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Intensity Mapping of H , Hβ, , and Lines at z < 5

Intensity mapping is becoming a useful tool to study the large-scale structure of the universe through spatial variations in the integrated emission from galaxies and the intergalactic medium. We study intensity mapping of the , [O iii] 5007 , [O ii] 3727 , and lines at . The mean intensities of the...

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Bibliographic Details
Published in:The Astrophysical journal 2017-02, Vol.835 (2)
Main Authors: Gong, Yan, Cooray, Asantha, Silva, Marta B., Zemcov, Michael, Feng, Chang, Santos, Mario G., Dore, Olivier, Chen, Xuelei
Format: Article
Language:English
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Summary:Intensity mapping is becoming a useful tool to study the large-scale structure of the universe through spatial variations in the integrated emission from galaxies and the intergalactic medium. We study intensity mapping of the , [O iii] 5007 , [O ii] 3727 , and lines at . The mean intensities of these four emission lines are estimated using the observed luminosity functions (LFs), cosmological simulations, and the star formation rate density (SFRD) derived from observations at . We calculate the intensity power spectra and consider the foreground contamination of other lines at lower redshifts. We use the proposed NASA small explorer SPHEREx (the Spectro-Photometer for the History of the universe, Epoch of Reionization, and Ices Explorer) as a case study for the detectability of the intensity power spectra of the four emission lines. We also investigate the cross-correlation with the 21 cm line probed by the Canadian Hydrogen Intensity Mapping Experiment (CHIME), Tianlai experiment and the Square Kilometer Array (SKA) at . We find both the auto and cross power spectra can be well measured for the H , [O iii] and [O ii] lines at , while it is more challenging for the Hβ line. Finally, we estimate the constraint on the SFRD from intensity mapping, and find we can reach an accuracy higher than 7% at , which is better than with the usual method of measurements using the LFs of galaxies.
ISSN:0004-637X
1538-4357
DOI:10.3847/1538-4357/835/2/273