2019
DOI: 10.1093/mnras/stz1878
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Constraining the evolution of [C ii] intensity through the end stages of reionization

Abstract: We combine available constraints on the local [CII] 158 µm line luminosity function from galaxy observations (Hemmati et al. 2017), with the evolution of the star-formation rate density and the recent [CII] intensity mapping measurement in Pullen et al. (2018, assuming detection), to derive the evolution of the [CII] luminosity -halo mass relation over z ∼ 0 − 6. We develop convenient fitting forms for the evolution of the [CII] luminosity -halo mass relation, and forecast constraints on the [CII] intensity m… Show more

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Cited by 58 publications
(33 citation statements)
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“…COBE/FIRAS has insufficient sensitivity to extract this emission, and searches in the Planck data have hit fundamental limits [309,310] at a 3σ excess consistent with [CII] emission. New instruments are needed to constrain this signal [311].…”
Section: Line Intensity Mappingmentioning
confidence: 99%
“…COBE/FIRAS has insufficient sensitivity to extract this emission, and searches in the Planck data have hit fundamental limits [309,310] at a 3σ excess consistent with [CII] emission. New instruments are needed to constrain this signal [311].…”
Section: Line Intensity Mappingmentioning
confidence: 99%
“…Figure 3 shows the power spectrum calculated by the methods described here. We model dn/dM through COLOSSUS software (Diemer, 2018), and use the [CII] mass-luminosity function from Padmanabhan (2019), resulting in Ī(z = 3) = 15.7 kJy sr −1 and b(z = 3) = 3.48. The orange (upper) shaded curve shows the total power spectrum, including both clustering and shot power spectra, the dark blue (lower) shaded curve describes the clustering power spectrum, and the flat dotted curve the shot power.…”
Section: Power Spectrum Statisticsmentioning
confidence: 99%
“…The rest frequency of [CII] is ν rest CII = 1900 GHz. We calculate the [CII] intensity by inserting the massluminosity function of Padmanabhan [23] into Equations 2 and 4, resulting in a biased intensity of [Ib](z = 1.5) = 144 Jy sr −1 . We model the Roman HOD through hod0 in [24], with a multiplicative constant scaled to obtain an average galaxy number density of n(z = 1.5) = 0.0016 h 3 Mpc −3 , and we calculate a bias b g (z = 1.5) = 2.3.…”
Section: B Realistic Survey Modelmentioning
confidence: 99%