TY - JOUR
T1 - Galactic ionizing photon budget during the epoch of reionization in the Cosmic Dawn II simulation
AU - Lewis, Joseph S.W.
AU - Ocvirk, Pierre
AU - Aubert, Dominique
AU - Sorce, Jenny G.
AU - Shapiro, Paul R.
AU - Deparis, Nicolas
AU - Dawoodbhoy, Taha
AU - Teyssier, Romain
AU - Yepes, Gustavo
AU - Gottlöber, Stefan
AU - Ahn, Kyungjin
AU - Iliev, Ilian T.
AU - Chardin, Jonathan
N1 - Funding Information:
The authors would like to acknowledge the judicious comments of the anonymous referee, as well as those of Max Gronke. This work has used PYTHON, and the following packages : PYTHON : MATPLOTLIB (Hunter 2007), NUMPY (Van Der Walt, Colbert & Varoquaux 2011), SCIPY (Virtanen et al. 2020), HEALPIX (Górski et al. 2005). PO acknowledges support from the French ANR funded project ORAGE (ANR-14-CE33-0016). ND and DA acknowledge funding from the French ANR for project ANR-12-JS05-0001 (EMMA). ITI was supported by the Science and Technology Facilities Council (grant numbers ST/F002858/1 and ST/I000976/1) and the Southeast Physics Network (SEPnet). JS acknowledges support from "l’Oréal-UNESCO ‘Pour les femmes et la Science’" and the ‘Centre National d’études spatiales (CNES)’ postdoctoral fellowship programs. KA was supported by NRF (grant number NRF-2016R1D1A1B04935414). GY acknowledges financial support by the MINECO/FEDER under project grant AYA2015-63810-P and MICIU/FEDER under project grant number PGC2018-094975-C21. PRS was supported in part by U.S. NSF grant number AST-1009799, NASA grant number NNX11AE09G, NASA/JPL grant number
Funding Information:
RSA Nos. 1492788 and 1515294, and supercomputer resources from NSF XSEDE grant number TG-AST090005 and the Texas Advanced Computing Center (TACC) at the University of Texas at Austin. The CoDa II simulation was performed at Oak Ridge National Laboratory/Oak Ridge Leadership Computing Facility on the Titan supercomputer (INCITE2016 award AST031). Processing was performed on the Eos and Rhea clusters. Auxiliary simulations were performed at pôle HPC de l’Université de Strasbourg (méso-centre). The simulations used for the resolution study were performed on CSCS/Piz Daint (Swiss National Supercomputing Centre), as part of the ‘SALT: Shining a light through the dark ages’ PRACE allocation obtained via the 16th call for PRACE Project Access (project id pr37). A series of test simulations for the initial conditions of CoDa II were performed at LRZ Munich within the project pr74no. This work has used v2.1 of the Binary Population and Spectral Synthesis (BPASS) models as last described in Eldridge et al. (2017).
Publisher Copyright:
© 2020 The Author(s).
PY - 2020/8/1
Y1 - 2020/8/1
N2 - Cosmic Dawn II yields the first statistically meaningful determination of the relative contribution to reionization by galaxies of different halo mass, from a fully coupled radiation-hydrodynamics simulation of the epoch of reionization large enough (∼100Mpc) to model global reionization while resolving the formation of all galactic haloes above ∼108 M. Cell transmission inside haloes is bi-modal-ionized cells are transparent, while neutral cells absorb the photons their stars produce-and the halo escape fractionfesc reflects the balance of star formation rate (SFR) between these modes. The latter is increasingly prevalent at higher halo mass, driving downfesc (we provide analytical fits to our results), whereas halo escape luminosity, proportional tof esc × SFR, increases with mass. Haloes with dark matter masses within 6 × 108 M < Mhalo < 3 × 1010 M produce ∼80 per cent of the escaping photons at z = 7, when the universe is 50 per cent ionized, making them the main drivers of cosmic reionization. Less massive haloes, though more numerous, have low SFRs and contribute less than 10 per cent of the photon budget then, despite their highfesc. High-mass haloes are too few and too opaque, contributing < 10 per cent despite their high SFRs. The dominant mass range is lower (higher) at higher (lower) redshift, as mass function and reionization advance together (e.g. at z = 8.5, xHI = 0.9, Mhalo < 5 × 109M haloes contributed ∼80 per cent). Galaxies with UV magnitudes MAB1600 between —12 and —19 dominated reionization between z = 6 and 8.
AB - Cosmic Dawn II yields the first statistically meaningful determination of the relative contribution to reionization by galaxies of different halo mass, from a fully coupled radiation-hydrodynamics simulation of the epoch of reionization large enough (∼100Mpc) to model global reionization while resolving the formation of all galactic haloes above ∼108 M. Cell transmission inside haloes is bi-modal-ionized cells are transparent, while neutral cells absorb the photons their stars produce-and the halo escape fractionfesc reflects the balance of star formation rate (SFR) between these modes. The latter is increasingly prevalent at higher halo mass, driving downfesc (we provide analytical fits to our results), whereas halo escape luminosity, proportional tof esc × SFR, increases with mass. Haloes with dark matter masses within 6 × 108 M < Mhalo < 3 × 1010 M produce ∼80 per cent of the escaping photons at z = 7, when the universe is 50 per cent ionized, making them the main drivers of cosmic reionization. Less massive haloes, though more numerous, have low SFRs and contribute less than 10 per cent of the photon budget then, despite their highfesc. High-mass haloes are too few and too opaque, contributing < 10 per cent despite their high SFRs. The dominant mass range is lower (higher) at higher (lower) redshift, as mass function and reionization advance together (e.g. at z = 8.5, xHI = 0.9, Mhalo < 5 × 109M haloes contributed ∼80 per cent). Galaxies with UV magnitudes MAB1600 between —12 and —19 dominated reionization between z = 6 and 8.
KW - Galaxies: high
KW - Galaxy: formation
KW - Redshift-dark ages, reionization, first stars
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U2 - 10.1093/mnras/staa1748
DO - 10.1093/mnras/staa1748
M3 - Article
AN - SCOPUS:85094165659
SN - 0035-8711
VL - 496
SP - 4342
EP - 4357
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 4
ER -