4.7 Article

The escape of ionizing photons from supernova-dominated primordial galaxies

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 398, Issue 2, Pages 715-721

Publisher

WILEY-BLACKWELL PUBLISHING, INC
DOI: 10.1111/j.1365-2966.2009.15195.x

Keywords

radiative transfer; dust; extinction; galaxies: evolution; galaxies: formation; galaxies: high-redshift

Funding

  1. MEXT [16002003]
  2. JSPS [20224002, 21244013, 18540242]
  3. Grants-in-Aid for Scientific Research [18540242, 21244013] Funding Source: KAKEN

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In order to assess the contribution of Lyman break galaxies (LBGs) and Lyman alpha emitters (LAEs) at redshifts 3 < z < 7 to the ionization of intergalactic medium (IGM), we investigate the escape fractions of ionizing photons from supernova-dominated primordial galaxies by solving the three-dimensional (3D) radiative transfer. The model galaxy is employed from an ultra-high-resolution chemodynamic simulation of a primordial galaxy by Mori & Umemura, which well reproduces the observed properties of LAEs and LBGs. The total mass of model galaxy is 10(11) M(circle dot). We solve not only photoionization but also collisional ionization by shocks. In addition, according to the chemical enrichment, we incorporate the effect of dust extinction, taking the size distributions of dust into account. As a result, we find that dust extinction reduces the escape fractions by a factor of 1.5-8.5 in the LAE phase and by a factor of 2.5-11 in the LBG phase, while the collisional ionization by shocks increases the escape fractions by a factor of approximate to 2. The resultant escape fractions are 0.07-0.47 in the LAE phase and 0.06-0.17 in the LBG phase. These results are well concordant with the recent estimations derived from the flux density ratio at 1500 to 900 A of LAEs and LBGs. Combining the resultant escape fractions with the luminosity functions of LAEs and LBGs, we find that high-z LAEs and LBGs can ionize the IGM at z = 3-5. However, ionizing radiation from LAEs as well as LBGs falls short of ionizing the IGM at z > 6. That implies that additional ionization sources may be required at z > 6.

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