%0 Generic %1 bera2022bridging %A Bera, Ankita %A Hassan, Sultan %A Smith, Aaron %A Cen, Renyue %A Garaldi, Enrico %A Kannan, Rahul %A Vogelsberger, Mark %D 2022 %K library %T Bridging the Gap between Cosmic Dawn and Reionization favors Faint Galaxies-dominated Models %U http://arxiv.org/abs/2209.14312 %X Current standard astrophysical models struggle to explain the tentative detection of the 21 cm absorption trough centered at $z\sim17$ measured by the EDGES low-band antenna. However, it has been shown that the EDGES results are consistent with an extrapolation of a declining UV luminosity density, following a simple power-law of deep Hubble Space Telescope observations of $4 < z < 9$ galaxies. We here explore the conditions by which the EDGES detection is consistent with current reionization and post-reionization observations, including the volume-averaged neutral hydrogen fraction of the intergalactic medium at $z\sim6-8$, the optical depth to the cosmic microwave background, and the integrated ionizing emissivity at $z\sim5$. By coupling a physically motivated source model derived from radiative transfer hydrodynamic simulations of reionization to a Markov Chain Monte Carlo sampler, we find that high contribution from low-mass halos along with high photon escape fractions are required to simultaneously reproduce the high-redshift (cosmic dawn) and low-redshift (reionization) existing constraints. Low-mass faint-galaxies dominated models produce a flatter emissivity evolution that results in an earlier onset of reionization with gradual and longer duration, and higher optical depth. Our results provide insights on the role of faint and bright galaxies during cosmic reionization, which can be tested by upcoming surveys with the James Webb Space Telescope.

@misc{bera2022bridging, abstract = {Current standard astrophysical models struggle to explain the tentative detection of the 21 cm absorption trough centered at $z\sim17$ measured by the EDGES low-band antenna. However, it has been shown that the EDGES results are consistent with an extrapolation of a declining UV luminosity density, following a simple power-law of deep Hubble Space Telescope observations of $4 < z < 9$ galaxies. We here explore the conditions by which the EDGES detection is consistent with current reionization and post-reionization observations, including the volume-averaged neutral hydrogen fraction of the intergalactic medium at $z\sim6-8$, the optical depth to the cosmic microwave background, and the integrated ionizing emissivity at $z\sim5$. By coupling a physically motivated source model derived from radiative transfer hydrodynamic simulations of reionization to a Markov Chain Monte Carlo sampler, we find that high contribution from low-mass halos along with high photon escape fractions are required to simultaneously reproduce the high-redshift (cosmic dawn) and low-redshift (reionization) existing constraints. Low-mass faint-galaxies dominated models produce a flatter emissivity evolution that results in an earlier onset of reionization with gradual and longer duration, and higher optical depth. Our results provide insights on the role of faint and bright galaxies during cosmic reionization, which can be tested by upcoming surveys with the James Webb Space Telescope.}, added-at = {2022-09-30T10:19:18.000+0200}, author = {Bera, Ankita and Hassan, Sultan and Smith, Aaron and Cen, Renyue and Garaldi, Enrico and Kannan, Rahul and Vogelsberger, Mark}, biburl = {https://www.bibsonomy.org/bibtex/240114e927c39c420dc7fec709d9d493d/gpkulkarni}, description = {Bridging the Gap between Cosmic Dawn and Reionization favors Faint Galaxies-dominated Models}, interhash = {dcf7002dd49321b8c04bc722428a998c}, intrahash = {40114e927c39c420dc7fec709d9d493d}, keywords = {library}, note = {cite arxiv:2209.14312Comment: 12 pages, 5 figures, submitted to ApJ, comments are welcome}, timestamp = {2022-09-30T10:19:18.000+0200}, title = {Bridging the Gap between Cosmic Dawn and Reionization favors Faint Galaxies-dominated Models}, url = {http://arxiv.org/abs/2209.14312}, year = 2022 }