei
Pen, Ue-Li
Peterson, Jeffrey B.
Rossi, Graziano
Schneider, Donald P.
Yadav, Jaswant
Zhao, Gong-Bo
Wolz, Laura
Pourtsidou, Alkistis
Masui, Kiyoshi W.
Chang, Tzu-Ching
Bautista, Julian E.
Mueller, Eva-Maria
Avila, Santiago
Bacon, David
Percival, Will J.
Cunnington, Steven
Anderson, Chris
Chen, Xuelei
Kneib, Jean-Paul
Li, Yi-Chao
Liao, Yu-Wei
Pen, Ue-Li
Peterson, Jeffrey B.
Rossi, Graziano
Schneider, Donald P.
Yadav, Jaswant
Zhao, Gong-Bo
Publication Year :
2021

Abstract

We present the joint analysis of Neutral Hydrogen (HI) Intensity Mapping observations with three galaxy samples: the Luminous Red Galaxy (LRG) and Emission Line Galaxy (ELG) samples from the eBOSS survey, and the WiggleZ Dark Energy Survey sample. The HI intensity maps are Green Bank Telescope observations of the redshifted 21cm emission on 100deg2 covering the redshift range $0.6<z<1.0$. We process the data by separating and removing the foregrounds with FastICA, and construct a transfer function to correct for the effects of foreground removal on the HI signal. We cross-correlate the cleaned HI data with the galaxy samples and study the overall amplitude as well as the scale-dependence of the power spectrum. We also qualitatively compare our findings with the predictions by a semi-analytic galaxy evolution simulation. The cross-correlations constrain the quantity $\Omega_{{HI}} b_{{HI}} r_{{HI},{opt}}$ at an effective scale $k_{eff}$, where $\Omega_{HI}$ is the HI density fraction, $b_{HI}$ is the HI bias, and $r_{{HI},{opt}}$ the galaxy-hydrogen correlation coefficient, which is dependent on the HI content of the optical galaxy sample. At $k_{eff}=0.31 \, h/{Mpc}$ we find $\Omega_{{HI}} b_{{HI}} r_{{HI},{Wig}} = [0.58 \pm 0.09 \, {(stat) \pm 0.05 \, {(sys)}}] \times 10^{-3}$ for GBT-WiggleZ, $\Omega_{{HI}} b_{{HI}} r_{{HI,{ELG}}} = [0.40 \pm 0.09 \, {(stat) \pm 0.04 \, {(sys)}}] \times 10^{-3}$ for GBT-ELG, and $\Omega_{{HI}} b_{{HI}} r_{{HI},{LRG}} = [0.35 \pm 0.08 \, {(stat) \pm 0.03 \, {(sys)}}] \times 10^{-3}$ for GBT-LRG, at $z\simeq 0.8$. We also report results at $k_{eff}=0.24 \, h/{Mpc}$ and $k_{eff}=0.48 \, h/{Mpc}$. With little information on HI parameters beyond our local Universe, these are amongst the most precise constraints on neutral hydrogen density fluctuations in an underexplored redshift range.<br />Comment: 18 pages, 19 figures, 1 table; accepted by MNRAS

Details

Database :
OAIster
Publication Type :
Electronic Resource
Accession number :
edsoai.on1363541590
Document Type :
Electronic Resource
Full Text :
https://doi.org/10.1093.mnras.stab3621